250 41 59MB
English Pages [83] Year 2023
Contents 1 February 7 - Introduction, simple and semisimple modules, skew fields 1.1 Rings, Modules, Ideals . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1.2 Invariant Basis Number Property . . . . . . . . . . . . . . . . . . . . . . 1.3 Simple modules, Schur Lemma . . . . . . . . . . . . . . . . . . . . . . . . 1.4 Semisimple modules . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
3 4 5 6 6
2 Semisimple modules, socles, Artinian rings, Wedderburnβs Theorem 2.1 More on semisimple modules . . . . . . . . . . . . . . . . . . . . . . . 2.2 Socles . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2.3 Isotypic components . . . . . . . . . . . . . . . . . . . . . . . . . . . 2.4 Classification of semisimple rings . . . . . . . . . . . . . . . . . . . . 2.5 Simple rings and Wedderburnβs Theorem . . . . . . . . . . . . . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
7 7 7 8 8 9
3 February 14: Isotypic decomposition, cobson radical 3.1 π [πΊ]-modules . . . . . . . . . . . . 3.2 Density Theorem . . . . . . . . . . 3.3 Noetherian and Artinian modules . 3.4 Composition Series . . . . . . . . . 3.5 Jacobson Radical . . . . . . . . . . .
. . . . .
. . . . .
Density Theorem, Noetherian and Artinian properties, Ja. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
9 . 9 . 9 . 10 . 10 . 11
4 February 16 - Socle and cosocle filtrations, Jacobson radical, Krull-Schmidt 4.1 Socle and cosocle filtrations . . . . . . . . . . . . . . . . . . . . . . . . . . . 4.2 Jacobson radical cont. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4.3 Local rings and indecomposable modules . . . . . . . . . . . . . . . . . . . . 4.4 Krull-Schmidt . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
12 12 12 13 14
5 February 23 - Jacobson radical, primitive and semi-primitive rings 14 5.1 Interlude on quiver representations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 5.2 Primitive and semi-primitive rings . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15 6 February 28 - Artinian rings are Noetherian, projective covers 17 6.1 The Akizuki-Hopkins-Levitzki Theorem (Artinian rings are Noetherian) . . . . . . . . . . . . . . . . . 17 6.2 Projective covers . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17 6.3 Preview of Morita theory . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19 7 March 2 - Categories and Morita equivalence 19 7.1 Morita equivalence . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19 7.2 Categories and the Yoneda Lemma . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20 7.3 Proof of Morita equivalence theorem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21 8 March 7 - Morita theory continued: (co)centers, functors and bimodules 8.1 Center and cocenter . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8.2 Morita equivalence via functors and bimodules . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8.3 Serre quotients . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
22 22 23 25
9 March 9 - more on Serre quotients, abelian categories 9.1 More on Serre quotients . . . . . . . . . . . . . . . . . . . . 9.2 Adjoint functors and (co)limits . . . . . . . . . . . . . . . . . 9.3 Additive categories . . . . . . . . . . . . . . . . . . . . . . . 9.4 Abelian categories . . . . . . . . . . . . . . . . . . . . . . . . 9.5 Compact projective generators and Serre quotients revisited
25 25 26 27 27 28
1
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
10 March 14 - Exts and Tors, Resolutions 10.1 Ext and Tor . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10.2 Projective, injective, and homological dimension . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10.3 Cartan matrices . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
29 29 30 30
11 March 16 - Koszul complexes 11.1 More on the Hattori-Stallings Dennis trace . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11.2 Minimal resolutions and Koszul rings . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11.3 Koszul complexes . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
32 32 32 33
12 March 21 - Koszul rings cont., bar complex 35 12.1 Finishing up Koszul rings . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 35 12.2 Bar complex and Hochschild (co)homology . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37 13 March 23 - Hochschild (co)homology cont., central simple algebras 38 13.1 Deformations and Hochschild cohomology . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38 13.2 Cobar complex and π΄! . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 39 13.3 Central simple algebras and Brauer group . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 39 14 April 4 - Brauer group and Skolem-Noether Theorems 14.1 Definition and first properties of Brauer group . . . . 14.2 Torsors and Galois forms . . . . . . . . . . . . . . . . 14.3 Centralizer of a commutative subfield . . . . . . . . . 14.4 Skolem-Noether . . . . . . . . . . . . . . . . . . . . . 14.5 Artin-Wedderburn . . . . . . . . . . . . . . . . . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
40 40 41 42 42 43
15 April 6 - Separable splitting fields and cross-product algebras 43 15.1 Separable splitting fields . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43 15.2 Group cohomology . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 44 15.3 Cross-product algebras . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45 16 April 11 - Cohomological description of the Brauer group 16.1 Cross-product algebras and Galois extensions . . . . . . . 16.2 Maximal commutative subfields and splitting fields . . . . 16.3 Proof of the theorem . . . . . . . . . . . . . . . . . . . . . 16.4 Applications . . . . . . . . . . . . . . . . . . . . . . . . . . 16.5 Index and period . . . . . . . . . . . . . . . . . . . . . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
45 45 46 46 46 47
17 April 13 - Brauer groups of central simple algebras, reduced norm and trace 17.1 Reduced norm and trace . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17.2 πΆ 1 fields . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 17.3 Second approach to the cohomological description of Brauer group . . . . . . 17.4 Brauer groups of local fields . . . . . . . . . . . . . . . . . . . . . . . . . . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
48 48 48 49 50
18 April 18 - Azumaya algebras 18.1 Azumaya algebras . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 18.2 Cohomological description of the Brauer group over a ring - preliminary discussion 18.3 Faithfully flat ring homomorphisms and faithfully flat descent . . . . . . . . . . . . 18.4 Universal splitting . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 18.5 Rewriting cochain complex for π» β (πΊ, πΈ Γ ) . . . . . . . . . . . . . . . . . . . . . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
51 51 52 53 53 54
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
. . . . .
19 April 20 - Brauer group of a ring cont., localization 54 19.1 Amitsur cohomology . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 54 19.2 Relationship between Brauer group and Amitsur cohomology . . . . . . . . . . . . . . . . . . . . . . 55 19.3 Final remarks on Brauer group . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 55
2
19.4 Localization . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 56 19.5 Ore conditions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 56 20 April 25 - Ore localization, Goldie theorem 20.1 Ore localization as a filtered colimit . . . 20.2 Ore domains . . . . . . . . . . . . . . . . 20.3 Growth of algebras . . . . . . . . . . . . 20.4 Semi-prime rings and Goldieβs theorem .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
57 57 58 59 59
21 April 27 - Goldie rank and Goldie theorem 60 21.1 More on essential modules . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 60 21.2 Goldie rank . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61 21.3 Regular elements in essential ideals . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 62 22 May 2 - Goldie Theorem, PI rings 22.1 Finishing up Goldie Theorem . . . . . . . . . . . . . . . . 22.2 Goldie rings . . . . . . . . . . . . . . . . . . . . . . . . . 22.3 Applications of Goldieβs Theorem . . . . . . . . . . . . . 22.4 PI rings . . . . . . . . . . . . . . . . . . . . . . . . . . . . 22.5 Amitsur-Levitzki Theorem . . . . . . . . . . . . . . . . . 22.6 Amitsur-Levitzki Theorem and the cohomology of π€π©(π)
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
62 62 63 63 63 64 65
23 May 9 - Another proof of Amitsur-Levitski, PI algebras 23.1 Proof of Amitsur-Levitski Theorem . . . . . . . . . . . 23.2 Primitive algebras and Kaplanskyβs theorem . . . . . . 23.3 Prime PI algebras and Posner theorem . . . . . . . . . . 23.4 Central polynomials . . . . . . . . . . . . . . . . . . . . 23.5 Rowenβs Theorem for semi-primitive algebras . . . . . 23.6 Proof of Rowenβs Theorem (for real) . . . . . . . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
. . . . . .
66 66 66 67 67 68 69
24 May 11 - Gelfand-Kirillov dimension 24.1 Growth of algebras and Gelfand-Kirillov dimension 24.2 Warfieldβs Theorem . . . . . . . . . . . . . . . . . . 24.3 Bergman gap theorem . . . . . . . . . . . . . . . . . 24.4 Ufnarovskii graph . . . . . . . . . . . . . . . . . . . 24.5 Smoktunowicz and Berele theorems . . . . . . . . . 24.6 GK dimension of a module . . . . . . . . . . . . . . 24.7 Poincare series . . . . . . . . . . . . . . . . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
. . . . . . .
70 70 71 72 73 73 73 74
25 May 16 - Final class: noncommutative geometry 25.1 Representation varieties . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25.2 Weyl algebra and deformations . . . . . . . . . . . . . . . . . . . . . . . . . 25.3 Coh(π ) and π· β (Coh(π )) . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25.4 Artin-Schelter regular algebras and noncommutative projective geometry
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
. . . .
75 75 77 78 79
1
. . . . . . .
. . . . . . .
February 7 - Introduction, simple and semisimple modules, skew fields
Noncommutative algebra studies algebraic phenomena that arise in a variety of contexts in mathematics and physics, wherever one encounters a multiplication rule where the commutativity law ππ = ππ fails. An example familiar from linear algebra is multiplication of matrices. Noncommutative groups and Lie algebras also come with such a multiplication; we will also require an addition law compatible with multiplication via the distributive law, groups and Lie algebras can be fit into that framework by passing to the group ring and enveloping algebra respectively. Some approaches to noncommutative algebras are inspired by known results about commutative ones, where we have familiar concepts of radical, localization etc. We will see noncommutative analogues of these concepts later in
3
the course. Another way to relate the noncommutative and the commutative settings is by deforming a commutative multiplication to obtain a noncommutative one; due to its relation to quantum physics this procedure is sometimes called quantization. Just as in the case of groups or commutative algebras, much of the work with the abstract composition rule comprising the structure of a group or a ring involves realizing it as composition of actual symmetries of a specific set or abelian group, this leads to the concept of an action of a group on a set, and an action of a ring on a module. A noncommutative ring will be the main protagonist of our story, the plot develops as the protagonist acts (on a module)! The language of categories and functors is ubiquitous in modern algebra, including study of noncommutative rings and modules over them. Its general concepts and their application to rings and modules will be discussed in the lectures. Powerful tools for study of rings and modules come from homological algebra, we will introduce its basic concepts in the course. We will look into core topics in noncommutative ring theory such as polynomial identities and rate of growth of algebras, and also touch upon connections of noncommutative algebra to other areas such as number theory (Brauer groups), Lie theory (Amitsur-Levitzki Theorem, Goldie rank) etc. The course ends with a brief discussion of noncommutative geometry, an area that grew out of an attempt to connect noncommutative algebra to geometry inspired by the success of algebraic geometry which provides such a connection for commutative algebra.
1.1
Rings, Modules, Ideals
Passing to formal math, the main object of study for us will be associative, possibly noncommutative rings. Definition 1.1: A ring (π
, +) is an abelian group with a multiplication that is associative and distributes over addition. Unless stated otherwise, rings will be unital (have a multiplicative identity). Homomorphisms of rings are required to send 1 to 1. Remark 1.2: Associativity is equivalent to the fact that left multiplication commutes with right multiplication. Definition 1.3: Let π
be a ring. The opposite ring π
op has the same underlying abelian group as π
, but left multiplication by π in π
op is defined as right multiplication by π in π
, i.e. π Β·op π = ππ. It is clear that (π
op ) op = π
. Example 1.4: Fields and skew fields are rings. Recall that a skew field (also known as a division ring) is a ring where every nonzero element is invertible. Example 1.5: Let π
be a ring. Then the set of π Γ π matrices with entries in π
, with matrix addition and multiplication, is also a ring, denoted Matπ (π
). Definition 1.6: A (left) module π over a ring π
is an abelian group equipped with a ring homomorphism π
β End(π). Equivalently, we have a bilinear map π
Γ π β π satisfying π 1 (π 2 (π)) = (π 1π 2 ) (π). A submodule π of π is a subgroup of π closed under the action of π
. Given such π β π, we can also equip π/π with the structure of an π
-module. Example 1.7: If π
is a field, then π
-modules are vector spaces.
4
Definition 1.8: A bimodule over π
is a module with compatible π
-module and π
op -module structures, i.e. the actions of π
and π
op commute. Example 1.9: π
is an π
-bimodule; the π
-module structure is left multiplication and the π
op -module structure is right multiplication, and the associativity of multiplication in π
implies that these are compatible. Definition 1.10: A left ideal of π
is an π
-submodule of π
. A right ideal of π
is an π
op -submodule of π
(treated as an π
op -module). A two-sided ideal of π
is a subbimodule of π
. Remark 1.11: If πΌ is a left ideal, as described in Definition 1.6, π
/πΌ is an π
-module, and likewise, if πΌ is a right ideal, π
/πΌ is an π
op -module. If πΌ is a two-sided ideal, then the multiplication of elements in π
/πΌ is well-defined, and π
/πΌ is a ring. Γ Definition 1.12: An π
-module π is free if it is isomorphic to π βπΌ π
, where πΌ is some (possibly infinite) index set. If π π
π , we say that π has rank π. Note that rank is not well-defined in general! Example 1.13: Every module over a skew field is free. (See linear algebra.) Remark 1.14: Remember that in the finite case, direct products and direct sums are the same, but in the infinite case, they are not. In an infinite direct sum, all but finitely many elements must be 0.
1.2
Invariant Basis Number Property
Definition 1.15: A ring π
has the invariant basis number (IBN) property if free modules of different ranks are not isomorphic. That is, rank is well-defined. Example 1.16: Linear algebra tells us that modules over a skew field satisfy the IBN. Lemma 1.17: If π : π
β π is a ring homomorphism and π satisfies IBN, then so does π
. Proof. To simplify the discussion, letβs focus on finite rank modules. Then Homπ
(π
π , π
π ) = Matπ,π (π
op ) (Endπ
(π
) = π
op because any map π
β π
commutes with left multiplication, hence is defined by its value at 1, and this can be extended to π
π ). If π
doesnβt satisfy IBN, there exist non-square matrices π΄ β Matπ,π (π
op ), π΅ β Matπ,π (π
op ) so that π΄π΅ = 1π , π΅π΄ = 1π . But applying π, we then see that π (π΄), π (π΅) give an isomorphism between π π and π π , contradiction. β‘ Corollary 1.18: Any ring admitting a homomorphism into a skew field satisfies IBN. Example 1.19: By Zornβs lemma, every commutative ring π
has a maximal ideal πͺ. Then π
β π
/πͺ, which is a field, so π
has the IBN. Example 1.20: We will see later that every left Noetherian ring maps to Matπ (π·) for some π, π· a skew field, so it satisfies IBN. Γβ Example 1.21: Let π = Cβ = π=1 C. Then π
:= End(π ) doesnβt satisfy IBN. Choose subspaces π1, π2 such that π = π1 β π2 and π π1, π2 . Then consider the ideals πΌπ := {π | π |ππ = 0}. π
= πΌ 1 β πΌ 2 , but also π
πΌ 1, πΌ 2 . Corollary 1.22: π
= End(Cβ ) does not admit a homomorphism into a skew field.
5
1.3
Simple modules, Schur Lemma
Theorem 1.23: Suppose that every π
-module is free. Then π
is a skew field. To prove this, we will use the Schur Lemma about simple modules. Definition 1.24: A module π is simple or irreducible if π β 0 and it has no nontrivial proper submodules. Example 1.25: π
is simple over itself iff π
is a skew field. (If π
is simple over itself, then π
has no nontrivial ideals, so every nonzero element must be invertible.) Lemma 1.26 (Schur): If π is simple, then Endπ
(π) is a division ring. Proof. Suppose π : π β π is nonzero. Then ker π β π, but π is simple, so ker π = 0. Hence π is injective. Likewise, im π β 0, so im π = π and π is surjective. Thus π is invertible. β‘ Corollary 1.27: Any nonzero map of simple modules is an isomorphism. In particular, if π, π are non-isomorphic simple modules, Hom(π, π ) = 0. Lemma 1.28: a) Every nonzero ring has a simple module. b) Every proper left ideal in a nonzero ring is contained in a maximal ideal. c) A proper submodule π in a module π is maximal iff π/π is simple. Proof. a) will follow from b) and c) because maximal left ideals of π
are maximal π
-submodules of π
. c) is true because the submodules of π/π are in bijection with the submodules of π containing π . b) follows from Zornβs Lemma. Its conditionsΓare satisfied because for a nested collection π0 β π1 β Β· Β· Β· β of proper submodules in a finitely generated π, ππ = π iff some ππ = π. β‘ Remark 1.29: Part b) is also true for finitely generated modules. If π is not finitely generated, b) may not be true. For example, let π
= Z, π = Q. Then π has no maximal proper submodule because you can find a nested collection of submodules of π whose union is also π. Corollary 1.30: Every finitely generated module has an irreducible quotient. Proof (of Theorem 1.23). Let πΏ be a simple π
-module (that exists by Lemma 1.28 π)). It doesnβt contain any submodule isomorphic to π
2 because every nonzero element of πΏ generates πΏ. So if πΏ is free, it must be isomorphic to π
. But then Endπ
(πΏ) Endπ
(π
) = π
op , and Endπ
(πΏ) is a skew field by Lemma 1.26. β‘
1.4
Semisimple modules
Definition 1.31: A module is semisimple if itβs isomorphic to a direct sum of simple modules. Example 1.32: C[π‘]/(π‘ 2 ) is not semisimple as a module over itself. However, we do have an exact sequence of C[π‘]/(π‘ 2 )-modules: 0 β C[π‘]/(π‘) β C[π‘]/(π‘ 2 ) β C[π‘]/(π‘) β 0. Γ Lemma 1.33: Let π = a semisimple module, ππ are simple modules. Then any submodule π β π π βπΌ ππ beΓ has a direct complement of the form π β π½ ππ for some π½ β πΌ . Γ Proof. Define π π½ := π β π½ ππ for π½ β πΌ . Consider π½ β πΌ such that π π½ β© π = 0; check that the union of a nested collection of these π½ is a subset π½ β² with π π½ β² β© π = 0. Then there exists a maximal such π½ . π π½ β© π = 0 by construction, 6
and π π½ + π = π. If not, there exists ππ β π π½ + π , and we could then replace π½ with π½ βͺ {π}, contradiction. Theorem 1.34: Every π
-module is semisimple iff π
= 2
2.1
π=1 Matππ (π·π )
Γπ
β‘
where the π·π are skew fields.
Semisimple modules, socles, Artinian rings, Wedderburnβs Theorem
More on semisimple modules
Example 2.1: Let π· be a skew field. Then π· π is a simple module over Matπ (π·): given any nonzero vector π£ β π· π , thereβs a change of basis matrix π such that ππ£ = (1, 0, . . . , 0), and we can then use permutation matrices to get all the other basis vectors. Therefore, Matπ (π·) (π£) = π· π . Corollary 2.2: Subquotients and sums of semisimple modules are semisimple. Proof. First, we show that submodulesΓ of semisimple modules are semisimple. Let π submodule. Then by Lemma 1.33, π β π β π½ πΏπ π. Therefore, the composition π β©β π β
Γ
πΏπ π β
πβπ½
Γ
Γ
π βπΌ
πΏπ and π β π a
πΏπ
π β π½ \πΌ
is an isomorphism and π is semisimple. Γ Then quotients of semisimple π are of the form π/π for π a submodule, so by the above π/π π β π½ πΏπ and is semisimple. Γ Γ Γ Γ Finally, Γππ is semisimple because there is a surjection ππ β ππ , so ππ is a quotient of the semisimple module ππ . β‘ Γπ Example 2.3: Matπ (π·) is semisimple over itself. It can be decomposed as π=1 Matπ (π·) (ππ ) where ππ are the standard basis vectors: each summand is matrices that have zeroes everywhere except the πth column. Therefore, Matπ (π·) (ππ ) π· π ; combined with Example 2.1, Matπ (π·) is then semisimple.
2.2
Socles
Definition 2.4: The socle of a module π, denoted Soc(π), is the sum of all semisimple (or simple) submodules of π. Equivalently, it is the maximal semisimple submodule of π. Example 2.5: Let π = C[π‘] as a C[π‘]-module. Then Soc(π) = 0. Submodules of π are ideals in C[π‘], and an ideal is simple iff it contains no other ideals. But if πΌ β 0, π‘πΌ β πΌ , so (0) is the only simple submodule of π. Example 2.6: Let π = C[π‘]/π‘ π as a C[π‘]-module. Then Soc(π) = π‘ πβ1 π and is one-dimensional. The submodules of π are all of the form π‘ π π, so they are simple iff π = π β 1; otherwise, π‘ (π‘ π π) β π‘ π π. Hence the only simple submodule of π is π‘ πβ1 π. Example 2.7: Let πΊ be a finite π-group and π be a field of characteristic π. Let π = π [πΊ] as a π [πΊ]-module. Then Soc(π) = π. To see that, we will show that the only simple πΊ-module is π. We will induct on the order of πΊ. Our base case is πΊ = Z/πZ. Let π be a simple πΊ-module. Because (π β 1) π = 0 for all π β πΊ, ker(π β 1) β 0 β ker(π β 1) = π . So π = 1 and π must be the trivial representation. Now suppose πΊ is an arbitrary π-group and π an irreducible πΊ-module. Then πΊ has a nontrivial center (can be shown by using the class equation), and the center must contain Z/πZ. In particular Z/πZ is a normal subgroup of πΊ, so π Z/πZ is a nonzero πΊ/(Z/πZ)-representation. By induction, it contains a copy of the trivial representation, and so π has a πΊ-invariant vector. So 0 β π πΊ β π and π must be trivial.
7
2.3
Isotypic components
Γ For a semisimple module π π πΏπ , the direct sum decomposition is not canonical; for example, vector spaces have many different bases. But we see that the multiplicity of each πΏπ is fixed: the number of summands πΏπ isomorphic to πΏ is dimπ· (Hom(πΏ, π)), π· = End(πΏ) op . Moreover, the sum of such πΏπ is well-defined because it is generated by the images of all maps πΏ β π (in fact, all embeddings πΏ β©β π). Definition 2.8: Using the above notation, component of π is the sum of the images of all embedΓ the πΏ-isotypic Γ dings πΏ β©β π. Equivalently, if π πΏπ , it is πΏπ πΏ πΏπ . Proposition 2.9: π is semisimple iff any short exact sequence 0 β π1 β π β π2 β 0 splits. Proof. If π is semisimple, Lemma 1.33 and Corollary 2.2 imply that every short exact sequence of the above form splits. So suppose that every short exact sequence of the above form splits. Consider the short exact sequence 0 β Soc(π) β π β π β 0; thus we can write π = Soc(π) β π and the module π has no simple submodules. Notice that any submodule of π β² β π is a summand of π : consider the complement of π β² + Soc(π) in π and project down to π . Now take some π β 0, π β π and let π β² := π
π β π . By Corollary 1.30, π β² has a simple quotient, say πΏ, and by the same argument πΏ must be a summand of π . But π has no simple submodules, a contradiction. β‘
2.4
Classification of semisimple rings
Theorem 2.10: Every π
-module is semisimple iff π
is semisimple over itself iff π
= are skew fields. (This is an augmented version of Theorem 1.34.)
π=1 Matππ (π·π )
Γπ
where the π·π
Proof. The first equivalence comes from the fact that every π
-module is a quotient of a free module, so if π
is semisimple, so is π
πΌ , and so are any quotients of π
πΌ (see Corollary 2.2). If π
is a finite product of matrix rings, Example 2.3 implies that π
is semisimple Γover itself. To show the last implication, assume π
is semisimple over itself and write π
= πΏπ . This sum Γ is finite because π
is cyclic (it is generated by 1), so if the sum were over an index set π β πΌ , we could write 1 = π β π½ βπΌ ππ where |π½ | < β Γ and ππ β πΏπ , so π
= π β π½ πΏπ . (The same argument would work for any finitely generated module.) Anyway, write π
as the sum of its isotypic components, say Γ π πΏπ π , πΏπ β πΏπβ² β π β π β². π βπ½
We know that π
op
! = Endπ
(π
) = Endπ
Γ π βπ½
π πΏπ π
=
Γ
Matπ π (Endπ
(πΏ π ))
π βπ½
and if we let π· π = (Endπ
(πΏ π )) op , we get an isomorphism Γ π
Matπ π (π· π ). π βπ½
β‘ Remark 2.11: It would seem natural to call rings π
semisimple over themselves semisimple. However, there is a separate notion of a simple ring, and not all simple rings are semisimple over themselves (see Example 2.13 below).
8
2.5
Simple rings and Wedderburnβs Theorem
Definition 2.12: A ring π
is simple if π
has no 2-sided ideals except for 0 and π
. Example 2.13: π
= Cβ¨π₯, ππ₯ β© is simple but not semisimple. To see that π
is not semisimple, consider π
/π
(π₯ ππ₯ ). This module has a surjection to π
/π
(ππ₯ ) that does not split (exercise). Definition 2.14: A ring π
is left (resp. right) Noetherian if every ascending chain of left (resp. right) ideals of π
stabilizes (called the ascending chain condition). Equivalently, every left (resp. right) ideal is finitely generated. Definition 2.15: A ring π
is left (resp. right) Artinian if every descending chain of left (resp. right) ideals of π
stabilizes (the descending chain condition). Warning : Being left Artinian/Noetherian is not equivalent to being right Artinian/Noetherian! Theorem 2.16 (Wedderburn): Let π
be a ring. TFAE: a) π
is simple and (either left or right) Artinian, b) every π
-module is semisimple and π
has a unique simple module up to isomorphism, c) π
Matπ (π·) where π· is a skew field. Proof. The equivalence of π) and π) follows from Theorem 2.10: if π
is a finite product of matrix rings over skew fields, check that Matπ (π·) is simple over itself, and so π
has a unique simple module iff the product only contains one matrix ring. This also shows that π) implies π). So suppose that π
is left Artinian and simple. Then Γ π
has a minimal left ideal (because any descending chain of left ideals will stabilize), call it πΏ. Notice that πΏπ
= π₯ βπ
πΏπ₯ is a nonzero two-sided ideal, hence all of π
, and π
= πΏπ
. Γ So π
as a left π
-module is a quotient of π₯ βπ
πΏ, and π
is semisimple over itself. Thus π) implies π) by use Theorem 2.10. β‘ 3
February 14: Isotypic decomposition, Density Theorem, Noetherian and Artinian properties, Jacobson radical
3.1 π [πΊ]-modules Example 3.1: Let πΊ be a finite group and π a field of characteristic not dividing |πΊ | (for simplicity, letβs say char π = 0, but the result holds in general). Then all π [πΊ]-modules are semisimple. We will show that every short exact sequence 0 β π β π β πΏ β 0 splits. WLOG, we can assume that πΏ is finite-dimensional. Tensoring with πΏ β and using the fact that HomπΊ (π ,π ) = (π β β π )πΊ when π is finitedimensional, it suffices to show that for π β πΏ, the restriction to π πΊ β πΏπΊ is also onto. But this is true because Γ Λ and consider |πΊ1 | π(π£), Λ which lies in π πΊ and maps to π£. given π£ β πΏπΊ , choose any preimage of π£ in π, say π£, Corollary 3.2: Suppose that π is algebraically closed and |πΊ | does not divide char π. Then |πΊ | = the ππ are the isomorphism classes of simple π [πΊ]-modules.
Γ
(dim ππ ) 2 where
Proof. The only finite skew field extensions of π are trivial if π is algebraically closed. Hence, by Theorem 2.10 Γ π [πΊ] semisimple means it can be written as ππ=1 Matππ (π), and the simple π [πΊ]-modules are exactly π ππ , while Γ 2 the dimension of π [πΊ] over π is ππ . β‘
3.2
Density Theorem
Theorem 3.3 (Density Theorem): Let πΏ be a simple π
-module and π· = Endπ
(πΏ). Then given any finite set π₯ 1, . . . , π₯π , π¦1, . . . , π¦π β πΏ with the π₯π linearly independent over π·, there exists π β π
such that π (π₯π ) = π¦π .
9
Proof. Let π = (π₯ 1, . . . , π₯π ). We want to show that the map π
β πΏπ taking π β¦β ππ is onto. Suppose that π
π β πΏπ is a proper submodule, say π . Since πΏπ is semisimple, we can then decompose πΏπ = π β π, π β 0. Therefore, π· π = Homπ
(πΏ, πΏπ ) = Homπ
(πΏ, π ) β Homπ
(πΏ, π). Therefore, there exists some (π 1, . . . , ππ ) β π· π annihilating the proper subspace Hom(πΏ, π ) (acting via the dot product), so the π₯π are linearly dependent, a contradiction. β‘ Remark 3.4: The submodules in an isotypic component πΏπ β π are in bijection with vector subspaces in π· π , π· = End(πΏ). The correspondence sends π β πΏπ to Hom(πΏ, π ) β Hom(πΏ, πΏπ ) = π· π (exercise). Corollary 3.5: If πΏ is finite-dimensional simple over π· := Endπ
(πΏ), then there is a surjection π
β Endπ· (πΏ) Matπ (π·), π = dimπ· (πΏ). Example 3.6: This is not true if π is infinite-dimensional over π·. For example, let π
= End(Cβ ) and π = Cβ . Then π· = Endπ
(π) = C but there is no surjection π
β Endπ· (π) (see Corollary 1.22).
3.3
Noetherian and Artinian modules
Definition 3.7: A module is Noetherian (resp. Artinian) if every ascending (resp. descending) chain of submodules stabilizes. Remark 3.8: Weβll see that every Artinian ring is also Noetherian, but this is not true for modules. Example 3.9: Let π
= Z. Then π = Z is a Noetherian module, but it is not Artinian because (π) β (π 2 ) β (π 3 ) β Β· Β· Β· is an infinite descending chain of submodules. Meanwhile, π = Q/Z is Artinian, but it is not Noetherian, because π1 π β π12 π β Β· Β· Β· . Proposition 3.10: A module is Noetherian iff every submodule is finitely generated. Proof. Let π be an π
-module. If every π β Γ π is finitely generated, suppose we had an ascending chain of submodules π1 β π2 β Β· Β· Β· β and consider π = ππ . Because π is finitely generated, say with generators π₯ 1, . . . , π₯π , there exists some π with ππ β {π₯ 1, . . . , π₯π }, and the ascending chain stabilizes at ππ . Now suppose that π is Noetherian and π β π is a submodule. Obtain a list of generators π₯π β π by taking π₯ 1 β 0 and π₯π any element not in ππ β1 := β¨π₯ 1, . . . , π₯π β1 β©. The ascending chain π 1 β π 2 β Β· Β· Β· must stabilize eventually, say at ππ , and π₯ 1, . . . , π₯π then generate π . β‘ Proposition 3.11: If 0 β π1 β π β π2 β 0 is a short exact sequence and π1, π2 are Noetherian (resp. Artinian), then π is also Noetherian (resp. Artinian). Proof. Clear.
3.4
β‘
Composition Series
Definition 3.12: A composition series of a module π is a filtration π0 = 0 β π1 β π2 β Β· Β· Β· β ππ = π where ππ /ππ β1 is simple for all π. That is, the filtration has simple associated graded subquotients. If π has a composition series, we say that it is of finite length and say that π has length π. Lemma 3.13: A module π has finite length iff π is both Noetherian and Artinian. Proof. First, suppose π has a composition series. Then induct on the length of π. If π has length 1, itβs simple, and therefore both Noetherian and Artinian. If π has length π, then 0 β ππβ1 β π β πΏ β 0 and ππβ1, πΏ are Noetherian and Artinian by induction, so π also is. Now suppose π is both Noetherian and Artinian. Because π is Artinian, by Zornβs Lemma any nonempty collec-
10
tion of submodules has a minimal element. So let π1 β π be a minimal nonzero submodule; it must be a simple submodule. Now inductively define ππ+1 to be the minimal submodule properly containing ππ ; this will exist unless ππ = π, and ππ+1 /ππ will be simple. This chain of submodules will terminate because π is Noetherian, so ππ = π for some π and we have constructed a composition series for π. β‘ Definition 3.14: Let π1 β Β· Β· Β· β ππ = π be a composition series for π. The associated graded of the composition series is π Γ gr(π) := ππ /ππ β1 . π=1
Theorem 3.15 (Jordan-HΒ¨older): Given two composition series ππ , ππβ² of π, gr(π) = grβ² (π). Equivalently, the number of irreducible subquotients isomorphic to a given simple module πΏ is independent of the choice of filtration. Proof. Induct on the length of ππ . If ππ has length 1, π is simple and both filtrations contain only π with multiplicity 1. If not, consider the smallest π such that πΏ = π1 β π πβ² . Since πΏ β π πβ² β1 , there is a nonzero map πΏ β π πβ² /π πβ² β1 = grβ²π (π), and a nonzero map between simples is an isomorphism. Hence grβ²π (π) πΏ. Therefore, π/π1 has two filtrations: one given by πΒ― π = ππ+1 /π1 and one defined by πΒ― πβ² is the image of ππβ² when β² /π when π β©Ύ π. We know that we get gr(π) = grβ² (π) from removing one copy of πΏ from gr(π) π < π and ππ+1 1 and grβ² (π), so by induction, gr(π) = grβ² (π). β‘ Remark 3.16: Inspecting the proof of Theorem 3.15, we see that a stronger version of it holds. This stronger version claims that for two composition series 0 β π1 β . . . β ππ = π, 0 β π1β² β . . . β ππβ² = π of π there βΌ βΌ exists a canonical bijection π : {1, . . . , π} ββ {1, . . . , π} and a canonical isomorphism ππ /ππ β1 ββ ππβ² (π ) /ππβ² (π ) β1 . This version of the theorem is interesting already for π
= π (so π is a finite-dimensional vector space): in this case, composition series of π are flags of subspaces in π, and π describes a βrelative positionβ of these two flags with respect to each other. Definition 3.17: Let M be a collection of π
-modules closed under subquotients. The Grothendieck group πΎ (M) is the free abelian group generated by [π], π β M, subject to the relations [π] = [π1 ] + [π2 ] when there is a SES 0 β π1 β π β π2 β 0. Remark 3.18: For π΄ an abelian group, any function M β π΄ additive on subquotients then induces a map πΎ (M) β π΄. For example, if π
= π· and M consists of the finite-dimensional vector spaces, dimension is such a function. Corollary 3.19: Let M be the modules of finite length over π
. Then πΎ (M) is freely generated by [πΏ] for (isomorphism classes of) irreducible modules πΏ. Proof. The existence of a composition series for each π β M means that the [πΏ] generate πΎ (M). To see that the [πΏ] have no relations, notice that Jordan-HΒ¨older implies that thereβs a well-defined homomorphism πΎ (M) β Z sending [π] to the multiplicity of πΏ in the Jordan-HΒ¨older series of π. Thus every [π] has a unique decomposition into the [πΏ]. β‘
3.5
Jacobson Radical
Definition 3.20: The Jacobson radical π½ = π½ (π
) of a ring π
is the intersection of the annihilators of all simple π
-modules. The Jacobson radical has many characterizations.
11
Lemma 3.21: For π β π
TFAE: a) π β Ann(πΏ) for all simple π
-modules πΏ (i.e., π β π½ (π
)), b) π β πΌ for all maximal left ideals πΌ , c) 1 β π₯π has a left inverse for all π₯, d) 1 β π₯ππ¦ has an inverse for all π₯, π¦, e) 1 β ππ₯ has a right inverse for all π₯, f) π β πΌ for all maximal right ideals πΌ , g) π β Ann(πΏ) for all simple π
op -modules πΏ (i.e., π β π½ (π
op )). 4 February 16 - Socle and cosocle filtrations, Jacobson radical, Krull-Schmidt
4.1
Socle and cosocle filtrations
Definition 4.1: The socle filtration of a module πis defined inductively as follows: π1 is the socle of π (see Definition 2.4) and ππ is the preimage of the socle of π/ππ β1 in π. Remark 4.2: The socle filtration can be generalized to transfinite numbers (e.g. ordinals), in which case it is called the Loewy filtration, but we wonβt talk about it. Definition 4.3: The cosocle filtration of an Artinian module π is also defined inductively: π 1 is the kernel of the map from π to its maximal semisimple quotient (called the cosocle), π 2 is the kernel of the map from π 1 to its cosocle, and so on. Remark 4.4: If π is Artinian, then the cosocle filtration always exists, but this is not true in general because π may not necessarily have a maximal semisimple quotient. One could consider all possible simple quotients Γ π β πΏπ and get a Γ map π β πΏπ , but this infinite product need not be semisimple. For example, this occurs when π
= Z; then π Z/πZ is not semisimple. But if π is Artinian, we know the intersection of the kernels of all maps π β πΏπ is equal Γ to the intersection of the kernels of finitely many such maps: we can order the kernels of all maps π β ππ=1 πΏπ to create a decreasing sequence of submodules, which must stabilize. Hence, there exists a maximal quotient corresponding to the Γ stabilized kernel, π β ππ=1 πΏπ . By definition, any map π β π where π is semisimple factors through this Γπ image, so π=1 πΏπ is the maximal semisimple quotient. Example 4.5: Let π
= C[π‘] and suppose that π is a finite-dimensional π
-module where π‘ acts nilpotently. Then ππ = ker(π‘ π ) and π π = im(π‘ π ).
4.2
Jacobson radical cont.
Proof (of Lemma 3.21). a) implies b): for any πͺ β π
, π
/πͺ is simple, so π annihilates π
/πͺ β π β πͺ. b) implies a): the annihilator of every simple module is a proper ideal in π
, thus contained in some maximal left ideal. c) implies b): if there exists a maximal ideal πͺ with π β πͺ, then there exists π₯ such that π₯π β‘ 1(mod πͺ). Hence 1 β π₯π is not invertible. b) implies c): first note that π‘ β π
is left invertible iff π
π‘ = π
iff π‘ does not belong to a proper left ideal. By Zornβs Lemma, this is equivalent to π‘ β πͺ for some maximal left ideal. So if π β πͺ for all maximal πͺ, 1 β π₯π β πͺ and 1 β π₯π is left invertible. d) implies c) follows from setting π¦ = 1. c) implies d): the set of all π satisfying a), b), c) forms a 2-sided ideal by a). So π₯ππ¦ also lies in this ideal and 1 β π₯ππ¦ has a left inverse by c); say it is 1 β π. Then (1 β π) (1 β π₯ππ¦) = 1, and so π also lies in the two-sided ideal. By c), 1 β π then has a left inverse, which implies that 1 β π₯ππ¦ is invertible. Since d) is left-right symmetric, e), f), and g) follow. β‘
12
Remark 4.6: If π is nilpotent with ππ = 0, then 1 β π is invertible with inverse 1 + π + Β· Β· Β· + ππβ1 . Hence, if π₯ππ¦ is nilpotent for all π₯, π¦, then π β π½ . β Example 4.7: Let π
= C[π₯ 1, . . . , π₯π ]/πΌ . The Jacobson radical of π
is πΌ /πΌ , which follows from Hilbertβs Nullstellensatz. Example 4.8: If π
is a commutative local ring, then π½ (π
) = πͺ, the unique maximal ideal. Example 4.9: If π
β Matπ (π) is the subalgebra of upper triangular matrices, then π½ (π
) is the strictly upper triangular matrices (zeroes on the diagonal).
4.3
Local rings and indecomposable modules
Definition 4.10: A ring π
is local if all non-invertible elements form an ideal, in which case said ideal is π½ (π
). If π
is local, π
/π½ (π
) is a skew field. Definition 4.11: A module π is indecomposable if it cannot be decomposed as a direct sum of nonzero submodules π1 β π2 . Example 4.12: Let π
= C[π‘], π = Cπ , and π‘ acts by some matrix π΄. Then π is indecomposable iff π΄ has only one Jordan block. Remark 4.13: π is indecomposable iff Endπ
(π) has no nontrivial idempotents, i.e. elements π such that π 2 = π. If π β Endπ
(π), then we could write π = ππ β π (1 β π): ker π = im(1 β π) because (1 β π) 2 = 1 β π, so ππ = 0 β (1 β π)π = π β (1 β π)π = π for some π. Conversely, given a decomposition π = π1 β π2 , we could set π = ππ1 : π β π1 . Remark 4.14: If we took an idempotent of π
instead of Endπ
(π), we would still get a splitting π = ππ β(1βπ)π, but this would only be a direct sum of abelian groups, not of π
-modules. Proposition 4.15: If π is indecomposable of finite length, then Endπ
(π) is local. Lemma 4.16: If π is an indecomposable finite length module, every π β Endπ
(π) is either nilpotent or invertible. Proof. For every π β End(π), consider the chains ker(π) β ker(π 2 ) β Β· Β· Β· β and im(π) β im(π 2 ) β Β· Β· Β· β. Because π is both Artinian and Noetherian, these both stabilize. Let π = ππ where π is such that ker(ππ+1 ) = ker(ππ ) and im(ππ+1 ) = im(ππ ). Thus ker(π 2 ) = ker(π), im(π 2 ) = im(π). We claim that then π = ker(π) β im(π). For π₯ β End(π), since im(π 2 ) = im(π), there exists π¦ such that π 2π¦ = ππ₯. So π₯ βππ¦ β ker(π) and π₯ = (π₯ βππ¦) +ππ¦ β π = ker(π) + im(π). To see that itβs the direct sum, note that π₯ β ker(π) β© im(π) implies π₯ = ππ¦ and ππ₯ = π 2π¦ = 0, but ker(π 2 ) = ker(π), so ππ¦ = 0 β π₯ = 0. Hence ker(π) β© im(π) = {0}. Since π is indecomposable, either ker(π) = 0 and im(π) = π or im(π) = 0 and ker(π) = π. If ker(π) = 0 and im(π) = π, then ker(π) = 0 and im(π) = π also and so π is invertible. If im(π) = 0, then π = 0, so π is nilpotent. β‘ Proof (of Proposition 4.15). If π β Endπ
(π) is not invertible, itβs nilpotent. Hence ker(π) β 0. So π₯π is also not invertible, hence nilpotent. By the same argument, π₯ππ¦ is also not invertible, hence nilpotent. By Remark 4.6, 1 β π₯ππ¦ is invertible for all π₯, π¦ and thus π β π½ (π
). β‘
13
4.4
Krull-Schmidt
Theorem 4.17 (Krull-Schmidt): a) Every finite length module can be decomposed as a direct sum of indecomposable modules. b) For any two such decompositions, the multisets of isomorphism classes of the indecomposable summands coincide. Example 4.18: Let π
= C[π‘]. Then a finite length module is a finite-dimensional vector space and π‘ acts by a matrix. Indecomposable modules correspond to matrices with a single Jordan block, so in this case, KrullSchmidt is equivalent to saying every matrix has a (essentially unique) Jordan normal form. Proof (of Theorem 4.17). The proof that such a decomposition exists only requires our module to be either Noetherian or Artinian, but not both. Suppose that π cannot be written as a direct sum of indecomposables. So π is not indecomposable, which means it has a decomposition π = π1 β π2 but one of π1, π2 is not a direct sum of indecomposables, WLOG π1 . Then we can split π1 , and inductively continue the process indefinitely. This gives us both an infinite descending chain of submodules (the submodules we split at every step) and an infinite ascending chain of submodules (the complement of those submodules), one of which stabilizes, a contradiction. However, uniqueness requires π to be of finite length. Let π, π be any two π
-modules. Let π = Endπ
(π) op . Then Homπ
(π, π) is a left π-module and Homπ
(π, π) is a right π-module. Even better, we have a pairing Homπ
(π, π) Γ Homπ
(π, π) (π , π)
β Homπ
(π, π) = π β¦β π β¦ π .
If π and π are indecomposable, then π is local with maximal ideal πͺπ = π½ (π). Then we claim that the image of this pairing lands in πͺπ iff π π. Suppose that there exists π , π with π β¦ π invertible; then π π β ker(π). This contradicts the indecomposability of π unless π π. Now consider Homπ
(π, π) := Homπ
(π, π)/πͺπ Homπ
(π, π) and likewise define Homπ
(π, π). Both of these are modules over the skew field π·π := π/πͺπ , i.e. vector spaces, so we get a π·-bilinear pairing Homπ
(π, π) Γ Homπ
(π, π) β π· and this pairing is nonzero iff π π. Moreover, if π is not indecomposable, but instead a direct sum π 1 β π 2 , then Homπ
(π, π) = Homπ
(π, π 1 ) β Homπ
(π, π 2 ) and likewise for Homπ
(π, π), and these direct sum decompositions are compatible with the pairing. Γπ Therefore, if π = π=1 π π for π π indecomposable, we can likewise decompose Homπ
(π, π) and Homπ
(π, π) and deduce that the number of ππ isomorphic to a given π is the rank of the pairing Homπ
(π, π) Γ Homπ
(π, π) β π·. This is independent of the decomposition, so the multiplicities of the isomorphism classes of the indecomposables are unique. β‘ 5
5.1
February 23 - Jacobson radical, primitive and semi-primitive rings
Interlude on quiver representations
While the indecomposables of C[π‘] have a nice classification via Jordan normal form, this is generally a wild problem. For example, one way we can generalize this is by asking how to parametrize finite sets of subspaces of a vector space π . For example, how can we parametrize triples π1, π2, π where π1, π2 β π ? Say two triples π1, π2, π and π1β², π2β², π β² are equivalent when there is an isomorphism π π β² that sends ππ β¦β ππβ² . This is not so bad β these triples are determined up to equivalence by the integers dim ππ , dim π , and dim(π1 β© π2 ).
14
Another nice example is considering invariants for π1, π2, π3, π4 β π when π = R2 . If we require all 4 to be 1dimensional subspaces of R2 , we want to parametrize quadruples of lines on the plane. In general position, no two coincide, and an isomorphism will take one configuration to the other when they have the same cross ratio. So in this case, our invariant is a general element of R, not a bunch of integers. More generally, you could ask how to describe any number of subspaces in a vector space. We can rephrase this question in the language of quiver representations. Recall that a quiver is an oriented graph, and a representation of a quiver is just an assignment of a vector space to each vertex and a map between the corresponding vector spaces for each edge. For example, a representation of the below quiver is 4 vector spaces, one for each vertex, and maps between them. β’ β’ β’
β’
That is, a representation looks like π1 π
π2
π3
and we can define isomorphisms and direct sums of representations, hence speak about indecomposable and simple representations of this quiver. Representations of a quiver π are equivalent to modules of its path algebra π΄(π). So Krull-Schmidt tells us that the decomposition of a finite-dimensional representation into indecomposables has unique multiplicities. Fact: the above quiver has 12 indecomposables, so there are 12 invariants necessary to describe a representation of this quiver (one for each indecomposable multiplicity). The dimension of π1, π2, π3 is at most 1, while the dimension of π is at most 2, in each indecomposable. In three of these, the maps arenβt injective. So quadruples π1, π2, π3 β π are parametrized by 9 invariants, and in fact, we can express these explicitly as intersections.
5.2
Primitive and semi-primitive rings
Definition 5.1: We say a ring π
is semi-primitive if π½ (π
) = 0. Equivalently, π
β©β End(π) for some semisimple π
-module π. Since π½ (π
) = π½ (π
op ), we could also say that π
β©β End(π) for a semisimple π
op -module π. Definition 5.2: We say a ring π
is (left, right) primitive if π
has a faithful simple (left, right) π
-module, that is, π
β©β End(π). There exist rings that are left but not right primitive. So primitive rings correspond to having a faithful simple module, while semi-primitive rings correspond to having a faithful semisimple module. Example 5.3: Simple rings are both left and right primitive: every simple module of a simple ring π
has to be faithful, because ker(π
β End(πΏ)) is a 2-sided ideal in π
, hence 0.
15
Example 5.4: Primitive rings need not be simple. For example, π
= End(Cβ ) is primitive but not simple. It is primitive because Cβ is a simple π
-module, but π
is not simple because operators of finite rank in π
form a two-sided ideal. 2
Example 5.5: Hereβs a more βreal-lifeβ example. consider π
= π (π°π©2 )/(πΆ), where πΆ is the Casimir π π + π π + β2 (a central element). We claim this is primitive but not simple. First, π
can be identified with the ring π of global differential operators on P1 . Verifying this is a hard exercise; here is an outline: π π . To move between copies, note that ππ₯ = On each copy of C, the differential operators are generated by π₯, ππ₯ π π π π βπ₯ β2 ππ₯ β1 . You can show that the global vector fields on P1 are generated by ππ₯ , 2π₯ ππ₯ , π₯ 2 ππ₯ , and the Lie algebra they generate (via taking the commutator of vector fields) has the same relations as π°π©2 . This gives us a map π (π°π©2 ) β π, and you can check that it kills πΆ, so we get a map π
β π, and you then show this map is an isomorphism. (The geometric explanation for this: SL2 acts on P1 , so we get a map from π°π©2 to the Lie algebra of vector fields on P1 . This has a far-reaching generalization describing differential operators on a flag variety as an appropriate quotient of the universal enveloping algebra modulo an ideal generated by central elements.) Anyway, to construct a faithful simple π
-module, note that the differential operators on A1 act on C[π₯], and this induces an action of differential operators on P1 on C[π₯]/C. Exercise: verify this is in fact a faithful simple π
-module. So now we have several examples where primitive rings need not be simple. However, if we add the condition that our ring must be Artinian (e.g. a finite-dimensional algebra over a field), then every primitive ring is in fact simple. Proposition 5.6: A (left or right) Artinian semi-primitive ring has the form Artinian primitive rings are of the form Matπ (π·), hence simple.
π=1 Matππ (π·π ),
Γπ
so (left or right)
Γ Proof. Suppose that π
is Artinian and semi-primitive, i.e. π½ (π
) = 0. We can also write π½ (π
) = πΌπΌ where the intersection is over all maximal left ideals πΌπΌ . Because π
is Artinian, there exists a finite subset of the πΌΓ πΌ such that Γπ πΌ = 0 (consider the infinite descending chain of ideals πΌ , πΌ β© πΌ , . . .. This must stabilize, but also πΌπΌ = 0, so 1 1 2 π=1 π it must stabilize at 0). Γπ Therefore, we have an injection π
β©β π=1 π
/πΌπ . Because each πΌπ is maximal, π
/πΌπ is simple, so π
is a submodule of a semisimple module, hence is semisimple itself. Then by Theorem 2.10, π
is a finite product of matrix algebras. Then the second part follows since the simple representations of π
will be Matππ (π·π ), and these are not faithful unless π
= Matπ (π·). β‘ Corollary 5.7: Suppose π
is Artinian. Then π is semisimple iff π½ (π
)π = 0. The socle filtration on π has ππ = ker π½ (π
)π and the cosocle filtration is π½ (π
)π π. Proof. In one direction, if π is semisimple, then by definition π½ (π
) annihilates all simple, hence all semisimple, modules. In the other, suppose that π½ (π
) acts trivially. Then π is a quotient over π
/π½ (π
). π½ (π
/π½ (π
)) = 0, so this Γ quotient is semi-primitive. It is also Artinian, so π is a module over ππ=1 Matππ (π·π ). This ring is semisimple, so π is semisimple. The second statement follows from the first; for example, the socle is the maximal semisimple submodule of π, which must then be the kernel of π½ (π
), and so on. β‘ Corollary 5.8 (A Version of Nakayama): Suppose π is a finitely generated π
-module such that π½ (π
)π = π. Then π = 0. Proof. If π is nonzero, we know that π has a simple quotient by Corollary 1.30, call it πΏ, and π½ (π
)πΏ = 0. Then π½ (π
)π β π. β‘
16
6
6.1
February 28 - Artinian rings are Noetherian, projective covers
The Akizuki-Hopkins-Levitzki Theorem (Artinian rings are Noetherian)
Lemma 6.1: If π
is Artinian, then π½ = π½ (π
) is a nilpotent ideal, i.e. there exists some π > 0 such that π½ π = 0. Proof. Saying that π½ π = 0 is equivalent to saying that π₯ 1π₯ 2 Β· Β· Β· π₯π = 0 for all π₯π β π½ . Consider the decreasing chain π½ β π½ 2 β Β· Β· Β· β, which stabilizes because π
is Artinian. So let πΌ = π½ π = π½ π+1 ; then πΌ = πΌ 2 also. If πΌ β 0, there exists a minimal left ideal π such that πΌ π β 0 (use that π
is Artinian). Pick π β π such that πΌπ β 0; then πΌ (πΌπ) β 0 and πΌπ β π, so πΌπ = π by minimality of π. Thus, there exists π₯ β πΌ such that π = π₯π, so 1 β π₯ is a zero divisor. But since π₯ β π½ , 1 β π₯ is invertible, contradiction. β‘ Theorem 6.2 (Akizuki-Hopkins-Levitzki): If π
is (left, right) Artinian, then π
has finite length as a (left, right) module over π
. In particular, π
is Noetherian. Proof. Weβll show that ππ := π½ π /π½ π+1 is a finite length π
-module. This module is annihilated by π½ , so itβs semisimple. Recall that semisimple modules are Artinian iff they are Noetherian iff they are a finite sum of irreducibles. But π½ π /π½ π+1 is Artinian, so it has a finite length. Then length(π
) =
πβ1 βοΈ
length(ππ )
π=0
where the sum is finite because π½ π = 0, so π
has finite length.
6.2
Projective covers
Definition 6.3: A module π is projective if Hom(π, β) is exact (takes short exact sequences to short exact sequences). Equivalently, given a surjection π β π, we can lift any map π β π (non-uniquely) to a map π β π . Example 6.4: Free modules are projective. Direct summands of projective modules are also projective, so direct summands of free modules are projective. In fact, the converse is also true, since every projective π has a surjection π
πΌ β π, so we can lift π π to π β π
πΌ , which gives us a splitting of π
πΌ = π β π. Corollary 6.5: Every module is the quotient of a projective module. Definition 6.6: A surjection π : π β π is an essential surjection if for all π β² β π, π | π β² is not onto. That is, no proper submodule of π surjects onto π . Definition 6.7: A projective cover of a module π is an essential surjection π β π from a projective module π. Example 6.8: Let π be a finite length module and π 1 be the first term of the cosocle filtration, so π := π/π 1 = π/π½ π is the maximal semisimple quotient (see Corollary 5.7). Then π β π is an essential surjection. One way to see this: if π β π and π β π = π/π½ π, then (π/π )/π½ (π/π ) = 0. So by Nakayama π/π = 0. In fact, any essential surjection π β π with π semisimple and π finite length has this form. Lemma 6.9: a) Suppose π : π β π is a projective cover and π : π β π is another surjection from a projective π to π. Then we can write π π β π β² with π|π β² = 0 and π|π = π. b) A projective cover (if it exists) is unique up to isomorphism.
17
β‘
πΛ
π
Proof. b) follows from a), so it suffices to prove a). We can lift π to a map πΛ : π β π with π : π β β π β π. Since π Λ β π). But surjective maps between projective modules split, is an essential surjection, π must be onto (as Im(π) so we get the desired splitting of π. β‘ Proposition 6.10: Suppose π
is Artinian. a) Every irreducible module has a projective cover. b) The isomorphism classes of irreducible modules are in bijection with isomorphism classes of indecomposable projectives. This bijection sends πΏ to its projective cover and a projective module to its cosocle (its maximal semisimple quotient). Proof. b) follows from a): let π be an indecomposable projective. Since π is a summand of a free, there is a nonzero map from π to π
, hence π β πΏ for some irreducible πΏ. But ππΏ , the projective cover of πΏ, is a direct summand of π by Lemma 6.9, so π ππΏ . To prove a), it suffices to find a projective ππΏ such that ππΏ /π½ ππΏ πΏ, where π½ = π½ (π
), since then ππΏ β πΏ is an essential surjection (see Example 6.8). We will induct on π such that π½ π = 0. If π = 1, π
is semi-primitive, and thus Γ π
Matππ (π·π ). Here everything is projective, so πΏ = ππΏ . In general, we will use the lifting of idempotents; the below lemma will show that we can lift idempotents from π
/πΌ to π
when πΌ 2 = 0. Suppose π > 1, then π
/π½ is semi-primitive, so there exists an idempotent πΒ― β π
/π½ such that (π
/π½ )πΒ― πΏ. Then we can lift idempotents repeatedly along surjections π
/π½ π+1 β π
/π½ π until we get some π in π
(use Lemma 6.11 below). Then consider ππΏ = π
π. This satisfies ππΏ /π½ ππΏ = (π
/π½ )πΒ― πΏ, and ππΏ is a summand of π
, so we are done. β‘ Lemma 6.11: Let π be a ring and πΌ β π a 2-sided ideal such that πΌ 2 = 0. Then any idempotent π β π
:= π/πΌ can be lifted to an idempotent πΒ― β π. Proof. Let π β² be any lift of π, not necessarily an idempotent. We can decompose πΌ into the direct sum πΌ = π β² πΌπ β² β π β² πΌ (1 β π β² ) β (1 β π β² )πΌπ β² β (1 β π β² )πΌ (1 β π β² ). Note that the decomposition above does not depend on the choice of π β² (use that πΌ 2 = 0). Notice that π := π β² (1 β π β² ) lies in πΌ (as itβs 0 mod πΌ ). Moreover, it satisfies π β²π (1 βπ β² ) = (1 βπ β² )ππ β² = π 2 = 0 (use that πΌ 2 = 0), so in the direct sum decomposition π has only nonzero first and last components. That is, we can write π = π + + π β , where π + β π β² πΌπ β² and π β β (1 β π β² )πΌ (1 β π β² ). Now we claim that πΒ― := π β² + π + β π β is an idempotent lifting of π. Indeed we have Β― = (π β² + π + β π β ) (1 β π β² β π + + π β ) = π β π β²π + β π β (1 β π β² ) = π β π β²π β π (1 β π β² ) = 0. πΒ―(1 β π) β‘ Remark 6.12: An alternative approach to the proof of Lemma 6.11: let π β² be a lift of π and set π β² := 1 β π β² . We β²2 have 1 β π β² 2 β π β² 2 β πΌ is nilpotent so π β² 2 + π β² 2 is invertible and it is easy to see that π β²β² = π β²2π+π β² 2 is the desired lift of π (use that π β² 2 π β² 2 = 0).
Remark 6.13: Let ππΏ be the projective cover of πΏ. Then Homπ
(ππΏ , πΏ β² ) = 0 if πΏ β² β πΏ, and Homπ
(ππΏ , πΏ) is a free op module over π· πΏ , where π· πΏ := Endπ
(πΏ).
18
Γ Corollary 6.14: Let π
be an Artinian ring and write π
/π½ = Matππ (π·π ), π·π = End(πΏπ ) op where the πΏπ are the isomorphism classes of simple π
-modules and ππ = dimπ·π (πΏπ ). Let ππ be the projective cover of πΏπ . Then Γ ππππ π
π
as a left π
-module. Proof. By Theorem 4.17, π
and ππ = ππ .
Γ π
ππππ for some multiplicities ππ . Then Homπ
(π
, πΏπ ) Homπ
(ππππ , πΏπ ), so πΏπ π·πππ β‘
Remark 6.15: Suppose π΄ is a finite-dimensional algebra over an algebraically closed field π. Then Endπ΄ (πΏ) π for all irreducible πΏ. Then we get another proof of Theorem 3.15, as in this case, the multiplicity of πΏπ in π will be dimπ Homπ΄ (ππΏ , π). Corollary 6.16: Let π
be an Artinian ring. Then any finitely generated π
-module has a projective cover. Proof. Induct on length. Consider 0 β πΏ β π β π β 0 where πΏ is simple and suppose we know π has projective cover π π with π : π π β π . If π π β π, then π π is also the projective cover of π. Otherwise, π must split as πΏ β Im(π) = πΏ β π , so ππΏ β π π is a projective cover of π. β‘
6.3
Preview of Morita theory
Γ ππ op If the ππ are the indecomposable projectives of a ring π
, how is π := Endπ
related to π
? It turns out that π ππ when ππ β©Ύ 1, π is Morita equivalent to π
, meaning that their module categories are equivalent. Theorem 6.17: π is Morita equivalent to π
iff π op = Endπ
(π), where π is a finitely generated βprojective generatorβ of π
-Mod. We will precisely define the projective generator next time, but when π
is Artinian, it will be when ππ β©Ύ 1 as mentioned above. 7
March 2 - Categories and Morita equivalence
Γ Remark 7.1: We can also discuss projective covers of graded modules over graded rings. Let π
= πβ©Ύ0 π
π with π
0 Artinian and let πΏ be an irreducible graded module over π
that is concentrated in one degree. WLOG we can assume πΏ is concentrated in degree 0. Then π = π
ππΏ is a graded projective cover of πΏ; ππΏ β π
0 is the idempotent corresponding to the projective cover of πΏ as an π
0 -module.
7.1
Morita equivalence
Definition 7.2: We say that two rings are Morita equivalent if their categories of modules are equivalent. (Below, we will recall some facts about categories.) Theorem 7.3: A ring π is Morita equivalent to a ring π
iff π = Endπ
(π) op where π is a finitely generated projective generator of the category of π
-modules. Definition 7.4: A projective module π over a ring π
is a projective generator if Hom(π, π) β 0 for every nonzero π
-module π. Lemma 7.5: π is a generator iff π
is a direct summand in π π for some π.
19
Proof. If π is a generator, then for every module π , the images of all possible homomorphisms π β π generate π . This is because if π is the sum of all the images of such maps, then Hom(π, π) β Hom(π, π ) is an isomorphism, and since π is a generator, this implies that π π . Γ Now if π is finitely generated, say with generators ππ , and ππ = ππ π (π π ) where ππ π β Hom(π, π ), then only images for those finitely many ππ π are needed to generate π . Hence there is a surjection π π β π . In particular, if we take π = π
, π
is projective, so the surjection splits and π
is a summand of π π . In the other direction, if π
is a summand of π π , this implies π π is a generator, and hence π is a generator also. β‘ Example 7.6: π
is Morita equivalent to itself. In this case, take π = π
(the rank 1 free module), and π
= Endπ
(π
) op . More generally, if we take π = π
π , then π = Endπ
(π
π ) op = Matπ (π
) is Morita equivalentΓ to π
also. Using the lemma, we see that if π
is Artinian with indecomposable projectives π1, . . . , ππ , π = ππππ is a op projective generator iff ππ β©Ύ 1 for all π. In particular, if we take ππ = 1 for all π, then π = Endπ
(π) is whatβs known as a based ring, meaning that each irreducible πΏπ is a one-dimensional vector space over π·π = Endπ
(πΏπ ). Proposition 7.7: Let π = π
π for an idempotent π β π
. Then π is a generator iff π
= π
ππ
. Γ Proof. Suppose π
= π
ππ
. Then we can write 1 = ππ πππ for ππ , ππ β π
, so the map π π β π
given by (π₯ 1, . . . , π₯π ) β β¦ Γ π₯π ππ is onto. So by the lemma 7.5, π is a generator. In the other direction, π = π
/π
ππ
satisfies Hom(π, π) = ππ = 0, so if π β 0, π canβt be a generator. β‘
7.2
Categories and the Yoneda Lemma
Quick review: a (small) category C consists of a set of objects Ob(C), a set of morphisms Hom C (π, π ) for all π, π β Ob(C), an identity morphism idπ β Hom(π, π ), and an associative composition operation. Remark 7.8: Small categories are those where Ob(C) is actually a set. Since there is no such thing as the βset of all setsβ, categories like Set or π
-Mod are not small. We could get around this by fixing a universe and only considering sets from this universe. We could also consider βlargeβ categories, whose objects form a collection more general than a set, called a class. We will ignore all these set-theoretic issues. Given two categories C1, C2 , we can talk about the category of functors Fun(C1, C2 ) whose objects are functors and whose morphisms are natural transformations. Definition 7.9: A functor πΉ is faithful if the map Hom(π, π ) β Hom(πΉ (π ), πΉ (π )) is injective for all π, π . Definition 7.10: A functor πΉ is fully faithful if the map Hom(π, π ) β Hom(πΉ (π ), πΉ (π )) is an isomorphism. Definition 7.11: A functor πΉ is essentially surjective if it is surjective on isomorphism classes of objects. Definition 7.12: A functor πΉ : C1 β C2 is an equivalence of categories if there exists πΊ : C2 β C1 such that πΉ β¦ πΊ, πΊ β¦ πΉ are isomorphic to the respective identity functors (that is, they are naturally equivalent to the identity functors). Lemma 7.13: A functor πΉ is an equivalence of categories iff it is fully faithful and essentially surjective. Proof. Since we are ignoring set-theoretic considerations, we get to use the axiom of choice. Itβs clear that if πΉ is an equivalence, then itβs fully faithful and essentially surjective. In the other direction, if πΉ is essentially surjective, the axiom of choice allows us to choose π β Ob(C2 ) and πΊ (π ) β Ob(C1 ) such that ππ : π πΉ (πΊ (π )). Then we can define πΊ (π : π β π ) as follows: first ππβ1 β¦ π β¦ ππ gives a map πΉ (πΊ (π )) β πΉ (πΊ (π )), and because πΉ is fully faithful, this corresponds to a unique πΊ (π ) : πΊ (π ) β πΊ (π ). Then one can verify that πΊ is indeed a functor and that πΉ β¦ πΊ and πΊ β¦ πΉ are equivalent to id Cπ . β‘
20
Lemma 7.14 (Yoneda Lemma): For a category C, consider the functors π
: C op β Fun(C, Set) and πΆ : C β Fun(C op, Set) where π
(π ) : π β¦β Hom(π,π ) and πΆ (π ) : π β Hom(π , π ). Then π
, πΆ are fully faithful. Here π
is for βrepresentβ and πΆ for βcorepresentβ. Proof (Sketch). For π, π β Ob(C), thereβs a natural map Hom(π, π ) β Hom(π
(π ), π
(π )) given by composing with the map π β π . In the other direction, given π : π
(π ) β π
(π ), send it to the element π (idπ ) β Hom(π, π ). Itβs easy to see these are inverse bijections. The argument for πΆ is similar. β‘ That is, an object in C is uniquely defined up to unique isomorphism up to the functor it (co)represents. Example 7.15: The initial (resp. final) object of a category C is an object πΌ (resp. πΉ ) such that Hom(πΌ, π ) (resp. Hom(π, πΉ )) is a singleton. By the Yoneda lemma, initial and final objects are unique up to unique isomorphism (if they exist). For example, in the category π
-Mod, the zero module is both initial and final. Definition 7.16:ΓThe coproduct representing (resp. corepresenting) the product of Γ (resp. product) is the object Γ Γ Hom sets: Hom ( ππ ,π ) = Hom(ππ ,π ) and Hom (π , ππ ) = Hom(π , ππ ). These are unique up to unique isomorphism if they exist. Example 7.17: In π
-Mod, these both exist; coproduct is the direct sum and product is the usual product. Remark 7.18: We can characterize the statement that a finite direct sum is the same as a finite product in Γ Γ Γ categorical terms. Using the final object 0, there is a morphism ππ β ππ . Hence, there is a map ππ β ππ , and this is an isomorphism when the ππ form a finite collection. Remark 7.19: This can also be used to show that Hom(π, π ) has an abelian group structure. You can define the sum of two maps π , π : π β π as the composition idπ β¨Ώ idπ
π Γπ
π ββββ π Γ π π β¨Ώ π ββββββββ π .
7.3
Proof of Morita equivalence theorem
Proof (of Theorem 7.3). Suppose πΉ : π-Mod β π
-Mod is an equivalence. We will show that π := πΉ (π) is a finitely generated projective generator in π
-Mod and that π = Endπ (π) op = Endπ
(π) op . This follows from the following observations: β’ πΉ sends projective π-modules to projective π
-modules. π is projective iff Hom(π, β) is exact, i.e. sends a surjective map of modules to a surjective map of sets. A map of modules π1 β π2 is surjective iff Hom(π2, π ) β©β Hom(π1, π ) is injective for all π . Using essential surjectivity of πΉ , we find π 1, π 2, π β π-Mod such that πΉ (ππ ) ππ and πΉ (π ) π ; then the full faithfulness of πΉ implies that π 1 β π 2 . Then Hom(π, π 1 ) β Hom(π, π 2 ) combined with full faithfulness of πΉ translates this into Hom(πΉ (π),π1 ) β Hom(πΉ (π),π2 ). β’ πΉ sends a projective generator to a projective generator, since Hom(π, π ) = 0 β Hom(πΉ (π), πΉ (π )) = 0 by full faithfulness of πΉ . β’ πΉ sends finitely generated projective π-modules to finitely generated projective π
-modules. Use the following characterization of finitely generated projectives: a projective Γ Γ π is finitely generated iff Hom(π, β) commutes with arbitrary coproducts (i.e. Hom(π, ππ ) = Hom (π, ππ ). If π is projective and finitely generated, itβs a direct summand of π π , which has this property, so π also has this property. In the other direction, suppose Γ Hom(π, β) commutes with coproducts. We is the direct summand of some free module, say πΌ π, Γknow πΓ Γ which then splits as π β Γ π. Then Hom(π, πΌ π) = Hom(π, π), so the image of π β©β π must land in πΌ πΌ π will also split as π β (π β© π π ), so π is in fact finitely generated. a finite direct sum π π = π, |π½ | < β. π π½ Since πΉ is an equivalence of categories, it preserves the property that Hom(πΉ (π), β) commutes with arbitrary coproducts, so πΉ (π) is also finitely generated projective. Combining these three, we get that πΉ (π) is a finitely generated projective generator. Because πΉ is fully faithful, 21
Homπ (π, π) Homπ
(πΉ (π), πΉ (π)) = Endπ
(π), so π = Endπ
(π) op . In the other direction, we want to show that if π = Endπ
(π) op for π a finitely generated projective generator π of π
-Mod, the functor πΉπ : π β¦β Homπ
(π, π) is the desired equivalence of categories. Here π β π
-Mod and Homπ
(π, π) has an π-action via composition. πΉπ induces an isomorphism Homπ
(π, π ) Homπ (πΉπ (π), πΉπ (π )) for all π : the RHS will be Homπ (π, πΉπ (π )) πΉπ (π ) = Hom(π, π ). This isomorphism coincides with the πΉπ -action on morphisms. Since π is finitely generated and projective, πΉπ commutes with coproducts. Moreover, π is a projective generator, we claim we can find an exact sequence π βπ½ β π βπΌ β π β 0. Lemma 7.20: A projective module π is a generator iff the free module π
is a direct summand in π π for some π iff every module is a quotient of π βπΌ . Now we want to show that Hom(π, π ) β Hom(πΉπ (π), πΉπ (π )) is an isomorphism. Notice that if this is true for π1, π2 , itβs also true for coker(π ), π : π1 β π2 because exactness of πΉπ implies that both Hom-spaces are the kernel of the map Hom(π2, π ) β Hom(π1, π ). So by the above, it suffices to show that this is true for π = π βπΌ , but that is what we proved above. So πΉπ is fully faithful. π
To see that πΉπ is essentially surjective, take π β π-Mod, which fits in an exact sequence π βπ½ β β π βπΌ β π β 0. Because πΉπ is fully faithful, π = πΉπ (π) for π : π βπ½ β π βπΌ . Hence π πΉπ (coker(π)). Thus, πΉπ is an equivalence of categories. β‘ Example 7.21: Now itβs interesting to consider notions that are invariant under Morita equivalence. We will see that the center π (π
) and cocenter πΆ (π
) of a ring are such notions, i.e. if π
, π are Morita equivalent, they have the same center and the same cocenter. 8
8.1
March 7 - Morita theory continued: (co)centers, functors and bimodules
Center and cocenter
Last time, we claimed that the center and cocenter are Morita invariant notions. Recall that the center π (π
) is defined as π (π
) := {π§ β π
| π§π = ππ§ βπ β π
} and is a commutative subring in π
. The cocenter πΆ (π
) is πΆ (π
) := π
/
βοΈ
[π¦π , π₯π ],
π
i.e. the quotient of π
by combinations of the commutators of elements in π
. πΆ (π
) is an abelian group and an π (π
)module, but generally does not have a ring structure. Proposition 8.1: If π
βΌπ π, then π (π
) π (π), πΆ (π
) πΆ (π). Remark 8.2: We will see later that π (π
) = HH0 (π
), the 0th Hochschild cohomology, and πΆ (π
) = HH0 (π
), the 0th Hochschild homology, and that the πth Hochschild (co)homology is also Morita invariant. Proof. We will need several intermediate lemmas that allow us to describe π (π
) and πΆ (π
) purely in terms of the category of modules. Lemma 8.3: π (π
) End(Idπ
), i.e. endomorphisms of the identity functor in π
-Mod, as commutative rings. Proof. An element in End(Idπ
) is a collection of maps π§π β End(π) such that π§ π β¦ π = π β¦ π§π for all π : π β π maps of π
-modules. If we take a central element π§ β π
, it corresponds to the functor where π§π is just the left action of π§ on π. If we are given a collection π§π , consider π§π
; note that it must commute with left multiplication by π for all π β π
, so it must be a central element. Hence we get the desired isomorphism. β‘
22
Definition 8.4: Let Projπ
be the category of finitely generated projective π
-modules. A trace map for Projπ
with values in an abelian group π΄ is an assignment of an element π (π, π) β π΄ for every π β Ob(Projπ
), π β End(π), such that π (π β π, π β π ) π (π, π β¦ π)
= π (π, π) + π (π,π ) = π (π, π β¦ π), π : π β π, π : π β π.
Lemma 8.5: Let Projπ
be the category of finitely generated projective π
-modules. Then πΆ (π
) is the universal abelian group receiving a trace map for Projπ
. In other words, πΆ (π
) is isomorphic (as abelian groups) to the quotient of the free abelian group generated by pairs (π, π) by the relations (π β π, π β π ) β (π, π) β (π,π ) and (π, π β¦ π) β (π, π β¦ π) (where π : π β π, π : π β π). Proof. Let us restate this in terms of matrices. Let π΄ = (ππ π ) β Matπ (π
) and set Tr(π΄) =
Γ
πππ (mod[π
, π
]). Then
Tr(π΄π΅) = Tr(π΅π΄). Call the abelian group in the statement πΆΛ (π
). We will use Tr to construct an isomorphism π : πΆΛ (π
) β πΆ (π
). Let π be a finitely generated projective. Then itβs the summand of a free, so choose π, π such that π β π = π
π . Then (π β 0) β End(π
π ) with matrix π΄π . Set π (π, π) := Tr(π΄π ). Then π is independent of choices of π, π and satisfies π (π, ππ) = π (π, ππ). Also, π is clearly additive on direct sums. So π is a homomorphism. It is onto since we can choose Γ π = π
Λ and π multiplication by any element in π
. To see itβs injective, it suffices to show that (π
π , π΄) = (π
, πππ ) in πΆ. But this is true because a matrix with zero sum of diagonal elements will map to 0 in πΆ (Matπ (π
)). β‘ Therefore, center and cocenter depend only on the category π
-Mod, which shows they are Morita invariant.
β‘
Example 8.6: For π β π
, we can consider the operator π
β π
of right multiplication by π. The trace of this map is just [π] β πΆ (π
).
8.2
Morita equivalence via functors and bimodules
Definition 8.7: Let π
, π be rings. An π
, π-bimodule π is an abelian group carrying a commuting left action of π
and right action of π (i.e. a left π op action). We denote such a module by π
ππ . Given a bimodule π
ππ , we get a functor πΉπ : π-Mod β π
-Mod given by π β¦β π βπ π. It is easy to see that πΉπ β¦ πΉπ = πΉπ βπ π for bimodules π
π π and π ππ . Thus, we have a functor from π
, π-Bimod β Fun (π-Mod, π
-Mod). Lemma 8.8: The functor π β¦β πΉπ is fully faithful. Proof. There is a natural map Hom(π, π) β Hom(πΉπ , πΉπ ). To construct a map in the other direction, note that π = πΉπ (π), and this is an isomorphism of π
, π-bimodules because the right action of π on πΉπ (π) is obtained by applying πΉπ to End(π). This defines a map Hom(πΉπ , πΉπ ) β Hom(π, π), and you can check that itβs the inverse bijection to the first map. β‘ Remark 8.9: In the proof of the Morita equivalence theorem last time, we used the functor π β¦β Homπ
(π, π). This can be written as π β¦β πΛ βπ
π, where πΛ = Homπ
(π, π
) as a right π
-module. We could rewrite Endπ
(π) op = Λ In fact, π β¦β πΛ gives an equivalence of categories Projop β Projπ
op . Endπ
op (π). π
23
Remark 8.10: Recall that in an equivalence of categories, you have two functors πΉ, πΊ and πΊ β¦ πΉ β Id C , πΉ β¦ πΊ β Id D . It turns out that if you fix πΉ, πΊ, and the first isomorphism of functors, then the second isomorphism of functors is uniquely determined so that if the two isomorphisms πΉ β¦ πΊ β¦ πΉ β πΉ coincide (from either πΉ β¦ Id C or Id D β¦πΉ , the two isomorphisms πΊ β¦ πΉ β¦ πΊ β πΊ also coincide. Therefore, if we want to define a Morita equivalence between π΄, π΅, we can rephrase this as finding π΄ ππ΅ , π΅ π π΄ , which will give us two functors π΄-Mod β π΅-Mod and π΅-Mod β π΄-Mod, such that π β π β π΄ and π β π β π΅, i.e. their compositions are isomorphic to the respective identity functors. Definition 8.11: A Morita context is the data of π΄, π΅, π΄ ππ΅ , π΅ π π΄ with maps π : π βπ΅ π β π΄ and π : π βπ΄ π β π΅ such that the two arrows π βπ΅ π βπ΄ π β π coincide and likewise for π βπ΄ π βπ΅ π β π. This can be rewritten in matrix form: π, π, and the bimodule structures define multiplication on matrices of the form π π , π β π΄, π β π, π β π, π β π΅. π π We can now talk about ππ, as π (π, π), etc., and our compatibility condition means this matrix multiplication is associative. Example 8.12: Let π΅ be a ring and π β π΅-Mod. The derived Morita context is given by π΄ = Endπ΅ (π) op , π = π, π = Homπ΅ (π, π΅), and π (π β π) = π (π), π (π β π) : π β¦β π (π)π. We can verify that the arrows π βπ΅ π βπ΄ π β π coincide: π β π β π β² β¦β π (π) β π β² , which sends π β¦β π β² (π)π (π). The other map is π β π β π β² β¦β π β π (π β π β² ), which sends π β¦β π (π β² (π)π) = π β² (π)π (π). A similar argument holds for π βπ΄ π βπ΅ π β π. Theorem 8.13: For a derived Morita context, the functors given by π, π are inverse equivalences iff π is a finitely generated projective generator. This is a reformulation of the theorem we proved last time. The proof is a consequence of the below lemmas. Definition 8.14: A generator π β π
-Mod is an object such that Homπ
(π, β) is faithful. Lemma 8.15: π is a generator iff for all π , there exists a surjection π βπΌ β π , iff π
is a direct summand of π π . Lemma 8.16: For a derived Morita context, a) π : π βπ΅ π β π΄ is onto iff π = π is a generator over π΄. b) π : π βπ΄ π β π΅ is onto iff π = π is a finitely generated projective over π΄. Proof. By definition im(π) is the sum of images of all homomorphisms π β π΄. So π is onto exactly when the sum of the images is π΄, which is when π is a generator. This proves a). Γ For b), first suppose π is onto. Then 1π΅ = Idπ = ππ=1 ππ ππ where ππ : π β π΄ and ππ : π΄ β π. Then consider the Γ maps π β¦β (π1 (π), . . . , ππ (π)) and (π 1, . . . , ππ ) β¦β ππ ππ . Their composition π β π΄π β π is the identity, so π π is a direct summand of π΄ , implying itβs a finitely generated projective. In the other direction, suppose that π is a finitely generated projective. Then write π = π΄π π for an idempotent π. Then End(π) = π Matπ (π΄)π and we have a surjection π΄π π β ππ΄π β End(π). β‘ Lemma 8.17: In a Morita context, π (resp. π) is onto implies π (resp. π) is an isomorphism. Γ Proof. Suppose that π : π βπ΅ π β π΄ is onto. Then write 1 = π ( ππ β ππ ). Consider the map βοΈ π β π βπ΄ π βπ΅ π, π β¦β π β π π β ππ . Then the composition πβid
π β π βπ΄ π βπ΅ π ββββ π΅ βπ΅ π = π 24
is the identity map. Tensoring with π on the left, we get the identity map π βπ΅ π β π βπ΅ π. But the composition is also equal to π βid
π βπ΅ π β (π βπ΅ π) βπ΄ π βπ΅ π ββββ π΄ βπ΄ π βπ΅ π = π βπ΅ π Γ where the first arrow sends π β π β¦β π β π β ( ππ β ππ ). Since an element in ker π would be killed by this composition, we must have ker π = 0, so π is an isomorphism. A similar argument works for π. β‘
8.3
Serre quotients
Motivating question: suppose that π β π΄-Mod is a finitely generated projective but not a generator and π΅ = Endπ΄ (π) op . How are π΄-Mod and π΅-Mod related? It turns out that π΅-Mod is a Serre quotient of π΄-Mod by {π | Hom(π, π) = 0}. Definition 8.18: A Serre subcategory of an abelian category (defined next time) is a full subcategory closed under subquotients and extensions. That is, for an SES 0 β π1 β π β π2 β 0, π is n the subcategory iff π1, π2 are. Example 8.19: A Serre subcategory in the category of finite length modules is uniquely determined by the set of irreducible objects it contains. So such subcategories are in bijection with subsets of the set of isomorphism classes of irreducibles. Let A be a Serre subcategory of an abelian category and B β A a Serre subcategory. Definition 8.20: A homomorphism π : π β π is an isomorphism modulo B if ker(π ), coker(π ) β B. Definition 8.21: The Serre quotient A/B is the category with a universal functor A β A/B sending isomorphisms modulo B to isomorphisms. (That is, for any functor A β C sending isos modulo B to isos, thereβs a unique functor A/B β C making the diagram commute.) The Serre quotient has the same objects as A, but different Hom-sets. 9
9.1
March 9 - more on Serre quotients, abelian categories
More on Serre quotients
Let A be a Serre subcategory in π
-Mod and B β A be a Serre subcategory. We defined the Serre quotient abstractly, but here is a more concrete description: β’ Objects of A/B are objects of A. β’ The morphisms Hom A/B (π, π ) are equivalence classes of βroof diagramsβ π β π β² β π , where the left arrow π β π β² is an isomorphism modulo B (i.e. its kernel and cokernel are both in B). Two roof diagrams π β π β² β π and π β π β²β² β π are equivalent if there exists a map π β²β² β π β² commuting with the other π β²β² arrows, i.e. π πβ² Another way to phrase this:
π Hom A/B (π, π ) = colim Hom(π β², π ) β² π βπ
where the colimit is taken over the category of objects π β² β A equipped with isomorphisms modulo B to π. Remark 9.1: We could also phrase Hom A/B in terms of βlower roofβ diagrams, where the arrows are reversed, so Hom A/B (π, π ) consists of diagrams π β π β² β π where π β² β π is an isomorphism modulo B. Why are these definitions equivalent? Given a lower roof diagram, you can construct the upper roof by setting π β² := π Γπ β² π (the pullback), i.e. ker(π β π β π β² ). Given an upper roof diagram, you can set π β² to be the pushforward, namely π β² := coker(π β² β π β π ).
25
Example 9.2: Let A be the category of finite length modules over an Artinian algebra π
and B be the subcategory of modules that do not have some fixed irreducibles πΏ1, . . . , πΏπ in their Jordan-Holder series. Then A/B will be the category of finite length modules over ! op π Γ ππ , π = End π=π+1
i.e. the sum of the projective covers of the remaining irreducibles. If we remove the finite length assumption, then you get a special case of π
-Mod/(π β₯ ) Endπ
(π) op -Mod. Example 9.3: Let π
be a commutative ring, A = π
-Mod, πΌ β π
, and B be the modules where every element of πΌ acts locally nilpotently. Then A/B = QCoh(Spec(π
)\π πΌ ) where π πΌ is the zero set of πΌ . This is a quasiaffine scheme (not necessarily affine). You can also get (quasi)coherent sheaves on more general varieties using the Serre quotient. For example, a projective variety π over a field π can be obtained as Proj(π΄) for a positively graded commutative algebra π΄ with π΄0 = π. Then Coh(π ) is the Serre quotient gr
π΄-Modfg /π΄-Mod0 gr
where π΄-Modfg is the category of finitely generated graded modules and π΄-Mod0 is the subcategory of finitedimensional (equivalently, concentrated in finitely many degrees) modules. Geometrically, this corresponds to starting with dilation equivariant sheaves on the cone Spec(π΄) and throwing away the origin.
9.2
Adjoint functors and (co)limits
Definition 9.4: An adjunction for a pair of functors πΏ : C1 β C2 , π
: C2 β C1 is an isomorphism Hom C2 (πΏ(π ), π ) Hom C1 (π, π
(π )) that is functorial in π, π . Then we say that πΏ, π
are adjoint functors, that πΏ is the left adjoint of π
, and π
is the right adjoint of πΏ. The Yoneda Lemma indicates that πΏ determines π
up to unique isomorphism and vice versa (if it exists). Example 9.5: In general, free and forgetful functors are adjoint; for example, the functor sending a set π to the corresponding free structure (group, abelian group, module, algebra, etc.) on π is left adjoint to the forgetful functor to Set. Likewise, the functor sending a Lie algebra to its universal enveloping algebra π€ β π (π€) is left adjoint to the functor sending an associative algebra to itself but as a Lie algebra (with the Lie bracket [π₯, π¦] = π₯π¦ β π¦π₯). Example 9.6: It is possible for a functor to have a left adjoint but no right adjoint: for example, the full embedding of commutative rings into associative rings has a left adjoint sending π
to the quotient by the 2-sided ideal generated by the commutators. But it has no right adjoint. Example 9.7 (Tensor-Hom adjunction): Let π΄ ππ΅ be a bimodule. Then πΏ = π βπ΅ β : π΅-Mod β π΄-Mod is left adjoint to π
= Homπ΄ (π, β) : π΄-Mod β π΅-Mod.
26
Example 9.8: Consider the category Fun(D, C) of functors from D β C. The functor Cons : C β Fun(D, C), Cons(π ) (π ) = π, Cons(π ) = Idπ has right adjoint Consβ ; this may or may not exist, but if it does, Consβ (πΉ ) is the limit or inverse limit of πΉ . Likewise, the left adjoint β Cons, if it exists, sends πΉ to the colimit or direct limit of πΉ . We can describe the limit more concretely. Consβ (πΉ ) has the following property: it is the universal object equipped with compatible maps into πΉ (π), π β D. That is, given an object π with compatible maps into πΉ (π) for π β D, there is a unique map π β Consβ (πΉ ) that makes the diagram commute. Note that not all limits and colimits may exist in a category. Some examples of limits and colimits: the colimit of β’ β’ is the coproduct, while its limit is the product. The limit of β’ β β’ β β’ is the pullback, the colimit of β’ β β’ β β’ is the pushout.
9.3
Additive categories
We are interested in categories like π
-Mod that have additional structure. Definition 9.9: An additive category A is a category where each Hom set has the structure of an abelian group such that the composition is bilinear and the following properties hold: a) There exists an object 0 A such that Hom(0 A , 0 A ) = 0 (the zero group), b) For every π1, π2 β A, there exists an object π = π1 β π2 with morphisms ππ : π β ππ and ππ : ππ β π such that π 1π 2 = π 2π 1 = 0, π 1π 1 = idπ1 , π 2π 2 = idπ2 , and π 1 π 1 + π 2 π 2 = idπ . This implies that Hom(0, π) = Hom(π, 0) = 0, so 0 is both the initial and final object. Also, π is both the coproduct and product of π1, π2 : you can see this by noting that the corresponding fact is true for abelian groups, then apply this to Hom(π, π ) and Hom(π, π). Notice that we were able to deduce a global property (about Hom in every object) from a local property (only looking at π, π , π, 0). Note : We donβt need to include an addition on Hom sets in the definition. If we know that there is an initial and final object and that therefore, the resulting map from coproducts to products is an isomorphism, you can recover addition on Hom sets, as discussed in the category of modules. But itβs more convenient to list it in the definition.
9.4
Abelian categories
An abelian category is essentially a βcategory where you can do homological algebraβ and was introduced by Grothendieck.
27
Definition 9.10: An abelian category is an additive category satisfying β’ AB1: existence of kernel and cokernels: that is, objects representing the functor π β ker(Hom(π, π) β Hom(π, π )) and corepresenting the functor π β ker(Hom(π , π ) β Hom(π, π )) for a morphism π : π β π . Morphisms with zero kernel are monic and morphisms with zero cokernel are epic. β’ AB2: A monic morphism is a kernel; that is, for π : π β π , let πΎ = ker π and πΆ = coker π , then coker(πΎ β π) β ker(π β πΆ) is an isomorphism. One can also add the additional axioms β’ AB3: the existence of arbitrary coproducts β’ AB4: the coproduct of any family of monic morphisms is monic A subobject of π΄ is an object π΄π with a monic morphism π΄π β©β π΄. The sum of some subobjects π΄π is im ( The intersection of two subobjects π΄, π΅ of πΆ is ker(πΆ β πΆ/π΅ β πΆ/π΄). We can add one last axiom Γ Γ β’ AB5: ( π΄π ) β© π΅ = (π΄π β© π΅) for a collection of increasing subobjects π΄π in π΄.
Γ
π΄π β π΄).
We can also define AB3,4,5β : a category satisfies ABnβ if A op satisfies ABn. If a category satisfies AB1-5, itβs called a Grothendieck category. Definition 9.11: A category D is filtered if Ob(D) β β
and for all π, π β D, there exists π β D such that Hom(π, π), Hom(π, π) are nonempty and such that for every pair of parallel morphisms π, π : π β π, there exists π : π β π such that ππ = ππ . The key feature of Grothendieck categories is that filtered colimits exist and are exact. Remark 9.12: The category of π
-modules satisfies AB5, AB3β , and AB4β . Remark 9.13: The only abelian category satisfying AB3-5 and AB3β -5β is the zero category. Sketch of proof: consider an object π in such a category and let Ξ£, Ξ be the coproduct and product of countably many copies of π . There is a canonical map π : Ξ£ β Ξ ; it is monic because itβs the colimit of embeddings of a direct summand and epic since it is the inverse limit of surjections to a direct summand. Hence π is an isomorphism. Now π β1
consider the composition π of the arrows π β Ξ βββ Ξ£ β π where the first arrow is the diagonal and the second arrow is the codiagonal. Then one can check that π + idπ = idπ because ββ + 1 = ββ²β² . Hence idπ = 0 and π 0.
9.5
Compact projective generators and Serre quotients revisited
Definition 9.14: An object π is compact if Hom(π, β) commutes with filtered colimits. If π is projective, this follows from commuting with arbitrary direct sums, since ! Γ Γ colim(πΉ ) = coker πΉ (π) β πΉ (π) π : πβπ
π
where the morphism takes π₯ β¦β π₯ β πΉ (π) (π₯). In general, this is not true, though it is true that every compact module is finitely generated. Definition 9.15: An object π is a generator if π β¦β Hom(π,π ) is a faithful functor. For a projective object, this is equivalent to the Definition 7.4. Alternatively, we could say that if π β₯ is the full subcategory whose objects are π such that Hom(π, π) = 0, then a projective object π is a generator iff π β₯ {0}. Theorem 9.16: An abelian category with coproducts (satisfying AB3) and a projective compact generator is End(π) op -Mod where π is a projective compact generator.
28
The proof is the same as the proof in the Morita theory case. Corollary 9.17: Let π be a compact projective object in an AB3 abelian category A. Let B = π β₯ . Then A/B End(π) op -Mod. Proof (Sketch). Itβs clear that 1) π is projective in A/B (use the lower roof diagram Homs) and 2) π is a generator (in A/B). B is closed under coproducts, so the projection functor A β A/B commutes with coproducts. Hence π is compact in A/B. β‘ This proves the claim at the beginning of Section 8.3. References for this lecture include the original article [9], which still makes for excellent reading. Textbook expositions can be found in [13] and in the appendix to [18]. 10
10.1
March 14 - Exts and Tors, Resolutions
Ext and Tor
Definition 10.1: Let π, π be objects in an abelian category. Extπ (π, π ) is the derived functor of Hom. Recall that Hom is left exact in the second argument and right exact in the first argument, so you can take either the right derived functor of Hom(π, β) or the left derived functor of Hom(β, π ), and these are the same. Although the most useful formalism for this is the derived category, we can also work in a typical category. The key property of Ext is that it is the universal delta functor. Delta functors were introduced by Grothendieck in his Tohoku paper; essentially, they turn short exact sequences to long exact sequences. Given a short exact sequence 0 β πΏ β π β π β 0, a delta functor is a functorial family of (additive) functors π π with boundary morphisms πΏ0
πΏπ : π π (π ) β π π+1 (πΏ) such that 0 β π 0 (πΏ) β π 0 (π) β π 0 (π ) ββ π 1 (πΏ) β Β· Β· Β· β is exact. One can define morphisms of delta functors as families of natural transformations that commute with the boundary morphisms, and a delta functor is universal when giving a morphism to any other delta functor is equivalent to only giving the natural transformation in degree zero. To show that something is a universal functor, itβs enough to show that itβs βeffaceableβ (in the language of Grothendieck), meaning that every element π β Extπ (π, π ), π > 0 is killed by some injection π β©β π β² . To actually compute Ext, we use projective and injective resolutions. A projective resolution of π is an exact sequence Β· Β· Β· β π 2 β π1 β π β 0 where the ππ are projective; these always exist for π
-modules. Ext(π, π ) is computed by applying Hom(β, π ) to the resolution, removing π, and computing the cohomology of the resulting complex. You can also compute Ext using left injective resolutions of π , i.e. 0 β π β πΌ 1 β Β· Β· Β· β where πΌπ are injective. Then, in this case, itβs easy to see that Ext is effaceable β every π has an injection into an injective πΌ , and every π receives a surjection from a projective π, so these maps efface all elements in Extπ , π > 0 because Extπ (π, π ) = Extπ (π, πΌ ) = 0 for π > 0. A better formal setting for this is the homotopy category of complexes H β(π
). The morphisms in this category are follows: for πΆ 1, πΆ 2 complexes in π
-Mod, let Homβ’ (πΆ 1, πΆ 2 ) be the complex where Homπ (πΆ 1, πΆ 2 ) = Γ definedπ as π+π β’ β’ 0 π Hom(πΆ 1, πΆ 2 ) and define Hom Hβ(π
) (πΆ 1, πΆ 2 ) := π» (Hom (πΆ 1, πΆ 2 )). Hom has a differential, which is to take the supercommutator with π. That is, it consists of maps π : πΆ 1 β πΆ 2 that commute with π modulo the equivalence that π βΌ π if π β π = ππΆ2 β + βππΆ1 where β : πΆ 1π β πΆ 2π+1 is any collection of maps. Exercise : There is a full embedding π
-Mod β H β(π
) taking π β¦β ππ , a projective resolution of π, which is unique up to unique isomorphism in H β(π
). (That is, projective resolutions are βunique up to homotopyβ). Let H β0 (π
) be category of complexes of projectives in nonpositive degree with π» π = 0, π < 0 (so they are exact outside of degree 0). Then there is an equivalence H β0 (π
) β π
-Mod taking πΆ β¦β π» 0 (πΆ).
29
Remark 10.2: π is projective iff Ext1 (π, π ) = 0 for all π . If π is projective, it has projective resolution 0 β π β π β 0. If Ext1 (π, π ) = 0, then 0 β π β π β π β 0 has a splitting for all π (either use the definition that Ext1 is extensions or the long exact sequence), so π is projective.
10.2
Projective, injective, and homological dimension
Definition 10.3: The projective dimension of a module π is max π | βπ s.t. Extπ (π, π ) β 0 β Zβ©Ύ0 βͺ {β}. If 0 β π β² β π β π β 0, pdim(π) = pdim(π β² ) + 1 unless π is projective. This is because for π β©Ύ 1, the LES says 0 β Extπ (π β², π ) β Extπ+1 (π, π ) β 0. Alternately, we can define projective dimension as the length of the minimal projective resolution. For example, if pdim(π) = 1, that means 0 β π β π β π β 0 is a resolution of π. Definition 10.4: The injective dimension of a module π is n o max π | βπ s.t. Extπ (π, π ) β 0 or the length of the minimal injective resolution. Definition 10.5: The homological dimension of a ring π
is the maximal projective dimension of an π
-module, which is the same as the maximal injective dimension of an π
-module. It is also n o max π | βπ, π s.t. Extπ (π, π ) β 0 . Remark 10.6: π is injective iff Ext1 (π, π ) = 0 for all cyclic π. Proof. Weβll show that if 0 β π β² β©β π, π β² β π , we can extend this to a map π β π . By Zornβs Lemma, it suffices to show that it can be extended to some π β²β² β π with π β² β π β²β² . Pick π β π \ π β² and let π β²β² be the submodule generated by π β², π. We have an exact sequence 0 β π β π β²β² β π β²β² /π β² β 0 and by construction π β²β² /π β² is cyclic. Hence, if Ext1 (π β²β² /π β², π ) = 0, there exists an extension of π β² β π to π β²β² β π . β‘ This remark implies that n o hdim(π
) = max π | Extπ (π, π ) β 0 for some π, π s.t. π is f.g. . Example 10.7: If π
is left Noetherian, a finitely generated π has a resolution of finitely generated projectives. Then Extπ (π, β) commutes with filtered colimits. Hence, we can assume that π is also finitely generated in the above definition of homological dimension. If π
is Artinian, we can say more: it suffices to consider only irreducible π, π .
10.3
Cartan matrices
In this section suppose that π
is Artinian and π
-Mod refers only to finitely generated modules. If π
has finite homological dimension, then πΎ 0 (π
-Mod) (Definition 3.17) is generated by classes Γ of projective modules: for every simple, write a projective resolution 0 β ππΏπ β Β· Β· Β· β ππΏ0 β πΏ β 0, then [πΏ] = (β1)π ππΏπ . Definition 10.8: Let πΏ1, . . . , πΏπ be the irreducibles for a ring π
, and π1, . . . , ππ be their projective covers. The Cartan matrix of π
is the π Γ π matrix with πΆπ π = [π π : πΏπ ], the multiplicity of πΏπ in π π . If π
is finite-dimensional over an algebraically closed field, we can also say that πΆπ π = dimπ Hom(ππ , π π ).
30
We then get an identification πΎ 0 (π
-Mod) Zπ via [π] β¦β ( [π : πΏ1 ], . . . , [π : πΏπ ]). Hence, if π
has finite homological dimension, πΆ β GLπ (Z); the π πth entry of πΆ β1 is n o βοΈ (β1)π # summands of ππΏππ isomorphic to π π . π
Corollary 10.9: If π = 1, π
has finite homological dimension iff π
= Matπ (π·) for a skew field π·. Now let π
be Artinian and π a finitely generated module. Lemma 10.10: Let Β· Β· Β· βββ π β1 βββ π 0 β π β 0 be a projective resolution and set πΆ π = ker(ππ ) = im(ππ β1 ). Then TFAE: π βπ β1 a) π βπ β1 βββββ πΆ βπ is a projective cover for every π. b) πΏ βπ
π β’ has 0 differential for all irreducible right π
-modules πΏ. c) Homπ
(π β’, πΏ) has 0 differential for all irreducible πΏ. Resolutions satisfying these properties are minimal. From π), if it exists, it is unique up to non-unique isomorphism because projective covers are unique. From π), we see that in the minimal resolution, π β2
π β1
π βπ =
Γ
ππ
πππ
ππ π , Extπ (π, πΏπ ) = π·π
π
where πππ = dimπ·π (Extπ (π, πΏπ )). Proof. π β π is a projective cover iff it induces an isomorphism Hom(π, πΏ) β Hom(π, πΏ) for all irreducibles πΏ. First, π β π iff Hom(π, πΏ) β©β Hom(π, πΏ) for all irreducibles πΏ. If π β π, then by applying Hom(β, πΏ), which is left exact, we see that Hom(π, πΏ) β©β Hom(π, πΏ). If the map π β π is not onto, then coker(π β π) is nonzero finitely generated, so it has irreducible quotient πΏ. Then π β πΏ is in the kernel of Hom(π, πΏ) β Hom(π, πΏ), so this map is not injective. If π β π is a projective cover, and there exists π β πΏ that doesnβt come from some π β πΏ, then ker(π β πΏ) β π, so the surjection is not essential, a contradiction. If π β π is not a projective cover, then there exists π β©β π with π β π. Then π/π has a simple quotient πΏ, and the map π β π/π β πΏ cannot come from a map π β πΏ: if it did, then π β π β πΏ should pull back to π β π β πΏ, but this is the zero map because itβs also the composition π β©β π β π/π β πΏ, which is zero. Hence Hom(π, πΏ) β Hom(π, πΏ) is not surjective. By definition 0 β π βπ β1 β π βπ β πΆ βπ+1 β 0. If π βπ β πΆ βπ+1 is a projective cover, then Hom(πΆ βπ+1, πΏ) Hom(π βπ , πΏ), iff Hom(π βπ , πΏ) Hom(π βπ+1, πΏ). β‘ Remark 10.11: This generalizes to Zβ©Ύ0 -graded rings where π΄0 is Artinian and π΄π is finitely generated over π΄0 . A common setting where this appears is an algebra π΄ over an algebraically closed field π where π΄0 is semisimple and π΄π is finite-dimensional over π. In this setting, there are still indecomposable projectives. In minimal resolutions, each term has finitely many generators in each degree.ΓThe graded irreducibles are concentrated in one degree (use that if π is a graded π΄-module, then πβ©Ύπ := π β©Ύπ ππ β π is a π΄-submodule of π for any π β Z). It follows that graded irreducible π΄-modules are annihilated by π΄ β©Ύ1 so they are just irreducible π΄0 -modules (up to a shift of grading). Γ If π΄0 = π is just a field, and for finitely generated (graded) π, we can consider its Poincare series π dim(ππ )π‘ π β Γ Z((π‘)). More generally, if π΄0 is semisimple then one can consider series ππ := π [ππ ]π‘ π β Z((π‘))π where π is the number of irreducibles for π΄0 and [ππ ] β πΎ 0 (π΄0 -Mod) Zπ . The Cartan matrix πΆ now lies in GLπ (Z[[π‘]]) instead of Matπ (Z) (it is clear that πΆ β Matπ (Z[[π‘]]) and πΆ (0) = Id since π΄0 is semisimple, it then follows that πΆ β GLπ (Z[[π‘]])). If πΏπ has finite homological dimension, and π΄ is Noetherian then πΆ β1 β Matπ (Z[π‘]). For example, considered as a graded algebra with deg π₯ = 1, then π = 1, πΏ1 = π, π1 = π [π₯], so Γβ π if1π΄ = π [π₯], πΆ = π=0 π‘ = 1βπ‘ , and πΆ β1 = 1 β π‘.
31
11
11.1
March 16 - Koszul complexes
More on the Hattori-Stallings Dennis trace
Recall from Lemma 8.5 that the cocenter π
/[π
, π
] = πΆ (π
) receives a universal trace map π (π, π) β πΆ (π
) where π is a finitely generated projective and π β End(π). In fact, if π
is Noetherian and of finite homological dimension, you can extend π to π (π, π) where π is any finitely generated module. To do so, choose a finite projective resolution 0 β π βπ β π βπ+1 β Β· Β· Β· β π 0 β π β 0 (which exists because π
has finite homological dimension). Then we can β’ ) and this will be unique up to homotopy. Define lift π to πΛ β End(ππ βοΈ (β1)π π (π βπ , πΛ βπ ) π (π, π) = π
which is well-defined because π β¦β is a fully faithful functor to the homotopy category of complexes. Moreover, π is additive on short exact sequences of modules. β’ ππ
Corollary 11.1: If π
is a finite-dimensional algebra of finite homological dimension over an algebraically closed field π, then π½ (π
) β [π
, π
]. Proof. Lemma 11.2: For π β π
-Mod and π β Endπ
(π), we can find a π-invariant Jordan-Holder series of π. Γ ππ Proof. Consider π | Soc(π ) : Soc(π) β Soc(π), where Soc(π) = π πΏπ is the socle of π. Then π induces an π
-linear map πΏπππ β πΏπππ i.e. an element of Endπ
(πΏπππ ) = Matππ (π) (use Schurβs lemma) and this matrix has an eigenvector, which generates a π-invariant irreducible submodule in π. Then by inducting on the length of π, we get a π-invariant Jordan-Holder series. β‘ Γ Γ Thus, π (π, π) = π π (πΏπ , ππ ) = π ππ π (πΏπ , 1) where ππ β π. It follows that the elements π (πΏπ , 1) β πΆ (π
) generate πΆ (π
) as a vector space over π (use Lemma 8.5 or Example 8.6). We conclude that πΆ (π
) has dimension (over π) at Β― Itβs easy to most the number of irreducibles πΏπ . On the other hand, let π
Β― := π
/π½ (π
) and note that πΆ (π
) β πΆ (π
). Β― = π #πΏπ , so πΆ (π
) πΆ (π
) Β― and π½ (π
) β [π
, π
]. see that πΆ (π
) β‘ Question : Is there a way to prove this without using the trace map?
11.2
Minimal resolutions and Koszul rings
Given a module π, how can we find its minimal resolution? For certain algebras called Koszul algebras, their minimal resolutions are called Koszul complexes. One great reference is [5, Section 2]. Let π΄ be a nonnegatively graded algebra over an algebraically closed field π with π΄0 semisimple. We will be interested in the case π΄0 = π so we can write π΄ = π β π΄ >0 . Γ Remark 11.3: An elementary property of minimal resolutions for graded modules is that if π = π β©Ύ0 ππ , then π βπ must be concentrated in degrees π and higher, since the projective cover π β π is an isomorphism in the bottom degree (use that π΄0 = π is semisimple). We will need the following technical lemma. Lemma 11.4: Let π be a finitely generated graded module over π΄. Then the following properties are equivalent: (i) π is generated by degree π elements, (ii) π βπ΄ π is concentrated in degree π, (iii) Homπ΄ (π, π) is concentrated in degree βπ. Proof. Lemma follows from the Nakayama lemma together with the fact that Homπ΄ (π, π) = Homπ΄0 (π/π΄ >0 π, π) = (π/π΄ >0 π) β . 32
β‘ Definition 11.5: We say that π΄ is Koszul if π βπ is generated by degree π elements. Equivalently, Torππ΄ (π, π) (where each of the π are in degree 0) is concentrated in degree π, which is equivalent to Extππ΄ (π, π) is concentrated in degree βπ (use Lemma 11.2 above). Theorem 11.6: a) Koszul rings are quadratic, i.e. π΄ = π (π )/β¨πΌ β©, where π (π ) is the tensor algebra for a vector space π and πΌ is a subspace of π β π . b) If π΄ is Koszul, then Extπ΄β’ (π, π) = π΄! , where π΄! is the dual quadratic algebra π (π β )/β¨πΌ β₯ β©. Example 11.7: Let π΄ = π (π ), so πΌ = 0. Then the dual quadratic algebra is π΄! = π (π β )/β¨π β β π β β© = π β π β . Hence Extπ΄ (π, π) is only nonzero in degrees 0 and 1. π = π (π )/β¨π β© then has a free resolution in degrees 0 and 1. Example 11.8: Let π΄ = Sym(π ) = π (π )/β¨β§2π β©. Then π΄! = π (π β )/β¨Sym2 (π β )β© = Definition 11.9: The πth Veronese subalgebra π΄ (π ) is
Γβ’
π β.
Γβ
π=0 π΄ππ .
Let us mention the following theorem without a proof (see [3] for details). Theorem 11.10: If π΄ is a finitely generated commutative algebra, π΄ (π ) is Koszul for large π. Remark 11.11: Using the approach of [6, Section 2] or [16] (see also Remark 12.2 below) one can easily prove (using Serreβs vanishing theorem) that for every π β Zβ©Ύ0 and large enough π (depending on π) the algebra π΄ (π ) has the following property: π βπ is generated by degree π elements for π β©½ π. The statement of Theorem 11.10 is stronger, and the proof is more involved.
11.3
Koszul complexes
Remark 11.12: Assume π΄ = π (π )/β¨πΌ β© is quadratic. Then π
π΄π = π (π )/β¨πΌ β©π = π
βπ
/
πβ2 βοΈ
! π
βπ
βπΌ βπ
βπβπ β2
.
π=0
Define π
π :=
πβ2 Γ
π βπ β πΌ β π βπβπ β2
π=0
to be the intersection rather than the sum. Then π
π = (π΄π! ) β , π
πβ
=π
ββπ
/
πβ2 βοΈ
! β βπ
(π )
β₯
β βπβπ β2
β πΌ β (π )
= π΄π! .
(1)
π=0
Definition 11.13: The Koszul complex, Kβ’ , is a complex of free π΄-modules Β· Β· Β· β π΄ βπ π
2 β π΄ βπ π
1 β Γβ denoted β’ β’ β’ π΄. As (graded) vector spaces, K = π=0 Kπ . The differential of Kπ is given by: Kππ βπ = π΄π β π
πβπ β©β π΄π β π β π
πβπ β1 β π΄π+1 β π
πβπ β1 = Kππ+1βπ where the left map is induced by the natural embedding π
πβπ β π β π
πβπ β1 and the right map is induced by the multiplication π΄π β π β π΄π+1 .
33
Definition 11.14: Let π be a vector space. A distributive lattice of subspaces of π is a collection of subspaces satisfying β’ For π in the lattice, π β π is also in the lattice β’ For π, π in the lattice, π + π is also in the lattice β’ For π, π, π in the lattice, π β© (π + π ) = (π β© π ) + (π β© π ) (distributivity). Theorem 11.15 (Theorem 11.6 cont.): a) Koszul rings are quadratic, i.e. π΄ = π (π )/β¨πΌ β©, where π (π ) is the tensor algebra for a vector space π and πΌ is a subspace of π β π . b) If π΄ is Koszul, then Extπ΄β’ (π, π) = π΄! , where π΄! is the dual quadratic algebra π (π β )/β¨πΌ β₯ β©. c) Say π΄ is a quadratic algebra. It is Koszul iff K is exact, i.e. π» π (K) = 0 for all π β 0, iff K is the minimal resolution of the left module π. d) Say π΄ is a quadratic algebra. It is Koszul iff for all π, the π β1 vector spaces π βπ βπΌ βπ βπβπ β2 , π = 0, . . . , π β2, generate a distributive lattice of subspaces of π βπ . Lemma 11.16: A collection of vector subspaces in a vector space π generate a distributive lattice iff there exists a basis of π such that every subspace is spanned by a subset of the basis. Proof. Clear.
β‘
Remark 11.17: The distributive property for the subspaces of π βπ described above is what implies the exactness of Kπ . Moreover, the exactness of Kπ , π β©½ π, implies the distributive property for the subspaces of π βπ . βπ For a collection W = (π ;π1, . . . ,ππ ), where Γ π isa vector space and π1, . . . ,ππ β π are its subspaces let πΎ = Γ π β1 π β1 πΎ βπ (W) := π=1 ππ / (ππ+1 + . . . + ππ ) β© π=1 ππ , where π = 0, 1, . . . , π + 1.
For example, we have πΎ
βπβ1
=
π Γ π=1
ππ , πΎ
βπ
=
πβ1 Γ π=1
ππ , πΎ
βπ+1
=
πβ2 Γ
ππ / ππ β©
π=1
π Γ
!! ππ
, . . . , πΎ β1 = π /
π=3
π βοΈ π=2
ππ , πΎ 0 = π /
π βοΈ
ππ .
π=1
We have the natural maps πΎ π β πΎ π+1 that make πΎ β’ = πΎ β’ (W) into a complex. Lemma 11.18: If π1, . . . ,ππ β π are proper subspaces and every proper subset of {π1, . . . ,ππ } generate a distributive lattice then π1, . . . ,ππ do the same iff πΎ β’ (W) is exact. Proof. It is clear that if {π1, . . . ,ππ } generate a distributive lattice then πΎ β’ (W) is exact (for example, use Lemma 11.16). Assume now that πΎ β’ (W) is exact. We prove the claim by the induction on π. We follow [4, Section 4.5]. We will use the following notations. Given a collection π 1, . . . , ππ β π , say that a subspace π΅ β π is a splitting for (π ; π 1, . . . , ππ ) if there exists πΆ β π such that π΅ β πΆ = π and (π΅ β© ππ ) + (πΆ β© ππ ) = ππ . We will say that (π ; π 1, . . . , ππ ) is indecomposable if π has no proper nonzero subspaces that split (π ; π 1, . . . , ππ ). The following easy facts will be extremely useful. Fact (1): The subspace π 1 β© . . . β© ππ or π 1 + . . . + ππ is a splitting for (π ; π 1, . . . , ππ ) iff it is a splitting for (π ; ππ+1, . . . , ππ ). Proof. Clear.
β‘
Fact (2): Assume that (π 1 + . . . + ππ ) β© (ππ+1 β© . . . β© π π ) = 0 and ππ+1 β© . . . β© π π is a splitting for (π ; π 1 + . . . + ππ , π π+1, . . . , ππ ). Then ππ+1 β© . . . β© π π is a splitting for (π ; π 1, . . . , ππ ).
34
Proof. Let (ππ+1 β© . . . β© π π ) β π΅ be a splitting for (π ; π 1 + . . . + ππ , π π+1, . . . , ππ ). Our goal is to check that it also gives a splitting for (π ; π 1, . . . , ππ ). From (π 1 + . . . +ππ ) β© (ππ+1 β© . . . β©π π ) = 0 we conclude that π 1 + . . . +ππ β π΅ so π 1, . . . , ππ β π΅. It remains to check that ππ = (ππ β© (ππ+1 β© . . . β© π π )) + (ππ β© π΅) for π = π + 1, . . . , π. This is clear since ππ+1 β© . . . β© π π β ππ . β‘ Fact (2β): Assume that (π 1 β© . . . β© ππ ) β© (ππ+1 + . . . + π π ) = 0 and π 1 β© . . . β© ππ is a splitting for (π ; ππ+1 + . . . + π π , π π+1, . . . , ππ ). Then π 1 β© . . . β© ππ is a splitting for (π ; π 1, . . . , ππ ). Proof. Same proof as the one of Fact 2.
β‘
Let us now return to the proof. Without losing the generality, we can assume that W = (π ;π1, . . . ,ππ ) is indecomposable and all ππ are nonzero (and proper). It then follows (use that by the inductive assumption, π1 β© π2,π3, . . . ,ππ β π , π1, . . . ,ππβ2,ππβ1 + ππ β π form distributive lattices and then apply Fact 1) that: π1 β© π2 = 0, ππβ1 + ππ = π .
(2)
We can assume that π β©Ύ 4 (for π = 3 the statement is clear, use exactness of πΎ β’ (W)). Assume that π = 4. We have π1 β© π3 β© π4 = 0 = π2 β© π3 β© π4 (use Fact 1). We also have (π1 +π2 ) β©π3 β©π4 = ((π1 +π2 ) β©π3 ) β© ((π1 +π2 ) β©π4 ) = ((π1 β©π3 ) + (π2 β©π3 )) β© ((π1 β©π4 ) + (π2 β©π4 )). We claim that the intersection ((π1 β© π3 ) + (π2 β© π3 )) β© ((π1 β© π4 ) + (π2 β© π4 )) is zero. Indeed, if π + π = π + π for some π β π1 β© π3 , π β π2 β© π3 , π β π1 β© π4 , π β π2 β© π4 then π β π = π β π must lie in π1 β© π2 = 0 i.e. π = π β π1 β©π3 β©π4 = 0, π = π β π2 β©π3 β©π4 = 0 so π = π = π = π = 0. We conclude that (π1 +π2 ) β©π3 β©π4 = 0. It then follows from Fact 2 that π3 β©π4 splits (π ;π1,π2,π3,π4 ) so we must have π3 β©π4 = 0 i.e. π = π3 β π4 . It remains to note that π = π3 βπ4 is splitting for (π ;π1,π2,π3,π4 ), and a contradiction finishes the argument. If π > 4. The propperty (2) implies that (π ;π1, . . . ,ππ ) remains acyclic after arbitrary transpositions of π1, . . . ,ππβ2 (by acyclic, we mean that the corresponding complex πΎ β’ is exact, it will be equal to zero in this case). So we may assume that for certain 1 β©½ π β©½ π β 3 one has π΄ = π1 β© . . . β© ππ β 0 and each π + 1-tuple from π1, . . . ,ππβ2 intersects by zero. Put π΅ = ππ+1 + . . . + ππβ2 . Then (π ; π΄; π΅;ππβ1,ππ ) satisfies the assumptions of Lemma 11.18 (acyclicity follows from the fact that π΄ β© π΅ = 0 and ππβ1 + ππ = π ) so (from π = 4 case) we conclude that π΄; π΅;ππβ1,ππ β π generate a distributive lattice so π΄ is a splitting for (π ;π1, . . . ,ππ ) by Fact 2β² . Since π΄ β 0, we get a contradiction. β‘ Proof (of Theorem 11.15). If Tor1 (π, π) is concentrated in degree 1, then π΄ β©Ύ1 is generated by degree 1 elements as an π΄-module (use the exact sequence 0 β π΄ β©Ύ1 β π΄ β π β 0 together with Nakayama). Hence, π΄ is generated by degree 1 elements as a ring. Let π = π΄1 and write π΄ = π (π )/πΌ . We have a map π΄ β π β π΄. Using that Tor2 (π, π) is concentrated in degree 2, we see that ker(π΄ βπ β π΄) is generated by elements in π΄1 βπ = π βπ . These elements considered as elements of π β π β π (π ) generated the ideal ker(π (π ) β π΄), so π΄ is quadratic. Exactness of Koszul complex implies Koszul: If Kπ is exact for π β©Ύ 1, then K is a free resolution of π as an 0
β π΄-module. So now we can use it to compute Extπ΄β’ (π, π). Since π
πβ β β π
πβ1 and π
πβ = π΄π! , Extππ΄ (π, π) = π΄π! . You also have to check that this is compatible with multiplication, but after showing that, we can deduce that π΄ is Koszul. To be continued next lecture. β‘
12 March 21 - Koszul rings cont., bar complex
12.1
Finishing up Koszul rings
Proof (of Theorem 11.15, cont.) Subspaces π βπ β πΌ β π βπβπ β2 β π βπ , π = 0, 1, . . . , π β 2 generate a distributive lattice iff Kπβ’ is exact: to see that it is enough to note that Kπβ’ = πΎ β’ (W) for W = (π βπ ; π βπβ2 β πΌ, π βπβ3 β πΌ β π , . . . , π βπβπ β1 β πΌ β π βπ β1, . . . , πΌ β π βπβ2 ). Now the claim follows from Lemma 11.18 (using induction on π). 35
Itβs easy to see that Kπ acyclic implies that K is a resolution for the trivial module, and Torππ΄ (π, π) is concentrated in degree π, so π΄ is Koszul. In the other direction, suppose π΄ is Koszul. We will inductively check acyclicity in the first π terms of the complex, which looks like Β· Β· Β· β π΄ β πΌ β π΄ β π β π΄. If this complex is exact up to degree π΄ π, then the minimal space of generators for ker(π΄ β π
π β π΄ β π
π β1 ) is (some lift of) Torπ+1 (π, π). Because π΄ is Koszul, this is in degree π + 1, so itβs a subspace in π΄1 β π
π = π β π
π . It is the kernel of the multiplication map, so it must be π
π+1 , so weβre done. β‘ Remark 12.1: In commutative algebra, a βKoszul complexβ often refers to a complex formed given a comβπ β π
, sending mutative ring Γππ
and π elements π₯ 1, . . . , π₯π β π
. The last arrow in the complex is π
π 1, . . . , ππ β¦β π=1 π₯π ππ . The Koszul complex for Sym(π ) is an example of this. Remark 12.2: We are now ready to give a sketch of the proof of the fact that for every π β Zβ©Ύ0 , and large enough π, the algebra π΄ (π ) has the following property: π βπ is generated by degree π elements for π β©½ π (see Remark 11.11 above). So, our goal is to check that for every π β Zβ©Ύ0 the degree πth term of the Koszul complex for π΄ (π ) is exact for large enough π. First of all, we can assume that π΄ is generated by π΄1 = π . Set π := Proj π΄. We can assume that the natural morphism π β©β Pπ is a closed embedding. We have a natural (very ample) line bundle Oπ (1) on π with Ξ(π, Oπ (1)) = π΄1 = π . Set π := π π , L := Oπ (1) β π . For a closed π β π we have π» 0 (π , L) = π βπ and denote by π π β π βπ the kernel of π» 0 (π , L) β π» 0 (π, L). Let Ξπ β π π be the diagonal given by π₯π = π₯π+1 . We have π Ξπ+1 = π βπ β πΌ β π βπβπ β2 . Let π π be the (finite) set of closed subschemes of π generated by {Ξπ | π = 1, . . . , π β 1} and π π , β
via unions and (scheme-theoretic) intersections. Using Serreβs vanishing theorem, we can assume that the statements of [6, Corollary 1.7] are satisfied for π π . It then follows from [6, Lemma 2.1] that subspaces π βπ β πΌ β π βπβπ β2 generate a distributive lattice of subspaces of π βπ so we are done by (the proof of) Theorem 11.15 (π). Corollary 12.3: The Poincare series of a graded algebra is βοΈ ππ΄ (π‘) = ππ π‘ π , ππ = dim π΄π . If π΄ is Koszul, then ππ΄ (π‘)ππ΄! (βπ‘) = 1. Proof. This follows from the (graded) Euler characteristic of K. If you look degree by degree, you can find that the Euler characteristic of Kπ is the πth coefficient of ππ΄ (π‘)ππ΄! (βπ‘) (see (1)) so the total Euler characteristic of K is equal to ππ΄ (π‘)ππ΄! (βπ‘). Recall now that the Euler characteristic of Kπ can also be computed as the alternating sum of dimensions of the cohomology of Kπ . It remains to note that Kπ is exact for π > 0 and K0 = π (sitting in degree 0). It follows that the total graded Euler characteristic of K is equal to 1. β‘ Example 12.4: Let π΄ =
Γπ
π . Then ππ΄ (π‘) = (1 + π‘)π . Likewise, πSym(π ) =
1 (1βπ‘ ) π .
Proof (of Theorem 11.15, cont. again). Finally, we need to check that π΄! β Extπ΄β’ (π, π) is an algebra isomorphism. First, we explain how to make Extβ’ into an algebra: Extπ΄β’ (π, π) = π» β (Hom(π β’, π β’ )) for a projective resolution π β’ ; Hom is a DGA. Here is how π΄! acts on K: start with the action of π (π β ) on π (π ) by contracting tensors π ββπ Γ π βπ β π βπβπ . Restrict this to π ββπ Γ π
π β π
πβπ , which factors through π΄π! Γ π
π . Recall that K βπ = π΄ β π
π . Consider the map (π΄ β π
π ) β π΄π! β π΄ β π
πβπ = K β (πβπ ) . β Kβπ This is the π΄! -action, and it commutes with the differential. Moreover, for π β π΄! , the composition K β represents the class of π. Hence, this is an algebra isomorphism. β‘ π
36
Remark 12.5: Let Projπ΄ be the projective graded π΄-modules. Then π΄! gives us an equivalence of derived categories π .π. π .π. H β(Projπ΄ ) β H β(Projπ΄! ) sending π (1) β¦β π [1] (β1) where π (1)π = ππ+1 and [Β·] is some homological stuff we wonβt discuss here. The idea is to use π as a generator for the derived category and consider the functor πΉπ : π β RHom(π, π) which generalizes πΉπ (π) = Hom(π, π). Remark 12.6: Let π΄1, π΄2 quadratic, π΄π = π (ππ )/πΌπ . Then π΄1 β π΄2 = π (π1 β π2 )/πΌ 1 β πΌ 2 β β¨π£ 1 β π£ 2 β π£ 2 β π£ 1 β© and
(π΄1 β π΄2 ) ! = π (π1β β π2β )/πΌ 1β₯ β πΌ 2β₯ + β¨π£ 1 β π£ 2 + π£ 2 β π£ 1 β©,
the βsuperβ (signed) tensor product. Remark 12.7: If π΄ is commutative and πΌ β β§2 (π ), then πΌ β₯ β π 2π β . Then all the relations of π΄! will be relations between anticommutators and π΄! will be the enveloping algebra of a Lie superalgebra. For more on Koszul rings, see [4] and [5].
12.2
Bar complex and Hochschild (co)homology
Definition 12.8: Let π΄ be any algebra over a field π. Then the bar complex of A is Β· Β· Β· β π΄ βπ π΄ βπ π΄ β π΄ βπ π΄ β π΄ β 0 where the last map is π β π β¦β ππ and in general π : π 0 β Β· Β· Β· β ππ β¦β π 0π 1 β π 2 β Β· Β· Β· β ππ β π 0 β π 1π 2 β Β· Β· Β· β ππ + Β· Β· Β· . The RHS is also written as π 0 |π 1 | Β· Β· Β· |ππ . Then π 2 = 0. Lemma 12.9: The bar complex is exact for any associative algebra. Proof. The map β : π 0 β Β· Β· Β· β ππ β¦β 1 β π 0 β Β· Β· Β· β ππ satisfies πβ + βπ = id, so it is a chain homotopy.
β‘
The bar complex is also a complex of π΄-bimodules. The left action is on π 0 , and the right action is on ππ . π΄ is the regular π΄-bimodule (i.e., π΄ βπ π΄op -module), and all the other terms are free, so the bar complex is a free resolution op for π΄. This allows us to compute Extππ΄βπ΄op (π΄, π΄) and Torππ΄βπ΄ (π΄, π΄). The bar complex also gives us a free resolution of every π΄-module by tensoring with π. The cohomology of the bar complex is Torππ΄ (π΄, π) = 0 for π > 0. Definition 12.10: The Hochschild homology of π΄ is the homology of the bar resolution. The Hochschild cohomology of π΄ is the cohomology of Hom(Bar, π΄), so the πth term is π΄ β (π΄ βπβ1 ) β . If π΄ is graded, you can likewise define graded Hochschild cohomology. Remark 12.11: If π΄ is augmented, you can use the reduced bar complex; let π΄+ be the augmentation ideal, the reduced bar complex has terms π΄ βπ π΄+ βπ . . . βπ π΄+ βπ π΄. This allows you to compute Extππ΄ (π, π) and Torππ΄ (π, π), and indeed π΄! is in the bottom degree.
37
13
13.1
March 23 - Hochschild (co)homology cont., central simple algebras
Deformations and Hochschild cohomology
From the definition of Hochschild (co)homology, we see that HH0 = πΆ (π΄) = π΄/[π΄, π΄] the cocenter and HH0 = Homπ΄βπ΄op (π΄, π΄) = π (π΄) the center. We also have a nice description for HH1 : the kernel of π is {π : π΄ β π΄ | π (ππ) = π (π)π + ππ (π)} and the image of π is {π | βπ₯ s.t. π (π) = [π, π₯]}. So HH1 is the derivations modulo the inner derivations, i.e., the outer derivations of π΄. Lemma 13.1: HH2 (π΄) is in bijection with isomorphism classes of first order deformations of π΄. Definition 13.2: An πth order deformation of π΄ is an algebra π΄Λ free over π [π‘]/(π‘ π+1 ) and an isomorphism Λ π΄Λ = π΄. A formal deformation of π΄ is the same as above, but over π [[π‘]] (and we need to use flatness instead π΄/π‘ of free), and a polynomial deformation of π΄ is the one over π [π‘]. Proof. Suppose π΄Λ is a first order deformation of π΄ and fix an isomorphism π΄Λ β π΄ βπ (π [π‘]/(π‘ 2 )). The multiplication π on π΄Λ will correspond to a cocycle: it is determined by π (π, π) for π, π β π΄, and we must have π (π, π) = ππ modulo π‘, so we can say that π (π, π) = ππ + π (π, π)π‘ where π : π΄ β π΄ β π΄. Then associativity of π corresponds to π being a cochain since we need ππ (π, π) β π (ππ, π) + π (π, ππ) β π (π, π)π = 0. Given any cocycle, we can define a deformation of π΄ by defining multiplication on π΄ β π [π‘]/π‘ 2 to be ππ + π (π, π)π‘. fπ β π π΄ f An isomorphism of deformations π΄ π is a map π : πΛ β¦β πΛ + π‘ π (π) for π : π΄ β π΄, since again it only depends on the values it takes on π΄. π is an algebra homomorphism iff (π β π) (π, π) = ππ (π) β π (π)π, that is, if π β π is a coboundary.
β‘
Remark 13.3: Given an πth order deformation, the obstruction to extending it to an π + 1th order deformation lies in HH3 (π΄); an expression in terms of the multiplication on π΄Λ must vanish in HH3 . Hence, if HH3 (π΄) = 0, any deformation can be extended, and the set of all such extensions is in bijection with HH2 . However, this bijection is not canonical. Exercise: to get a canonical bijection, you also need the data of a torsor over HH2 . Example 13.4: What is HHβ’ (π΄) and HHβ’ (π΄) for π΄ = π [π₯ 1, . . . , π₯π ] = Sym(π )? For simplicity, assume char π = 0. We see we need to compute Extβ’Sym(π βπ ) (Sym(π ), Sym(π )) and already know how to do this: change coordinates using the Koszul complex to find that itβs Sym(π ) β Γ we (π β ). In particular, we remarked above that HH1 is the outer derivations. For a commutative ring, there are no inner derivations, so HH1 (π΄) is exactly the derivations of Sym(π ), which are ( π ) βοΈ ππ . ππ ππ₯π , ππ β π [π₯ 1, . . . , π₯π ], ππ₯π : π β ππ₯ π π=1 Hence, HHβ’ (π΄) is the polyvector fields on π β = Spec(Sym(π )) and HHβ’ (π΄) β Sym(π ) β β1. These are the differential forms on π , Ξ©π is in degree βπ.
38
Γ
π,
Γ
π is in degree
Remark 13.5: Hochschild-Kostant-Rosenberg generalized this to a smooth algebraic variety π . HHβ’ and HHβ’ carry more structure, related to differential geometry: the de Rham differential on forms corresponds to the Connes differential, which corresponds to cyclic cohomology. The latter uses the fact that the differential in the bar complex has cyclic symmetry. The polyvector fields have a Schouten bracket, extending the commutator of vector fields [π£, π€] = Lieπ£ (π€) (the Lie derivative). This generalizes to HHβ’ (π΄), e.g. the obstruction in HH3 for extending the 1st order deformation is [β, β] where β is the deformation class.
13.2
Cobar complex and π΄!
Γ Let π΄ be an augmented algebra, π΄ = π Β· 1 β π΄+ , π΄+ = πβ©Ύ1 π΄π . This induces a splitting of the bar resolution Γ π΄ β π΄+ β Β· Β· Β· β π΄+ β π΄ span(π 0 β Β· Β· Β· β 1 β Β· Β· Β· β ππ ). This is because π (πΌ β 1 β π½) = π (πΌ) β 1 β π½ Β± πΌ β 1 β π (π½) + stuff and you can check that the stuff is all like Β· Β· Β· ππ β1 β ππ Β· Β· Β· β Β· Β· Β· ππ β1 β ππ Β· Β· Β· so it cancels. Therefore, both of the above are closed under the π-action. Hence, we can consider the reduced bar resolution and we can use it to compute graded Extπ΄β’ (π, π) and show that it is π΄! . Γ Γ β Define the graded dual of π = ππ to be π β := ππ ; in this notation, the cobar complex is π΄β+ β π΄ββ2 β Β·Β·Β· + where the first is in degree β©½ β1, the second is in degree β©½ β2, and so on. Consider the degree βπ part in the πth term; it will equal (π β ) βπ where π = π΄1 , and Extππ΄ (π, π) βπ β π β /π () where π () is spanned by π (π 1 β π 2 β Β· Β· Β· β π β π π β Β· Β· Β· β ππ ) where ππ β π β and π β π΄β2 ; this is Β±π (π 1 β π 2 β Β· Β· Β· β ππ β Β· Β· Β· β ππ ). So π : π΄β2 β π΄β1 β π΄β1 , π΄2 = π΄1 β π΄1 /πΌ , and πΌ is the space of degree 2 relations. π΄β2 = πΌ β₯ β©β π β β π β . So π β /π () β π΄π! , the quadratic dual to the quadratic part of π΄. Γ The cobar complex above is a DGA acting on the bar resolution of π. Hence, π΄! β Extππ΄ (π, π) βπ is an algebra isomorphism. π
Note : For our next topic, weβll need that π» β (πΊ, π) = Extβ’Z[πΊ ] (Z, π) where πΊ is a group (see Section 15.2 below).
13.3
Central simple algebras and Brauer group
We will look at simple Artinian rings π
, so they are of the form π
= Matπ (π·) for π· a skew field. The center of π· is a field π; then we say that π
is a central simple algebra over π. We want to understand central simple algebras of finite dimension over a given field π. Theorem 13.6: a) If π΄, π΅ are two finite-dimensional central simple algebras over π, so is π΄ βπ π΅. b) Consider the set of finite-dimensional central simple algebras over π modulo Morita equivalence. This set is in bijection with central division rings over π of finite dimension. With the operation [π΄] + [π΅] := [π΄ βπ π΅], this set forms an abelian group, called the Brauer group of π. Lemma 13.7: If π΄ is a finite-dimensional central simple algebra over π, then π΄π := π΄ βπ π΄op β Endπ (π΄). Proof. π΄ is a simple algebra iff π΄ is a simple π΄π -module (π΄-bimodule). So π (π΄) = Endπ΄π (π΄) β π and π΄ is finite-dimensional over π. Then by the density theorem, π΄π β Endπ (π΄). If π = dimπ (π΄), then dimπ (π΄π ) = 39
dimπ (End(π΄)) = π 2 , so in fact this surjection is an isomorphism.
β‘
Theorem 13.8 (Azumaya-Nakayama): Suppose A is a central simple algebra over π and π΅ is any algebra over π. Then two-sided ideals in π΄ βπ π΅ are in bijection with two-sided ideals in π΅. Proof. Our goal is to describe submodules of the π΄π βπ π΅π -module π΄βπ π΅. Consider π΄βπ π΅ as an π΄π βπ π-module first. Then itβs a simple module tensored with vector space. Hence π΄π -submodules of it are of the form π΄ βπ π , π β π΅ a subspace (this follows from the classification of submodules in a semisimple module). But π΄ βπ π is a π βπ π΅π submodule iff π is a π΅π -submodule of π΅, so in fact π must be a two-sided ideal of π΅. β‘ 14
14.1
April 4 - Brauer group and Skolem-Noether Theorems
Definition and first properties of Brauer group
Lemma 14.1: The center of a simple ring is a field. Proof. Saying that π΄ is a simple ring, i.e. it has no nontrivial proper two-sided ideals, is equivalent to saying that π΄ is simple as an π΄ βπ π΄op -module. Then Homπ΄βπ π΄op (π΄, π΄) = π (π΄) and by Schurβs Lemma, it must be a division ring. It remains to note that every commutative division ring is a field. β‘ Lemma 14.2: For π΄, π΅ two algebras over π, π (π΄ βπ π΅) = π (π΄) βπ π (π΅). Γ Proof. Suppose π₯ β π΄ β π΅ is central. We can write π₯ = ππ β ππ where the ππ β π΄ are linearly independent and likewise for the ππ β π΅π . Then for all π β π΄, βοΈ [π₯, π β 1] = [π, ππ ] β ππ = 0. Since the ππ are linearly independent, this implies the ππ are all central. Likewise, ππ β π (π΅).
β‘
Proof (of Theorem 13.6). a) By Theorem 13.8, the tensor product π΄βπ π΅ is a simple ring, and by the above lemmas its center is the field π (π΄) βπ π (π΅) = π. b) The tensor operation is well-defined up to Morita equivalence since π΄ βΌ Matπ (π΄) and Matπ (π΄) βπ π΅ = Matπ (π) βπ π΄ βπ π΅ = Matπ (π΄ βπ π΅). The operation is obviously commutative and associative, has identity π, and inverse β[π΄] = [π΄op ] since [π΄ βπ π΄op ] = [Endπ (π΄)] = [π]. To see that the set is in bijection with division rings over π of finite dimension, note that Theorem 2.16 implies that any central simple algebra π΄ with center π has the form Matπ (π·) where π· is a skew field with center π. π· is unique because we can define π· as Endπ΄ (πΏ) op where πΏ is the unique simple π΄-module. β‘ Example 14.3: Br(R) Z/2Z because there are exactly two finite-dimensional skew fields over R, namely R and H. Lemma 14.4: If πΈ/πΉ is a field extension, then π΄ is a central simple algebra over πΉ iff π΄ βπΉ πΈ is a central simple algebra over πΈ. More generally, if π΅ is an algebra over πΈ, and π΄ is an algebra over πΉ , then π΄ βπΉ π΅ is a central simple algebra over πΈ iff π΄ is a central simple algebra over πΉ and π΅ is a central simple algebra over πΈ. Proof. Assume that π΄/πΉ and π΅/πΈ are central simple algebras. Then, by Theorem 13.8, π΄ βπΉ π΅ is a simple ring. Its center is (by lemma 14.2): π (π΄ βπΉ π΅) = π (π΄) βπΉ π (π΅) = πΉ βπΉ πΈ = πΈ. Assume now that π΄ βπΉ π΅ is a central simple algebra over πΈ. Again from lemma 14.2 we know that π (π΄) βπΉ π (π΅) = π (π΄ βπΉ π΅) = πΈ so we must have π (π΄) = πΉ, π (π΅) = πΈ. It remains to note that if π΄ is not simple, then there 40
exists a nonzero proper two-sided ideal πΌ β π΄ but then πΌ βπΉ π΅ will be a nonzero proper two-sided ideal in π΄ βπΉ π΅. Contradiction finishes the proof. β‘ Corollary 14.5: If πΈ/πΉ is a field extension, it induces a group homomorphism called the base change map Br(πΉ ) β Br(πΈ), [π΄] β¦β [π΄ βπΉ πΈ]. Proof. Itβs a group homomorphism because (π΄ βπΉ πΈ) βπΈ (πΈ βπΉ π΅) πΈ βπΉ (π΄ βπΉ π΅). β‘ Example 14.6: Algebraically closed fields have no finite skew field extensions, so if π = πΒ― then Br(π) = 0. This implies that all central simple algebras over such π are of the form Matπ (π). Definition 14.7: Let π΄ be a central simple algebra over an arbitrary field πΉ . The degree of π΄ is the π such that π΄ βπΉ πΉΒ― Matπ ( πΉΒ―). Alternately, it is the π such that dimπΉ (π΄) = π 2 . Definition 14.8: The kernel of the base change map for an extension πΈ/πΉ is denoted Br(πΈ/πΉ ). Definition 14.9: Let π΄ be a central simple algebra over πΉ . We say an algebraic field extension πΈ/πΉ splits π΄, or that π΄ splits over πΈ, if [π΄] β Br(πΈ/πΉ ), i.e. π΄ βπΉ πΈ Matπ (πΈ). Example 14.10: Every central simple algebra π΄ over πΉ will split over πΉΒ―. Corollary 14.11: Every central simple algebra π΄ over πΉ will split over a finite extension, namely the one generated by the matrix coefficients of the isomorphism π΄ βπΉ πΉΒ― Matπ ( πΉΒ―) (in some bases of π΄, Matπ (πΉ )).
14.2
Torsors and Galois forms
Classifying the central simple algebras of a fixed degree over a fixed field πΉ splitting over a fixed field extension of πΈ is a special case of Galois forms or the Galois descent problem. Here is an overview of the general procedure and the classification: Assume that πΈ/πΉ is Galois. Then consider the set πΌ of all πΈ-linear isomorphism π΄ βπΉ πΈ Matπ (πΈ). PGLπ (πΈ) acts on Matπ (πΈ) by conjugation; in fact, it is isomorphic to the group of automorphisms of Matπ (πΈ) (either a special case of the Theorem 14.14, see below, or a direct computation). conj
Hence, PGLπ (πΈ) acts on πΌ by sending an isomorphism π΄ βπΉ πΈ Matπ (πΈ) to π΄ βπΉ πΈ Matπ (πΈ) ββββ Matπ (πΈ). It turns out that this action is simply transitive. On the other hand, we have an action of the Galois group πΊ = Gal(πΈ/πΉ ) on both π΄ βπΉ πΈ and on Matπ (πΈ), so it acts on πΌ by conjugation. These actions of PGLπ (πΈ) and πΊ are compatible. This defines what we call a PGLπ (πΈ)-torsor over πΊ. Hence, to every central simple algebra π΄ of degree π split over πΈ, we can assign a corresponding PGLπ (πΈ)-torsor over πΊ, and it is not hard to see that this is a bijection. For example, the trivial torsor, where πΌ = PGLπ (πΈ), corresponds to π΄ Matπ (πΉ ). We will see in the next lecture that isomorphism classes of such torsors are classified by the nonabelian cohomology group π» 1 (πΊ, PGLπ (πΈ)). Moreover, this method generalizes to other algebraic objects depending on the choice of the base field, as long as
41
βbase change under field extensionβ makes sense: fix a reference object π, then the objects whose base change to πΈ are isomorphic to π are in bijection with Aut(π)-torsors over πΊ.
14.3
Centralizer of a commutative subfield
β π΄ where π΄ is a central simple algebra over π, dimπ (π΄) = π 2 , [πΉ : 2 π] = π, and π΅ = ππ΄ (πΉ ), then dimπΉ (π΅) = ππ and π΅ is a central simple algebra over πΉ also. That β πΉ
Lemma 14.12: If π
π2
π΄ is,
πΉ
π
π
.
(π/π) 2
π΅ = ππ΄ (πΉ ) Moreover, [π΅] = [π΄ βπ πΉ ] β Br(πΉ ). Proof. π΄ βπ πΉ is a central simple algebra over πΉ , and moreover it acts on π΄ by π β π : π₯ β¦β ππ₯ π . So Endπ΄βπ πΉ (π΄) = ππ΄ (πΉ ) = π΅ is also a central simple algebra and is Morita equivalent to π΄ βπ πΉ (recall that we have the natural βΌ identification π΄ βπ π΄op ββ Endπ (π΄) and ππ΄ (πΉ ) βπ π΄op identifies with EndπΉ (π΄) β Endπ (π΄) so, by Lemma 14.4, π΅ = ππ΄ (πΉ ) is indeed a c.s.a. over πΉ ). To find dimπΉ (π΅), notice that for any central simple algebra πΆ over πΉ and a πΆ-module π with πΈ = EndπΆ (π), we have dimπΉ (πΆ) dimπΉ (πΈ) = dimπΉ (π) 2 . Moreover, πΆ βπΉ πΈ EndπΉ (π). This is because πΆ = Matπ (π·), so π = (π· π )π for some π and πΈ = Matπ (π· op ). Then πΆ βπΉ πΈ = Matππ (π· β π· op ) = Matπππ (πΉ ) = EndπΉ (π) where π = dimπΉ (π·), and taking dimensions we get the desired identity. Setting πΆ = π΄ βπ πΉ, π = π΄, π΅ = πΈ, we get 2 π . π dimπΉ (π΅) = π β dimπΉ (π΅) = π 2
2
β‘ Corollary 14.13: Let π΄ be a central simple algebra of degree π over a field π. Then every subfield πΉ of π΄ has degree β©½ π over π. Moreover, field πΉ is a maximal commutative subalgebra of π΄ iff [πΉ : π] = π. Proof. The fact that [πΉ : π] β©½ π directly follows from Lemma 14.12. If πΉ β π΄ is maximal commutative, then ππ΄ (πΉ ) must be equal to πΉ (indeed, otherwise there exists an element π₯ β ππ΄ (πΉ ) \ πΉ so πΉ [π₯] is a commutative subalgebra of π΄ that is bigger than πΉ ). So ππ΄ (πΉ ) = πΉ and the claim about the dimension of πΉ (over π) follows from Lemma 14.12. β‘ Warning : It may happen that πΉ β π΄ is a maximal commutative subfield but not a maximal commutative subalgebra (take, for example, π΄ = Matπ (π) and πΉ = π). If π΄ is a skew field, then these two properties do coincide.
14.4
Skolem-Noether
Theorem 14.14 (Skolem-Noether): Let π΄ be a simple Artinian ring with center π and π΅ a simple finitedimensional π-algebra. Then any two π-linear homomorphisms π΅ β π΄ are conjugate by an invertible element of π΄. This allows us to relate different embeddings of a given field in a central simple algebra. 42
Proof. Let π : π΅ β π΄,π : π΅ β π΄ be two π-linear maps π΅ β π΄. These give π΄ two structures as an (π΄, π΅)-bimodule: π΄π where π β π : π₯ β¦β ππ₯π (π) and π΄π where
π β π : π₯ β¦β ππ₯π (π).
π΅ op
Since π΄ βπ is simple (Theorem 13.8) and finitely generated as an π΄-module, it must be Artinian. So π΄ βπ π΅ op has only one simple module πΏ, and any module π finitely generated over π΄ will be isomorphic to πΏπ , π < β, and π is determined by the isomorphism class of π |π΄ . Then π΄π π΄π . The isomorphism is given by right multiplication by some left invertible, hence invertible, element of π΄ that conjugates π into π . β‘
14.5
Artin-Wedderburn
Theorem 14.15 (Artin-Wedderburn): There are no finite noncommutative skew fields. Hence, the Brauer group of a finite field is trivial. Proof. Suppose that π· is a noncommutative finite skew field with center πΉ = Fπ . Let πΈ β π· be a maximal commutative subfield. So by Corollary 14.13, [πΈ : πΉ ] = π where π 2 = dimπΉ (π·). For πΌ β π·, πΎ = πΉ (πΌ) will have degree π β² over πΉ with π β² | π. Then πΈ = Fππ and πΎ = Fππ β² . This implies that πΎ is isomorphic to a subfield in πΈ as an extension of πΉ . This gives us two homomorphisms πΈ β π· and πΎ β π·, so there exists an π₯ β π· Γ such that π₯πΎπ₯ β1 β πΈ by Theorem 14.14. π· Γ is a finite group and πΈ Γ β π· Γ is a subgroup, and the following lemma implies that πΈ = π·. Lemma 14.16: Let π» β πΊ be a subgroup in a finite group πΊ. If every element in πΊ is conjugate to an element in π» , then π» = πΊ. Proof. Let C be the set of conjugacy classes in πΊ. For each conjugacy class πΆ β C, we know |πΆ | = |πΊ : ππΊ (π)|, π β πΆ, and ππΊ (π) is the centralizer of π. By assumption πΆ β© π» is nonempty for every conjugacy class, and we can bound [πΊ : ππΊ (π)] |πΆ | |πΆ β© π» | β©Ύ [π» : πΆπ» (π)] β©Ύ = . [πΊ : π» ] [πΊ : π» ] with equality when πΆ β© π» is single π» -conjugacy class (first equality) and ππΊ (π) β π» (second equality). In particular, if π = 1, we will always get a strict inequality. Then Γ βοΈ |πΆ | |πΊ | |π» | = |πΆ β© π» | > = , [πΊ : π» ] [πΊ : π» ] contradiction.
β‘ β‘ 15 April 6 - Separable splitting fields and cross-product algebras
15.1
Separable splitting fields
Theorem 15.1: For a finite Galois extension πΈ/πΉ , we have a natural isomorphism Br(πΈ/πΉ ) = π» 2 (Gal(πΈ/πΉ ), πΈ Γ ). To use this theorem, we want to say that every element splits over a finite Galois extension. In characteristic 0, every finite extension is contained in a finite Galois extension and we proved that every element splits over a finite extension. In general, a field extension is contained in a Galois extension iff it is separable. Proposition 15.2: Every element in Br(πΉ ) splits over a finite separable extension (and hence over a finite Galois extension).
43
Proof. Let π· be a skew field with center πΉ (so a central simple algebra over πΉ ). Itβs enough to show that there exists a commutative subfield πΈ β π· such that πΈ β πΉ and πΈ/πΉ is separable; then we can consider instead the centralizer π· β² = π π· (πΈ); since [π π· (πΈ)] = [πΈ βπΉ π·], we are done by induction on dimπΉ π·, use Lemma 14.12. π Suppose such an πΈ does not exist. Then, by field extension theory, for every π₯ β π·, there exists π such that π₯ π β πΉ . Lemma 15.3: Let π΄ be an Fπ -algebra. For π₯ β π΄, we have ad(π₯) π = ad(π₯ π ), where ad(π₯) (π¦) = π¦ β¦β π₯π¦ β π¦π₯. Proof. If π, π are commuting elements in an Fπ -algebra, then (π β π) π = ππ β π π . Applying this to π = πΏπ₯ and π = π
π₯ , where πΏπ₯ is left multiplication by π₯ and π
π₯ is right multiplication by π₯, we see that (π β π) π = ad(π₯) π while ππ β π π = ad(π₯ π ). β‘ Now we have two ways to finish the argument. The first uses Engelβs Theorem (see 18.745): if π€ β π€π©π (πΉ ) is a subalgebra consisting of nilpotent matrices, then π€ is nilpotent. Equivalently, it is contained in the algebra of strictly upper triangular matrices in some basis. The lemma implies that ad(π₯) is nilpotent for all π₯. Hence, the image of π· in the Lie algebra EndπΉ (π·) (via the map π₯ β¦β ad(π₯)) is nilpotent by Engelβs Theorem. This contradicts that π· βπΉ πΈ Matπ (πΈ) for some πΈ. The second uses Jordan normal form. Pick π₯ β π· such that π₯ β πΉ but π₯ π β πΉ . Let πΈ = πΉ (π₯). Then [πΈ : πΉ ] = π and 2 dimπΉ (π π· (πΈ)) = ππ . By the lemma, ad(π₯) π = 0 where ad(π₯) : π· β π·, and dimπΉ (ker(ad(π₯))) = dimπΉ (π π· (πΈ)) =
dimπΉ (π·) . π
Therefore, the Jordan normal form of ad(π₯) must have π 2 /π equal Jordan blocks of size π > 1. In particular, ker(ad(π₯)) β im(ad(π₯)). So if π₯ β ker(ad(π₯)), there exists π¦ such that [π₯, π¦] = π₯. Then ad(βπ¦) fixes π₯, so ad(βπ¦) cannot be nilpotent, contradiction. β‘
15.2
Group cohomology
Let πΊ be a group. Recall that a πΊ-module is the same as a Z[πΊ]-module, and for such a πΊ-module π, we define π» π (π) := ExtπZ[πΊ ] (Z, π) where Z is the trivial Z[πΊ]-module. In other words, π» π is the πth derived functor of the functor of πΊ-invariants. To compute this, you can also use the bar resolution, which is a resolution for any flat algebra over a commutative ring, in particular Z[πΊ]. This results in a complex where πΆ π consists of maps π : πΊ π β π and the differential is π π (π0, . . . , ππ ) = π0 π (π1, . . . , ππ ) +
πβ1 βοΈ
(β1)π π (. . . , ππ ππ+1, . . .) + (β1)π π (π0, . . . , ππβ1 ).
π=0
Example 15.4: In particular, a 1-cocycle is a map π : πΊ β π such that ππ (β) β π (πβ) + π (π) = 0; these are called βcross homomorphismsβ and you can produce them from an π-torsor π over πΊ and a choice of point π₯ 0 β π . The correspondence takes a cocycle π to the πΊ-module structure on π where π.π = π + π (π) (π = π and π₯ 0 = 0). Given a torsor π and a point π₯ 0 β π , for each π β πΊ we set π (π) to be the element in π such that π(π₯ 0 ) = π₯ 0 + π (π). Varying the choice of a point results in adding a coboundary to the cocycle. We end up with a bijection between π» 1 (πΊ, π) and isomorphism classes of π-torsors over πΊ. There is also a bijection between π» 1 (πΊ, π) and extensions of Z by π because of its definition as Ext1 . Remark 15.5: Moreover, the definition of π» 1 (πΊ, π) generalizes to the case when π is a nonabelian group equipped with a πΊ-action, and in this case we view π as acting on itself on the right, while πΊ acts on the left. This does not hold for higher cohomology.
44
Example 15.6: A 2-cocycle is a map π : πΊ 2 β π such that ππ (β, π) β π (πβ, π) + π (π, βπ) β π (π, β) = 0. Definition 15.7: A cross-product extension of πΊ by π is a group πΊΛ with a normal subgroup identified Λ with π and an isomorphism πΊ/π πΊ (i.e. an extension of πΊ by π) such that the conjugation action of πΊΛ on π, which automatically factors through πΊ, coincides with the given action of πΊ on π (the cross-product). 2-cocycles are in bijection with cross-product extensions of πΊ by π together with a splitting of the surjection of sets πΊΛ β πΊ. Choosing a different splitting modifies the cocycle by a coboundary. Hence, there is a bijection between π» 2 (πΊ, π) and cross-product extensions of πΊ by π up to isomorphism.
15.3
Cross-product algebras
Recall that given a group πΊ acting on a ring π
, we can form the smash product Γ πΊ#π
= π
π , π₯ππ¦β = (π₯π(π¦))πβ . πβπΊ
Given a cocycle π β π» 2 (πΊ, π
Γ ), one can define a twisted version of this called the cross-product algebra, Γ πΊ#π π
= π
π , π₯ππ¦β = (π₯π(π¦)π (π, β))πβ . πβπΊ
Up to isomorphism, the cross-product algebra depends only on the class of π in π» 2 (πΊ, π
Γ ). This can also be described in terms of the cross-product group πΊΛ as Λ πΊ#π
/(π β [π]), π β π
Γ , [π] β πΊΛ is the corresponding element. 16
April 11 - Cohomological description of the Brauer group
More on the Brauer group.
16.1
Cross-product algebras and Galois extensions
Proposition 16.1: Suppose πΈ/πΉ is a Galois extension. Then we have a bijection between central simple algebras over πΉ with maximal commutative subfield (isomorphic to) πΈ and cross-product extensions of πΊ = Gal(πΈ/πΉ ) by πΈ Γ . Proof. The bijection will send a central simple algebra π΄ with maximal commutative subfield πΈ to πΊΛ = Nmπ΄ Γ (πΈ), where Nm is for normalizer; this is a cross-product extension of πΊ by πΈ Γ . Since conjugating by an element of πΊΛ induces a Galois automorphism of πΈ by definition, there is a homomorphism πΊΛ β πΊ. Skolem-Noether implies that this is onto. The kernel of this homomorphism is the invertible elements of π΄ that commute with πΈ. Since ππ΄ (πΈ) = πΈ, the kernel must be πΈ Γ and we have an exact sequence 0 β πΈ Γ β πΊΛ β πΊ β 0, giving us a crossproduct extension. In the other direction, the bijection will take a cross-product extension, which corresponds to π β π» 2 (πΊ, πΈ Γ ), to Γ π΄ := πΊ#π πΈ. First, we claim that π΄ is a central simple algebra. First, it is simple. Notice that πΈ βπΉ πΈ πΊ πΈ (by Galois theory) and π΄ is a free rank 1 module over πΈ βπΉ πΈ. Conjugation by an element π₯π β π΄π , π₯ β 0, will permute the copies of πΈ and send πΈβ to πΈβ β² . Therefore, for a nonzero ideal πΌ β π΄, πΌ must have a nonzero intersection with some πΈπ , hence it contains πΈπ , but then πΌ contains all the πΈπ and πΌ = π΄. And ππ΄ (πΈ) = πΈ: if π₯ = (π₯π ) β π΄ with π₯π β 0 and π β 1, we can pick π¦ β πΈ such that π(π¦) β π¦, in which case (π₯π¦)π = π(π¦)π₯ β π¦π₯ = (π¦π₯)π . Hence, π (π΄) β πΈ and π (π΄) = πΈπΊ = πΉ . Λ since if Now we check these are inverse bijections. Start with πΊΛ = πΊΛ π and let π΄ = πΊ#π πΈ. Then Nmπ΄ Γ (πΈ) = πΊ, Γ β1 β1 Γ π β π΄ normalizes πΈ, then ππ β π (πΈ) for some π β πΊ, so ππ β πΈ . Conversely, starting with π΄, mapping to a Γ cocycle π, the map (π₯π ) β¦β π₯π is a homomorphism. Then the map πΊ#π πΈ β π΄ is injective because πΊ#π πΈ is simple, 45
and moreover, these have the same dimension over πΉ , so the map is an isomorphism.
β‘
Remark 16.2: While the above gives a transparent relation between central simple algebras and cross-products, some questions about this construction turn out to be quite hard. In particular, itβs hard to determine whether a given cross-product algebra is a skew field or whether a given skew field is isomorphic to a cross-product algebra, see e.g. [2].
16.2
Maximal commutative subfields and splitting fields
Lemma 16.3: Let πΈ/πΉ be a finite extension and π΄ a central simple algebra over πΉ . Then [π΄] β Br(πΈ/πΉ ) iff π΄ is equivalent to an algebra π΄β² containing πΈ as a maximal subfield. Proof. Suppose that πΈ β π΄ is a maximal subfield. Recall that π΄ is isomorphic to a matrix algebra over some skew field π·. It is enough to show that π· splits over πΈ. From the last lecture, we proved that for a central simple algebra π· over πΉ and a field πΈ β π·, [π· βπΉ πΈ] = [π π· (πΈ)]. So if π π· (πΈ) = πΈ, then [π π· (πΈ)] = 0 and π· splits over πΈ. In the other direction, suppose that π΄ splits over πΈ and is represented by a skew field π·. Write π΄ = Matπ (π·) and consider the minimal π such that Matπ (π·) β πΈ (as πΉ -rings). Then we claim π΄β² := Matπ (π·) contains πΈ as a maximal subfield. Let π΅ = ππ΄β² (πΈ). Then [π΅] = [π· βπΉ πΈ] (also from last time). Moreover, we claim that π΅ cannot contain any nontrivial idempotents. Otherwise, π Matπ (π·)π would be a smaller central simple algebra in the same Brauer class containing πΈ, as π₯ β¦β ππ₯ would be a nonzero homomorphism πΈ β π Matπ (π·)π. Hence π΅ is a skew field. So if π΄ splits over πΈ, then [π΅] = 0 β Br(πΈ), and π΅ = πΈ as it is a skew field. So π΄β² contains π΅ = πΈ as a maximal subfield. β‘
16.3
Proof of the theorem
Corollary 16.4: Let πΈ/πΉ be a finite Galois extension. Then Br(πΈ/πΉ ) π» 2 (Gal(πΈ/πΉ ), πΈ Γ ). Proof. Now we know that there is a bijection between central simple algebras over πΉ with maximal commutative subfield πΈ and π» 2 (πΊ, πΈ Γ ). The Lemma 16.3 implies that every class π΄ in Br(πΈ/πΉ ) has a representative π΄β² with maximal commutative subfield πΈ, hence there is a map Br(πΈ/πΉ ) β π» 2 (πΊ, πΈ Γ ) (currently just a map of sets, not a homomorphism). It is an injection (on sets), since two equivalent central simple algebras of the same degree are isomorphic: if Matπ (π·) and Matπ (π·) have the same dimension over their center, π = π. So we have a bijection between Br(πΈ/πΉ ) and π» 2 (πΊ, πΈ Γ ). We need to check that this is a group homomorphism. Letβs rewrite the group structure on π» 2 in terms of crossproducts. Given πΊΛ π 1 and πΊΛ π 2 , one can check that πΊΛ π 1π 2 πΊΛ π 1 ΓπΊ πΊΛ π 2 /(π, βπ) β π Γ π. Now we want to check that
π΅ := π΄π 1 βπΉ π΄π 2 βΌ π΄π 1π 2 .
But π΅ β πΈ βπΉ πΈ = πΊ πΈ. Let π = 11 β πΈ βπΉ πΈ. Then ππ΅π π΄π 1π 2 and this represents the class [π΄π 1 ] + [π΄π 2 ], so the group structures on both are compatible. β‘ Γ
16.4
Applications
Proof (of Theorem 14.15). Recall that we want to prove that there are no finite noncommutative skew fields. This is equivalent to proving that Br(Fππ /Fπ ) is trivial, i.e. by the above, that π» 2 (πΊ, FπΓπ ) = 0. The Galois group of this extension is Z/πZ. Pick a generator πΎ β Z/πZ. For cyclic groups, we can use the following resolution of Z to compute π» β (Z/πZ, π): 1++Β·Β·Β·+πΎ πβ1
1βπΎ
1+πΎ +Β·Β·Β·+πΎ πβ1
1βπΎ
Β· Β· Β· β Z[πΊ] ββββββββββ Z[πΊ] ββββ Z[πΊ] βββββββββββ Z[πΊ] ββββ Z[πΊ] β Z
46
where the leftmost arrow fits in the exact sequence because (1 β πΎ)
πβ1 βοΈ
ππ πΎ π =
πβ1 βοΈ
π=0
π=0
The complex is 2-periodic, since πβ1 βοΈ π=0
(ππ β ππ β1 )πΎ π = 0 β ππ = π π βπ, π .
! πΎ
π
πβ1 βοΈ
! ππ πΎ
π
=
π=0
πβ1 βοΈ π=0
! ππ
πβ1 βοΈ
! πΎ
π
.
π=0
Γ So π» 2π (Z/πZ, π) = π πΊ /Im(Av), where Av : π β π πΊ takes π β¦β πβπΊ π(π). Thus if πΈ/πΉ is a Galois extension with πΊ Z/πZ, which is our case, Br(πΈ/πΉ ) = π» 2 (πΊ, πΈ Γ ) = πΉ Γ /Nm(πΈ Γ ) where here Nm is the image of the π norm map. But for πΉ = Fπ , πΈ = Fππ , Nm(π₯) = π₯ (π β1)/πβ1 , so cyclicity of πΈ Γ implies that Nm : πΈ Γ β πΉ Γ and Br(πΈ/πΉ ) = 0. β‘ Remark 16.5: We have shown that if πΈ/πΉ is a Galois extension with πΊ Z/πZ, then Br(πΈ/πΉ ) = π» 2 (πΊ, πΈ Γ ) = πΉ Γ /Nm(πΈ Γ ). The identification can be explicitly described as follows: recall that πΎ β πΊ is a generator. Consider Γ the βtwisted polynomial algebraβ πΈβ¨π₯; πΎβ© := { π ππ π₯ π | ππ β πΈ} with π₯π = πΎ (π)π₯ for π β πΈ. Pick π β πΉ Γ , the corresponding central simple algebra is πΈβ¨π₯; πΎβ©/(π₯ π β π) (such algebras are called cyclic algebras). Example 16.6: Br(C/R) = RΓ /Nm(CΓ ) = Z/2Z. It is easy to see that the element [1] β Z/2Z corresponds to the central simple algebra H of quaternions.
16.5
Index and period
Definition 16.7: The index of an element in a Brauer group is the degree of its minimal representative. That is, the index of [Matπ (π·)] = [π·] equals π if π· is a skew field of dimension π 2 . Definition 16.8: The period of a central simple algebra π΄ over πΉ is the order of [π΄] β Br(πΉ ). Lemma 16.9: The period of an element in the Brauer group divides its index. In particular, the period is always finite, and Br is torsion. Proof. Let π· be the skew field representative of this element, say it has degree π, with center πΉ . We proved that π· has a maximal subfield πΈ such that πΈ/πΉ is separable in Proposition 15.2. Let πΎ be a Galois extension of πΉ containing πΈ and πΊ = Gal(πΈ/πΉ ). Then πΈ = πΎ π» for an index π subgroup π» β πΊ, π» = Gal(πΎ/πΈ). Now the lemma follows from the following fact about group cohomology: given a finite group πΊ, π» β πΊ of index π, and a πΊ-module π, the kernel of res : π» π (πΊ, π) β π» π (π», π) is killed by π. This is because weΓcan define a map π : π» π (π», π) β π» π (πΊ, π) so that π β¦ res is multiplication by π. For π = 0, this map sends π β¦β πβπΊ/π» π(π), and in higher degrees, take an injective resolution of π over πΊ, which will restrict to an injective resolution over π» , then apply the above map to each term of the resolution. Hence, the πth power of every element in the Brauer group vanishes. β‘ Not all integers arise as indexes of Brauer classes: Lemma 16.10: If πΉ is a perfect characteristic π field, the Brauer group has no π-torsion. Proof. A separable finite extension πΈ of πΉ is also perfect. Hence πΈ Γ β πΈ Γ , π₯ β¦β π₯ π is an isomorphism, so it induces β‘ an automorphism π» 2 (πΊ, πΈ Γ ) β π» 2 (πΊ, πΈ Γ ). Finally, we give a cohomological description of Br(πΉ ) in terms of the absolute Galois group. We can describe by taking a limit of the Br(πΈ/πΉ ), but we need to take into account that the absolute Galois group πΊ πΉ = Gal( πΉΒ―sep /πΉ ) (where πΉΒ―sep is the separable algebraic closure) is a profinite group. Hence, we need to consider continuous cohomology instead of normal cohomology, where all cocycles in the standard complex are required to be continuous. Then we can show 47
that
2 Γ π» cont (πΊ πΉ , πΉΒ―sep ) = lim π» 2 (Gal(πΈ/πΉ ), πΈ Γ ) = lim Br(πΈ/πΉ ) = Br(πΉ ). ββ
ββ πΈ
17
17.1
April 13 - Brauer groups of central simple algebras, reduced norm and trace
Reduced norm and trace
We can generalize the determinant and trace to central simple algebras. Suppose π΄ is a central simple algebra of degree π over π. Proposition 17.1: There exist unique polynomial maps π, πΏ : π΄ β π so that for any field extension πΎ/π such that π΄ splits over πΎ, ππ : π΄ βπ πΎ Matπ (πΎ) β πΎ is the trace and πΏπΎ : π΄ βπ πΎ Matπ (πΎ ) β πΎ is the determinant. π is called the reduced trace and πΏ is called the reduced norm. Example 17.2: Letβs take π΄ = H and π = R. Then π : π +ππ +π π +ππ β¦β 2π and πΏ : π +ππ +π π +ππ β¦β π 2 +π 2 +π 2 +π 2 . Proof. By the Artin-Wedderburn theorem, WLOG we can assume |π | = β so that we can say that polynomials are determined by their values on π π . Now the proof follows from Galois descent and the fact that Tr, det are invariant under all automorphisms of the matrix ring. For a fixed extension πΎ/π, π, πΏ satisfying the compatibility with Tr, det are unique; moreover, they will satisfy the same compatibility for any extension πΎ β² β πΎ, and also for πΎ β²β² β πΎ if πΎ splits π΄. So we only have to construct π, πΏ satisfying the compatibility for a fixed extension splitting π΄. Choose a finite Galois extension πΎ/π which splits π΄ and choose an isomorphism π΄ β πΎ Matπ (πΎ). Let πΊ = Gal(πΎ/π), it acts on π΄ β πΎ by acting on πΎ. It suffices for us to show that det, Tr commute with the πΊ-action, which will imply that they come from polynomial maps defined over π. To see this, consider the action of πΊ on Matπ (πΎ), which is different from the action above; say it sends π β¦β πΎ π. Then the map π β¦β πΎ β1 (πΎ π) is a πΎ-linear automorphism on Matπ (πΎ), hence given by conjugation by some element ππΎ β GLπ (πΎ). Since det is conjugation-invariant, we have det(π) = det(πΎ β1 (πΎ π)) β det(πΎ (π)) = det(πΎ π) = πΎ (det π). The same argument works for trace. So we are done.
β‘
From these, we see that π (ππ) = π (ππ), πΏ (ππ) = πΏ (π)πΏ (π), and πΏ (1) = 1.
17.2 πΆ 1 fields Definition 17.3: We say a field is a quasi-closed or πΆ 1 if any homogeneous polynomial of degree π in π > π variables has a nontrivial zero. More generally, we say a field is πΆπ if any homogeneous polynomial of degree π in π > π π variables has a nontrivial zero. Proposition 17.4: If πΉ is πΆ 1 , Br(πΉ ) = 0. Proof. Suppose not. Then let π· be a skew field finite over πΉ with π (π·) = πΉ . Then πΏ (the reduced norm) is a degree π polynomial but dimπΉ (π·) = π 2 , so πΏ has a nontrivial zero. But πΏ is invertible, a contradiction. β‘ Lemma 17.5: Finite extensions of πΆ 1 fields are also πΆ 1 .
48
Proof. Suppose πΉ is πΆ 1 and πΈ/πΉ is a degree π extension. Let π be a polynomial of degree π in π variables over πΈ. By choosing a basis for πΈ over πΉ , we can identify πΈπ = πΉ ππ . Then consider the polynomial πΛ (π₯) := NmπΈ/πΉ (π (π₯)); this is a degree ππ polynomial in ππ variables over πΉ , and it has a nontrivial zero iff π does.
β‘
Theorem 17.6 (Chevalley-Warning): Finite fields are πΆ 1 fields. Proof. The previous lemma shows that itβs enough to consider Fπ . Then the result follows from the following fact: if π is a homogeneous polynomial in π variables of degree π > π over Fπ , the number of zeroes is 0 mod π. Since there is at least one zero (the trivial one), there are at least π zeroes. So it remains to prove this fact. We know that for π β Fπ , ππ β1 is either 0 or 1 (if π β 0). So βοΈ (1 β π (π 1, . . . , ππ ) π β1 ) β‘ # zeroes of π (mod π). π 1 ,...,ππ βFπ
Every monomial in this sum (considered as a polynomial in ππ ) will have at least one variable that has exponent less than π β 1 because the polynomial has degree π (π β 1)Γand has π variables (we use that π (π β 1) < π(π β 1) because π < π). Summing over that variable and using that π ππ = 0 when 0 β©½ π < π β 1, we see that the whole sum is 0. β‘ Remark 17.7: This gives another proof of Theorem 14.15. Theorem 17.8 (Tsenβs Theorem): Suppose π is algebraically closed. Then the field πΉ = π (π‘) is πΆ 1 . Proof (Sketch). Clear denominators so that WLOG π β π [π‘] [π₯ 1, . . . , π₯π ]. Then use that a system of π homogeneous polynomial equations over π in π variables has a nontrivial solution if π > π (this is true because π is algebraically closed). If πΎ is the maximum degree (in π‘) of a coefficient of π, look at a solution of degree π . Then you get ππ +πΎ + 1 equations in (π + 1)π variables and π < π implies ππ + πΎ + 1 < (π + 1)π when π β« 0. β‘
17.3
Second approach to the cohomological description of Brauer group
Let π΄ be a central simple algebra over πΉ and πΈ/πΉ a finite Galois extension. As described in the proof of Proposition 17.1, when you fix an isomorphism π΄ βπΉ πΈ Matπ (πΈ), you get two πΊ-actions, πΎ (π) and πΎ π, that differ by conjugation by ππΎ β GLπ (πΈ). This ππΎ is determined up to multiplication by a scalar matrix, so ππΎ1 ππΎ2 and ππΎ1πΎ2 have the same image in PGLπ (πΈ) = Aut(Matπ (πΈ)) (but lifting to GLπ requires a choice). So we can define π (πΎ 1, πΎ 2 ) = ππΎ1 ππΎ2 ππΎβ1 β πΈΓ. 1πΎ 2 In fact, π is a 2-cocycle, and its class in π» 2 is independent of choice. Therefore, we get a map Br(πΈ/πΉ ) β π» 2 (πΊ, πΈ Γ ), and itβs an isomorphism.
49
Remark 17.9: We can interpret the definition of π as follows. The set of isomorphisms π΄ βπΉ πΈ Matπ (πΈ) form a PGLπ (πΈ)-torsor over πΊ. As discussed earlier, the isomorphism class of this torsor corresponds to an element πΛ β π» 1 (πΊ, PGLπ (πΈ)), the nonabelian cohomology group. A short exact sequence of abelian groups with a πΊ-action will produce a long exact sequence in cohomology. For 1 β πΈ Γ β GLπ (πΈ) β PGLπ (πΈ) β 1 the first few terms of the sequence are still well-defined, even though the sequence involves two nonabelian groups. The class π is the image of πΛ under the connecting homomorphism. The injectivity of the map can be deduced from Hilbertβs Theorem 90, which says that π» 1 (πΊ, GLπ (πΈ)) = 1. (Hilbert originally considered the case π = 1 only.) An equivalent form of this statement is as follows: given an π-dimensional πΈ-vector space ππΈ with a compatible πΊ-action, there is an πΉ -vector space ππΉ and a πΊ-equivariant isomorphism ππΈ = ππΉ βπΉ πΈ.
17.4
Brauer groups of local fields
Theorem 17.10: Let πΉ be a non-Archimedean local field, i.e. itβs a finite extension of Qπ or Fπ ((π‘)) (in which case πΉ Fπ ((π‘))). Then Br(πΉ ) Q/Z. First, let us recall without proof some facts about non-Archimedean local fields. If πΉ is such a field, we have a valuation πΉ Γ β Z satisfying π£ (ππ) = π£ (π) + π£ (π) and π£ (π + π) β©Ύ min(π£ (π), π£ (π)); we can extend this to πΉ by setting π£ (0) = β. WLOG we can assume that π£ is onto. Then there exists an element π with π£ (π) = 1, called a uniformizer. The elements π₯ with π£ (π₯) β©Ύ 0 form the ring of integers O β πΉ , the elements π₯ with π£ (π₯) β©Ύ 1 form the unique maximal ideal πͺ = π O β O, and the residue field π = O/π O is finite. For all π₯ β πΉ Γ , π₯π βπ£ (π₯ ) β O Γ . Definition 17.11: If πΈ/πΉ is a finite extension, then ππΈ /π πΉ is an extension of finite fields. Its degree π πΈ/πΉ = [ππΈ : π πΉ ] is the inertia degree of the extension. The ramification index of the extension, π = π πΈ/πΉ , is the integer such that ππΈπ π πΉβ1 β O Γ where ππΈ , ππΉ are uniformizers of their respective valuations. Then [πΈ : πΉ ] = π πΈ/πΉ π πΈ/πΉ since you can see these are both dimππΉ (OπΈ /πͺπΈ ). Remark 17.12: This also works if πΈ is a skew field. Definition 17.13: If π = 1, we say that πΈ/πΉ is unramified. In this case, πΈ/πΉ is Galois and Gal(πΈ/πΉ ) Gal(ππΈ /π πΉ ) (in particular, it is cyclic). Proposition 17.14: Every central simple algebra over a local field πΉ splits over an unramified extension. Proof (Sketch). Let π· be a central simple algebra over πΉ . Then we can extend the valuation to π· Γ , choose a uniformizer ππ· where π£ π· (ππ· ) = 1, Oπ· = {π₯ β π· | π£ π· (π₯) β©Ύ 0}. We get a finite extension ππ· := Oπ· /ππ· Oπ· over π πΉ (note that by Artin-Wedderburn theorem, ππ· is a field), and dimπΉ π· = π 2 = [ππ· : π πΉ ]π π·/πΉ where π is the degree of π·. We also claim that π π·/πΉ , π π·/πΉ β©½ π (recall that π π·/πΉ := [ππ· : π πΉ ]). To see this, itβs enough to show the existence of commutative subfields πΈ 1, πΈ 2 in π· with π π·/πΉ β©½ [πΈ 1 : πΉ ] and π π·/πΉ β©½ [πΈ 2 : πΉ ] (use Corollary 14.13). Let πΈ 1 = πΉ (πΌ) where πΌ β Oπ· is such that πΌ mod ππ· Oπ· generates ππ· over π πΉ and πΈ 2 = πΉ (ππ· ). Therefore, π π·/πΉ = π π·/πΉ = π = [πΈ 1 : πΉ ]. This shows that πΈ 1 /πΉ is unramified and that it is a maximal commutative subfield in π·. Thus it splits π· (see Lemma 16.3) and is our desired extension. β‘
50
Proposition 17.15: If πΈ/πΉ is an unramified degree π extension of a non-Archimedean local field, then Br(πΈ/πΉ ) = Z/πZ. Proof. We saw last time that for a cyclic extension, Br(πΈ/πΉ ) πΉ Γ /Nm(πΈ Γ ). Since πΈ/πΉ is unramified, Gal(πΈ/πΉ ) Gal(ππΈ /π πΉ ) and every extension of finite fields is cyclic (the Galois group is generated by the Frobenius). For an unramified extension, OπΈΓ β OπΉΓ ; this follows from surjectivity of the associated graded maps ππΈΓ β π πΉΓ and (1 + π π OπΈ )/(1 + π π+1 OπΈ ) β (1 + π π OπΉ )/(1 + π π+1 OπΉ ), where π = π πΉ . The first map is identified with the norm and the second with the trace ππΈ β π πΉ . Since Nm(π) = π π , we get that Br(πΈ/πΉ ) = Z/πZ. β‘ Proof (of Theorem 17.10). Let πΉ unr be a maximal unramified extension of πΉ . Then it contains a unique degree π subextension πΉπ /πΉ for every π > 1 and Br(πΉ ) = Br(πΉ unr /πΉ ) = lim Br(πΉπ /πΉ ) = lim Z/πZ = Q/Z. ββ
ββ
β‘ Remark 17.16: The theorem allows us to formulate a version of the reciprocity law of Class Field Theory. Let π be a global field, i.e. a finite extension of Q or Fπ (π‘). For every valuation π£, we get a corresponding local field π π£ by completing π at π£. Then we get a map Γ Br(π) β Br(π π£ ) π£
and we claim that in fact
Br(π) β©β
Γ
Br(π π£ )
π£
and this induces an isomorphism of Br(π) with the kernel of the sum map, i.e. ( ) ! Γ βοΈ Γ Br(π) (π π£ ) β Br(π π£ )| π π£ = 0 = ker Br(π π£ ) β Q/Z . π£
π£
This is one of several equivalent forms of the reciprocity law of class field theory. For example, the corresponding identity for degree 2 central simple algebras over Q, Hπ,π = Qβ¨π, πβ©/(π 2 = π, π 2 = π, π π = βππ) is essentially equivalent to quadratic reciprocity. 18 April 18 - Azumaya algebras
18.1
Azumaya algebras
Let π
be a commutative ring and π΄ a ring over π
that is finitely generated and projective (equivalently, locally free) as an π
-module. Then the rank is a locally constant function on Spec(π
). Assume this function is nowhere vanishing. It will also be occasionally convenient for us to assume that the rank is constant. Let us use the notation π΄π := π βπ
π΄ for a homomorphism of rings π
β π. Lemma 18.1: For π
, π΄ as above the following are equivalent: a) The map π΄ βπ π΄op β Endπ
(π΄) is an isomorphism. b) For every algebraically closed field π and a homomorphism π
β π, π΄π Matπ (π). c) For every maximal ideal πͺ β π
, let π = π
/πͺ; the ring π΄π is a central simple algebra over π. Proof. We check that π) β π) β π) β π). π) β π): since π΄ is locally free, for every π
β π, Endπ (π΄π ) = (Endπ
(π΄))π . Thus property π) is inherited by base change and π΄π is a finite-dimensional central simple π-algebra. Hence itβs isomorphic to Matπ (π) when π is algebraically closed. Β― π΄π is a central simple algebra. π) β π): since π΄π βπ πΒ― Matπ (π),
51
π) β π): If π : π β π is a map of finitely generated modules over a commutative ring where π is projective that induces an isomorphism ππ β ππ for every π = π
/πͺ, then it is an isomorphism. This is because Nakayamaβs Lemma implies π is surjective, so π projective implies π π β ker π; then another application of Nakayamaβs Lemma shows that ker π = 0. Applying this fact to π = π΄ βπ
π΄op , π = Endπ
(π΄), we get the claim. β‘ Definition 18.2: A ring π΄ satisfying the equivalent conditions of the lemma is called an Azumaya algebra over π
. Example 18.3: Let π
be a Noetherian domain and π΄ an π
-algebra finitely generated as an π
-module. Let πΉ be the field of fractions of π
, and suppose π
πΉ is a central simple algebra over πΉ . Then, for a finite localization π = π
(π ) (π β π
), the ring π΄π is an Azumaya algebra over π. Example 18.4 (Differential operators in char π): Let π be a characteristic π field and π΄ = π β¨π₯, π¦β©/(π¦π₯ βπ₯π¦β1) be the Weyl algebra. Then π₯ π , π¦ π are central in π΄ since ad(π₯ π ) = ad(π₯) π while ad(π₯) 2 (π¦) = [π₯, 1] = 0, likewise for π¦. We claim that π΄ is an Azumaya algebra over π
= π [π₯ π , π¦ π ]. One can check that {π₯ ππ¦π | π, π β Zβ©Ύ0 } form a π-basis in π΄, so π΄ is a free module over π [π₯ π , π¦ π ] with basis π₯ ππ¦π , π, π β {0, . . . , π β 1}. To check that itβs an Azumaya algebra, it suffices to check this holds after an extension of Β― so WLOG we can assume that π = π. Β― Then by the Hilbert Nullstellensatz, maximal ideals in π
are scalars to π, generated by π₯ π β π, π¦ π β π for π, π β π. Then π΄π,π := π΄/(π₯ π β π, π¦ π β π) Matπ (π) = Endπ (π [π₯]/π₯ π ) where the isomorphism sends π₯ to βmultiplication by π₯ + πΌβ and π¦ to
π ππ₯
+ π½, πΌ π = π, π½ π = π.
Example 18.5 (Quantum torus): Let π΄ = Cβ¨π§, π§ β1, π‘, π‘ β1 β©/(π§π‘ = ππ‘π§) for π β CΓ fixed constant. If π is a primitive order π root of unity, then π΄ is an Azumaya algebra over C[π§π , π§ βπ , π‘ π , π‘ βπ ]; the proof is similar to the previous example. Azumaya algebras allow us to define the notion of a Brauer group over a ring. In particular, if π΄, π΅ are Azumaya algebras over π
, then so is π΄ βπ
π΅. Definition 18.6: The Brauer group of a ring π
is the set of Morita equivalence classes of Azumaya algebras over π
; [π΄] + [π΅] = [π΄ βπ
π΅], β[π΄] = [π΄op ]. For a homomorphism π
β π, we have a base change homomorphism Br(π
) β Br(π), given by π΄ β¦β π΄π ; this is a homomorphism since π΄π is Azumaya over π and (π΄ βπ
π΅)π π΄π βπ π΅π . Remark 18.7: [π΄] = 0 iff π΄ Endπ
(π) where π is a finitely generated projective constant rank module over π
. This does not necessarily imply that π΄ Matπ (π
) as in the field case.
18.2
Cohomological description of the Brauer group over a ring - preliminary discussion
Recall that for a central simple algebra π΄ over a field πΉ , we proved that a) π΄ is split over some algebraic extension of πΉ . b) We can choose such an extension to be separable. c) For a fixed splitting Galois extension πΈ/πΉ , the action of πΊ = Gal(πΈ/πΉ ) on π΄ βπΉ πΈ Matπ (πΈ) leads to the cohomological description of the Brauer group. These statements can be generalized to a Noetherian commutative ring π
.
52
18.3
Faithfully flat ring homomorphisms and faithfully flat descent
Let π΄ be an Azumaya algebra over a Noetherian commutative ring π
. The obvious analog of point 1 is some π with a map π
β π such that π΄π splits. However, in the ring setting, we can lose information from the base change map; for example, π
= π 1 Γ π 2 β π = π 1 . So we need an additional condition on π. One that works well is that π is faithfully flat over π
. Definition 18.8: A ring π is flat over π
if the functor π β¦β ππ , π
-Mod β π-Mod is exact. It is faithfully flat over π
if it is conservative, i.e., π β π is an isomorphism iff ππ β ππ is an isomorphism. Remark 18.9: If π is flat, the conservativity condition is equivalent to ππ β 0 for π β 0. Definition 18.10: Let π be an π
-module. The descent data for π is a module π = ππ over π, and an isomorphism π between the base changes of π to π βπ
π such that the three base changes to π βπ
π βπ
π form a commutative diagram. Proposition 18.11: If π
β π is faithfully flat, the functor sending π to its descent data is an equivalence. Remark 18.12: There is a parallel algebraic geometry statement. Notice that π 1 βπ
π 2 is the coproduct in the category of commutative rings, and Aff = Commop (affine schemes) where π
corresponds to Spec(π
), so Spec(π 1 βπ
π 2 ) = Spec(π 1 ) ΓSpec(π
) Spec(π 2 ), the fiber product. The descent data is parallel on π by gluing the corresponding data for Γ to how to define a vector bundle or sheafΓ an open covering π = ππ . Replace Spec(π
) by π , Spec(π) by π = ππ , and π βπ
π is replaced by the disjoint union of ππ β© π π . The compatibility condition for base changes to π βπ
π βπ
π correspond to checking that the data for ππ β© π π β© ππ makes sense. Noetherian rings have a faithful flatness criterion. Definition 18.13: A homomorphism of commutative rings π
β π is formally smooth if for every commutative ring π = πΛ /πΌ with πΌ 2 = 0 and compatible maps π
β πΛ , π β π , you can lift to π β πΛ . Example 18.14: Suppose π
, π are finitely generated π-algebras with π a field, π = π, πΛ = π [π‘]/π‘ 2 . Then πΌ = (π‘). We have maps π
β π [π‘]/π‘ 2 and π β π, and so also a map π
β π, so we have maximal ideals πͺπ β π, πͺπ
β π
with residue field π. Extending a map π
β π to a homomorphism to π [π‘]/π‘ 2 is equivalent to specifying a vector in (πͺπ
/πͺπ
2 ) β , i.e. the tangent vector to Spec(π
) at the corresponding point. So formal smoothness implies that the map on tangent spaces induced by π
β π is onto, a condition appearing in the definition of submersion in differential geometry. Now suppose that π
is Noetherian and π is finitely generated over π. If π is formally smooth over π
, then it is flat over π
. Moreover, if the map on π-points Hom(π, π) β Hom(π
, π) is onto for every algebraically closed field π, then π is faithfully flat.
18.4
Universal splitting
Let π΄ be an Azumaya algebra over π
of constant rank π 2 . Then we can construct an example of a faithfully flat ring π splitting π
. Theorem 18.15: a) Consider the functor πΉ sending a commutative π
-ring π to the set of isomorphisms π΄π Matπ (π). This functor is representable and is represented by a ring π univ finitely generated over π
. b) π univ is formally smooth over π
. If π
is Noetherian, it is faithfully flat over π
.
53
Proof. Recall that π΄ is a projective module over π
(of rank π 2 ). So π΄ π (π
π ) as an π
-module where π β Matπ (π
) is an idempotent. 2 First consider the functor sending π to the π-module isomorphisms π΄π π π . If π΄ π (π
π ); then such an isomorphism is equivalent to producing two matrices π β Matπ 2,π (π), π β Matπ ,π 2 (π) such that π π = πΌπ 2 and ππ = π. These are degree 2 equations in the entries of π, π, while the requirement that the isomorphism is compatible with the algebra structure on Matπ (π) is another collection of degree 2 equations on the matrix entries of π. So we can define π univ as the quotient of the polynomial ring in 2ππ 2 variables over π by the ideal generated by these degree 2 equations. To check that π univ is formally smooth over π
, we show that if π΄π Matπ (π ), then π΄πΛ Matπ (πΛ ) where π = πΛ /πΌ, πΌ 2 = 0, since thatβs what it means to be able to lift to a map π univ β πΛ . Consider a rank 1 idempotent π β Matπ (π ) (without loosing the generality we can assume that π = π 11 ). We will use the same notation for the corresponding element on π΄π . So π΄π maps isomorphically to Endπ (π΄π π). We can lift π to πΛ β π΄πΛ such that πΛ mod πΌ = π. Then π΄πΛ β EndπΛ (π΄πΛ π) is a map of free πΛ -modules of rank π 2 that is an isomorphism modulo πΌ , hence an isomorphism. Hence, π univ is flat over π
when π
is Noetherian. To check it is faithful, we need to check that π΄π Matπ (π) for every algebraically closed field π, but this is one of the properties of Azumaya algebras. β‘
18.5
Rewriting cochain complex for π» β (πΊ, πΈ Γ )
Letβs rewrite the complex used to compute π» β (πΊ, πΈ Γ ) for a finite Galois field extension πΈ/πΉ , πΊ = Gal(πΈ/πΉ )Γ in a way that can be generalized to Noetherian commutative rings. Recall that the πth term is πΆ π = Map(πΊ π , πΈ Γ ) = ( πΊ π πΈ) Γ . Γ Γ From Galois theory, πΊ πΈ πΈ βπΉ πΈ (this is an isomorphism of algebras). By induction, πΊ π πΈ = πΈ βπΉ πΈ βπΉ Β· Β· Β· βπΉ πΈ where there are π + 1 factors in the RHS. Thus πΆ π = (πΈ βπΉ Β· Β· Β· βπΉ πΈ) Γ where there are π + 1 factors in the RHS. 19
19.1
April 20 - Brauer group of a ring cont., localization
Amitsur cohomology
Let πΉ : Comm β Ab be a functor. We can generalize the complex from the previous lecture to πΉ , though we will mostly use π
β¦β Gπ (π
) = π
Γ . Given a homomorphism π
β π we can form the Amitsur complex as follows: Write ππ
βπ = π βπ
Β· Β· Β· βπ
π with π factors in the RHS. Set πΆ π := πΉ (ππ
βπ+1 ), ππ :=
π+1 βοΈ
(β1)π πΉ (ππ ) : πΆ π β πΆ π+1
π=0
where ππ : ππ
βπ+1 β ππ
βπ+2 is the insertion map that puts a 1 in the πth place, i.e. π 0 β Β· Β· Β· β π π β¦β π 0 β Β· Β· Β· β π π β1 β 1 β Β· Β· Β· β π π . π (πΉ ). We denote its cohomology by π»π/π
54
Example 19.1: Let π
= πΉ, π = πΈ with πΈ/πΉ a finite Galois extension and let the functor be Gπ . Recall that there is an isomorphism ! Γ Γ βπ+1 Γ βΌ (πΈ πΉ ) ββ πΈ = Map(πΊ π , πΈ Γ ). πΊπ
Choosing the isomorphism amounts to defining pairwise distinct homomorphisms βπ1 Β·Β·Β·ππ (π₯ 0 β π₯ 1 β Β· Β· Β· β π₯π ) = π₯ 0π1 (π₯ 1 )π1π2 (π₯ 2 ) Β· Β· Β· π1 Β· Β· Β· ππ (π₯π ) where βπ1 Β·Β·Β·ππ : πΈ πΉβπ+1 β πΈ. This commutes with ππ since if you let π₯π = 1, you skip the (π + 1)th factor and you get βπ1 Β·Β·Β·ππ (π₯ 0 β π₯ 1 β Β· Β· Β· β π₯π β1 β 1 β π₯π+1 β Β· Β· Β· β π₯π ) = βπ1,...,ππ β2,ππ β1ππ ,ππ+1,...,ππ (π₯ 0 β Β· Β· Β· β π₯π ). Hence the Amitsur complex is the standard complex computing π» β (πΊ, πΈ Γ ). Remark 19.2: The algebraic geometry interpretation: Since Commop = Aff, πΉ can also be interpreted as a contravariant functor Aff β Ab. Then π β π
corresponds to Spec(π
) β Spec(π); consider the analogous construction where you replace an affine Γ scheme by a topological space, so we can instead consider morphisms π β π where π is the disjoint union ππ of open subsets in an affine covering of π . If the assignment of an abelian group to each ππ β π comes from a sheaf F on π , we recover the Cech complex for π» β (π, F ).
19.2
Relationship between Brauer group and Amitsur cohomology
We sketch how to correspond Azumaya algebras with a class in the second cohomology. Let π΄ be an Azumaya algebra over π
and choose an isomorphism π΄π Matπ (π). Then we have two isomorphisms π΄π β2 Matπ (ππ
β2 ), and π
again, their ratio will be an Amitsur 1-cocycle π with nonabelian coefficients that is independent of the choice of iso1 (PGL ), where PGL is the functor π
β¦β PGL (π
) (again, morphism up to scaling. Hence it gives an element in π»π/π
π π π these will be nonabelian groups). Notice that PGLπ (π
) = Aut(Matπ (π
)) is an algebraic group and the homomorphism GLπ (π
)/π
Γ β PGLπ (π
) may not be surjective (unlike in the field case). Letβs just assume that we can lift π to GLπ , e.g. the map GLπ (π βπ
π) β PGLπ (π βπ
π) is surjective, so π lifts to 2 (G ) by the same procedure as in the field case: consider the πΛ β GLπ (π βπ
π). Then we can get a cocycle in π»π/π
π Γ Λ which takes values in πΈ , giving the desired cocycle. differential of π, Remark 19.3: In fact, one can find a faithfully flat π for which a lift πΛ exists, but the proof is beyond the scope π (π
, G ) (A for Amitsur) as colim π» π of the lecture. Then you can define π» fl,π΄ π π π/π
where the colimit is over all faithfully flat π. Restricting to eΒ΄ tale π, you get π» eΒ΄π t,π΄ (π
, Gπ ), and this coincides with the eΒ΄ tale cohomology of Spec(π
). 2 (π
, G ) and π» 2 (π
, G ). We have injective maps from Br(π
) into π» fl,π΄ π π eΒ΄ t,π΄
19.3
Final remarks on Brauer group
First, we describe how to generalize separable splittings to rings. It turns out that for an Azumaya algebra π΄ over π
, we can always find an eΒ΄ tale, faithfully flat homomorphism π
β π such that π΄π splits. Definition 19.4: A ring homomorphism π
β π is eΒ΄ tale if for every commutative ring π = πΛ /πΌ with πΌ 2 = 0 and compatible maps π
β πΛ , π β π , there exists a unique compatible map π β πΛ . Exercise : A finite field extension is eΒ΄ tale iff it is separable. Theorem 19.5: Let π
be a (formally) smooth finitely generated commutative domain over an algebraically closed field and πΉ = Frac(π
). Then Br(π
) β©β Br(πΉ ).
55
Proof (Sketch). The proof involves an object called the Brauer-Severi variety (to be denoted by π΅). We need the notion of a line bundle (a locally free coherent sheaf of rank 1) and the fact that for a smooth variety π over a field and π β π an open subvariety, every line bundle on π can be extended to one on π . This follows from the correspondence between line bundles and divisors and the fact that the closure of a divisor on π is a divisor on π . We also need the concept of an algebraic group action on an algebraic variety and the quotient by such an action. Let π΄ be an Azumaya algebra on π = Spec(π
) and π = π univ be the universal splitting ring. Then πΊ = PGLπ acts on π = Spec(π) so that π /πΊ π . Recall that πΊ also acts on Pπβ1 . Set π΅ := (Pπβ1 Γ π )/πΊ . Thus π΅ β π and every geometric fiber of this map is isomorphic to Pπβ1 . Then one can check that π΄ is split iff there exists a line bundle πΏ on π΅ whose restriction to a geometric fiber is isomorphic to the line bundle π (1) on Pπβ1 . If π΄πΉ splits then there exists a nonempty open π β π such that π΄π splits, so π΄ splits. β‘
19.4
Localization
Let π
be a ring and π a multiplicatively closed subset, i.e. 1 β π and π, π β π β ππ β π. Definition 19.6: The localization π
π of π
at π is the universal ring receiving a homomorphism from π
sending π to invertible elements. That is, Hom(π
π ,π ) = {π : π
β π | π (π ) is invertible βπ β π } . The Yoneda Lemma shows that π
π is unique up to unique isomorphism if it exists. Lemma 19.7: π
π = π
β¨π‘π β©π βπ /(π‘π π = π π‘π = 1).
19.5
Ore conditions
Unlike in the commutative ring case, it is hard to say much about π
π from this construction; for example, we donβt even know if π
π is the zero ring. We can impose additional conditions on π to give π
π an explicit description. Definition 19.8: Let π β π
be a multiplicative subset. The (right) Ore conditions are β’ (O1) For all π β π
, π β π, then ππ β© π π
β β
. β’ (O2) For all π β π
, π β π, if π π = 0, then there exists π‘ β π such that ππ‘ = 0. If π satisfies O1, it is called a right Ore set. If π satisfies O1 and O2, it is called a right reversible or right denominator set. There are analogous definitions for left everything. Remark 19.9: O1 allows us to pull denominators of fractions to the right: if ππ β© π π
β β
, then ππ‘ = π π for π‘ β π, π β π
. So using formal inverses, π β1π = ππ‘ β1 . Using O1 and O2, then π
π will consist of pairs (π, π ) β π
Γ π modulo the equivalence that (π, π ) βΌ (π β², π β² ) if there exist π’, π’ β² β π
such that ππ’ = π β²π’ β², π π’ = π β²π’ β² β π. That is,
ππ β1 = (ππ’) (π π’) β1 = (π β²π’ β² ) (π β²π’ β² ) β1 = π β² (π β² ) β1 .
This has a ring structure where π β¦β (π, 1) is a ring homomorphism. Remark 19.10: Localization of a ring or a module can also be presented as a filtered colimit. We can create a diagram category π· where the objects are π and Hom(π , π‘) = {π’ | π π’ = π‘ } and composition is given by π£ β¦π’ = π’π£. Then if O1 and O2 both hold, then π· is filtered. Moreover, π
π is the filtered colimit limπ· π
. This shows that localization is exact because filtered colimits are (for abelian groups); also, it comes with the forgetful functor. We will prove this next lecture.
56
20
April 25 - Ore localization, Goldie theorem
Proposition 20.1: Let π be a right reversible multiplicative subset in a ring π
, i.e. it satisfies O1 and O2. Say that (π, π ) βΌ (π β², π β² ) if there exist π‘, π‘ β² β π
such that ππ‘ = π β²π‘ β² and π π‘ = π β²π‘ β² β π (that is, π/π = π β² /π β² ). This is an equivalence relation on π
Γ π and the map (π, π ) β¦β ππ β1 is a bijection between (π
Γ π)/βΌ and the localization π
π . Proof. The relation is clearly reflexive and symmetric, we need to show transitivity. Suppose (π, π ) βΌ (π β², π β² ), so ππ‘ = π β²π‘ β² and π π‘ = π β²π‘ β² β π for some π‘, π‘ β² β π
, and also (π β², π β² ) βΌ (π β²β², π β²β² ), so there exist π’, π’ β² β π
such that π β²β²π’ = π β²π’ β², π β²β²π’ = π β²π’ β² β π. We need to find π£, π£ β²β² β π such that ππ£ = π β²β²π£ β²β², π π£ = π β²β²π£ β²β² β π. Apply O1 to πΌ := π β²π‘ β², π := π β²π’ β² to see that there exists π§ 0 β π, π₯ 0 β π
such that π β²π‘ β²π§ 0 = π β²π’ β²π₯ 0 . Applying O2 to π β² (π‘ β²π§ 0 β π’ β²π₯ 0 ) = 0, there exists some π β π such that (π‘ β²π§ 0 β π’ β²π₯ 0 )π = 0. In other words, there exist elements π§ β π, π₯ β π
satisfying π‘ β²π§ = π’ β²π₯. Therefore, ππ‘π§ = π β²π‘ β²π§ = π β²π’ β²π₯ = π β²β²π’π₯ with
π π‘π§ β π β²β²π’π₯ = π β² (π‘ β²π§ β π’ β²π₯) = 0 β π β²β²π’π₯ = π π‘π§ β π.
Hence, βΌ is an equivalence relation. To define a ring structure on the set of equivalence classes, write ππ β1 for the equivalence class of (π, π ). To multiply ππ β1 Β· ππ‘ β1 , find π β π
, π’ β π with ππ’ = π π and set ππ β1 Β· ππ‘ β1 = ππ (π‘π’) β1 . To add ππ β1 + ππ‘ β1 , find π β², π‘ β² such that π π β² = π‘π‘ β² β π (these exist using O1), then ππ β1 + ππ‘ β1 = (ππ β² ) (π π β² ) β1 + (ππ‘ β² ) (π‘π‘ β² ) β1 = (ππ β² + ππ‘ β² ) (π π β² ) β1 . One can check that these are well-defined and produce an associative ring. Denote this ring by π
π β1 . There is a map π
π β π
π β1 since the map π
β π
π β1 sending π β¦β (π, 1) sends π to units. In the other direction, there is a map π
π β1 β π
π sending (π, π ) β¦β ππ β1 . Itβs easy to see this map is a homomorphism and the two homomorphisms above are inverse isomorphisms. β‘ Corollary 20.2: For a right denominator set π β π
, the kernel of the canonical homomorphism π
β π
π is the set of elements whose right annihilator intersects π. Proof. The kernel is the set of elements π β π
such that (π, 1) βΌ (0, 1), which is true iff ππ = 0 for some π β π.
β‘
Definition 20.3: An element of π
is regular if it is neither a left nor right zero divisor. Corollary 20.4: If π consists of regular elements, the natural map π
β π
π is injective.
20.1
Ore localization as a filtered colimit
Extending the remark 19.10 from last time, the localization can also be interpreted as a filtered colimit. Recall from Definition 9.11 that a category π· is filtered if Ob(π·) β β
and β’ for every π, π β π·, there exists π β π· such that Hom(π, π) and Hom(π, π) are nonempty β’ for every pair of parallel morphisms π, π : π β π, there exists π : π β π such that π β¦ π = π β¦ π . Taking the filtered limit of abelian groups is exact and commutes with the filtered colimit of sets under the forgetful functor. The filtered colimit of sets can be described as follows: for a functor πΉ : π· β Set, its colimit is the
57
quotient
Γ
πΉ (π)/βΌ
πβOb(π· )
where π₯ βΌ π¦ for π₯ β πΉ (π), π¦ β πΉ (π) if π¦ = πΉ (π) (π₯) for some π β Hom(π, π). (That is, thereβs an arrow in the image of πΉ from π₯ to π¦.) As in the last lecture, we can create a diagram category π· where the objects are π and Hom(π , π‘) = {π’ | π π’ = π‘ } and composition is given by π£ β¦ π’ = π’π£. Proposition 20.5: If π is a right denominator set (i.e. both O1 and O2 hold), then π· is filtered. Proof. First, π· is nonempty because 1 β π. For every π , π‘ β Ob(π·) = π, there exists π, π such that π π = π‘π via O1, so Hom(π , π π) and Hom(π‘, π‘π) are nonempty. Two parallel morphisms π β π‘ are π, π β π
such that π‘ = π π = π π. Then by O2, π (π β π) = 0 implies there exists π’ β π such that (π β π)π’ = 0. So by composing the two parallel morphisms π, π with the morphism π‘ β π‘π’ given by π’, we get the same morphism. β‘ Now for π a right π
-module, define a functor πΉπ : π· β π
op -mod by sending every object to π and every morphism corresponding to π’ β π
to right multiplication by π’. Hence, π
π is the colimit of πΉπ
. Therefore, colim πΉπ := π βπ
π
π =: ππ is the localization of π at π, and π β¦β ππ is exact. Remark 20.6: Ore conditions can also be generalized to categories: many important constructions involve inverting a class of morphisms in a category, and the generalization of the Ore conditions guarantees a manageable result. The construction of a derived category as a localization of the homotopy category of complexes is an example.
20.2
Ore domains
Definition 20.7: A ring π
is an Ore domain if itβs a domain and π
\{0} satisfies O1. In this case, π
π for π = π
\{0} is clearly a skew field and π
π = Frac(π
). Example 20.8: A free ring (e.g. over a field) with at least two generators is not an Ore domain: if π₯, π¦ are free generators then π₯π
β© π¦π
= 0. Proposition 20.9: Assume π
is a domain. a) (Goldie) Either π
is a right Ore domain or it contains a free right ideal of infinite rank. b) (Jategoankar) Say π
is an algebra over a field π. Then either π
is a left and right Ore domain or it contains a free ring π β¨π₯, π¦β©. Proof.
a) Suppose π
is not a right Ore domain, so there exist π, π such that ππ β© ππ
= β
(recall that π = π \ {0}). Then we claim that π, ππ, π 2π, . . . , is right independent over π
. Otherwise, we could find {ππ } such that ! π π βοΈ βοΈ π π β1 π πππ = 0 β βππ 0 = π π πππ , π=0
π=1
contradiction (note that we can assume that π 0 β 0 i.e. βπ 0 β π). b) Suppose π
is not a right Ore domain and pick π₯, π¦ such that π₯π
β©π¦π
= 0. Let π (π₯, π¦) = π+π₯ π1 +π¦ π2 be a minimal relation where π β π. If π = 0, then π₯ π1 = π¦ π2 β 0 but π₯π
β© π¦π
= 0, contradiction. If π β 0, multiplying everything by π¦ on the right, we have ππ¦ + π₯ π1π¦ + π¦ π2π¦ = 0. Since π β π, ππ¦ = π¦π and π₯ (π1π¦) = π¦ (π + π2π¦). These are again both nonzero: if π1π¦ = 0, then π1 = 0 because π
is a domain, so π¦ π2 + π = 0, so π¦ is invertible. Then π¦π
= π
, so π₯π
β© π¦π
β 0, contradiction. Likewise, π + π2π¦ β 0. So π₯π
β© π¦π
has a nonzero element, a contradiction. Thus π₯, π¦ generate a free algebra. 58
The same argument works if π
is not a left Ore domain. β‘
20.3
Growth of algebras
Let π΄ be a finitely generated π-algebra for a field π. Let π be a (finite-dimensional) vectorΓ space of generators for π΄, so we have an onto map ππ β π΄ where ππ is a tensor algebra. Let π΄πβ©½π be the image of π β©½π π βπ and set ππ (π) := dimπ (π΄πβ©½π ). π For a different space of generators π , ππ β ππ , but ππ (π) β©½ ππ (π 0π) always for some fixed π 0 because π΄π β©½π β π΄ β©½π 0π for some π 0 .
So say that two (monotone) functions π , π on N are equivalent if there exists π 0 such that π (π) β©½ π(π 0π), π(π) β©½ π (π 0π). So the equivalence class of ππ (π) is independent of the choice of π . Definition 20.10: We say that π΄ has exponential growth if π (π) β©Ύ ππΌ π for some constants πΌ > 1, π. If π΄ does not have exponential growth, it necessarily has subexponential growth, i.e. for all πΌ > 1, π (π)/πΌ π β 0. Example 20.11: If π΄ contains a free algebra, then π΄ has exponential growth. Corollary 20.12 (of Proposition 20.9): If π΄ is a domain of subexponential growth, then π΄ is an Ore domain. Example 20.13: The Weyl algebra ππ = π β¨π₯ 1, . . . , π₯π , π¦1, . . . , π¦π β©/( [π₯π , π¦ π ] = πΏπ π , [π₯π , π₯ π ] = [π¦π,π¦ π ] = 0) and π (π€) for π€ a finite-dimensional Lie algebra are domains of polynomial, hence subexponential, growth, and therefore are Ore domains.
20.4
Semi-prime rings and Goldieβs theorem
Recall that an element is regular if itβs neither a left or right zero divisor. Remark 20.14: For a regular element, left invertibility is equivalent to right invertibility, since π π = 1 β ππ π = π β ππ = 1. Definition 20.15: A ring is called prime if πΌ π½ β 0 for any two nonzero two-sided ideals πΌ, π½ β π
. It is semi-prime if πΌ 2 β 0 for any nonzero two-sided ideal πΌ β π
. Recall that a ring is semi-primitive if its Jacobson radical vanishes, which is equivalent to the existence of a faithful semisimple (either left or right) module. Proposition 20.16: Every semi-primitive ring is semi-prime. Proof. Suppose πΌ β π
is a nonzero two-sided ideal, and π
is semi-primitive. So we can find an irreducible π
-module πΏ such that πΌπΏ β 0. Then from the density theorem, it follows that we can find π₯ β πΌ, π£ β πΏ, π£ β 0 where π₯π£ = π£. Hence, π₯ 2 β 0. β‘ The converse is not true, but we do have the following: Theorem 20.17 (Goldie): If π
is a semi-prime right Noetherian ring, then the set π of all regular elements satisfies (right) O1, and π = π
π is an Artinian semisimple ring.
59
Corollary 20.18: If π
is left or right Noetherian, it admits a homomorphism to Matπ (π·), so it satisfies the IBN. Proof. If π
is right Noetherian, then π
Β― := π
/π½ (π
) is semi-primitive and right Noetherian, hence semi-prime. By Γ Goldieβs theorem, π
Β―π is Artinian semisimple, so π
Β―π = ππ=1 Matππ (π·π ). Hence π
β π
Β― β π
Β―π β Matπ1 (π· 1 ) is the desired homomorphism.
β‘
The idea of the proof of the theorem is that π π
is βtoo bigβ to miss ππ; we need a notion of size. Definition 20.19: Let π be a right π
-module. A submodule πΈ β π is essential if for all nonzero π β π, π β© πΈ β 0. That is, every nonzero submodule in π has a nonzero intersection with π . We say that π is uniform if π β 0 and every nonzero submodule in π is essential. Example 20.20: If π is of finite length, πΈ β π is essential iff πΈ β Soc(π) and π is uniform iff Soc(π) is simple. For example, for π
= π [π‘], π = π [π‘]/(π‘ π ) is uniform. Another example is a domain π
considered as a (right) module over itself. Lemma 20.21: If π β π is a submodule, then there exists a submodule π β² β π such that π β π β² is an essential submodule in π. π β² is called the essential complement of π . Proof. Consider all submodules with zero intersection with π . Then the condition of Zornβs Lemma holds, so there exists a maximal element π β² in this set. Then π β π β² is essential in π. β‘ The measure of size we will use is the maximal number of uniform submodules of π such that their direct sum is also a submodule of π. Proposition 20.22: a) Let π Γbeπ a Noetherian module. Then it contains an essential submodule that is a sum of uniform submodules, πΈ= π=1 ππ , πΈ essential and ππ uniform. b) The number of uniform summands is independent of choices and is the Goldie rank or uniform dimension. c) Every submodule of full Goldie rank is essential. That is, if π β π and Grank(π) = Grank(π ), then π is essential in π. Corollary 20.23: If π β π
is a regular element, then π π
β π
is an essential ideal. Lemma 20.24: The preimage of an essential submodule is essential. Proposition 20.25: An essential right ideal in a semi-prime right Noetherian ring contains a regular element. Next time, we will prove these and discuss other facts about essential modules. 21
21.1
April 27 - Goldie rank and Goldie theorem
More on essential modules
Corollary 21.1: A module π has no proper essential submodules iff it is semisimple. Proof. We proved that a module π is semisimple iff every submodule π has a direct complement. So if π β π, we know it has an essential complement π β² such that π β π β² is essential. If π has no proper essential submodules, then π β π β² = π and π is semisimple. If π is semisimple, every submoduleβs direct complement doesnβt intersect it, so there are no proper essential submodules. β‘
60
Lemma 21.2: a) If π β π β π with π essential in π and π essential in π , then π is essential in π. b) The preimage of an essential submodule is essential. c) If π 1 β π1, π 2 β π2 are essential, then π 1 β π 2 β π1 β π2 is essential. a) If π β π has nonzero intersection with π (use that π β π is essential), then π β© π β π has nonzero intersection with π (use that π β π is essential). b) Let π : π β π and πΈ β π essential. Suppose π β π is a nonzero submodule. Then either π β ker(π) or π (π ) is nonzero. If π β ker(π), π β π β1 (πΈ). If π (π ) β 0, then π (π ) β© πΈ β 0, so π β© π β1 (πΈ) β 0. c) By a), itβs enough to consider π1 = π 1 . Then π1 β π 2 is the preimage of π 2 under the projection π1 β π2 β π2 , so it is essential by b). β‘
Proof.
21.2
Goldie rank
Definition 21.3: A module π has finite Goldie rank if it does not contain an infinite sum of nonzero submodules. Example 21.4: If π is Noetherian, it has a finite Goldie rank. In fact, one can restate the finite Goldie rank condition as the condition that split increasing chains of submodules should stabilize, where a chain of submodules ππ splits if ππ has a direct complement in ππ+1 for all π. Proposition 21.5: A finite Goldie rank module contains an essential submodule which is a finite sum of uniform submodules. Proof. Suppose for contradiction that π does not contain such an essential submodule. Then π is not uniform, so it has a nonessential submodule π 1 with essential complement πΆ 0 . Then if both π 1, πΆ 0 contain essential submodules πΈ 1, πΈ 2 respectively, then πΈ 1 β πΈ 2 is essential in π. So WLOG suppose πΆ 0 does not contain an essential submodule. Then repeat the same argument for πΆ 0 ; we get two submodules π 2, πΆ 1 where π 2 β πΆ 1 β πΆ 0 and πΆ 1 does not contain an essential submodule. Thus by induction we get πΆ 1, πΆ 2, . . . where πΆπ β ππ β πΆπ+1 . Hence π β π 1 β π 2 β Β· Β· Β· , contradicting the assumption. β‘ Γπ Theorem 21.6: Suppose π=1 ππ an essential sum of uniform submodΓπ π has finite Goldie rank and contains πΈ = ules. If π β π = π with π β 0, then π β©½ π. If π = π, then π is essential and each ππ is uniform. π π=1 π Γπ Proof. First, π β² := then we claim that π β² β© ππ = 0 for some π. Otherwise, π β² β© ππ β 0 is π=2 ππ is not Γessential. π β² essential in ππ , so by the lemma π=1 (π β© ππ ) is essential in π and π β² is essential in π. WLOG say that π β² β© π 1 = 0. Then π 1 β π 2 β Β· Β· Β· β ππ β π. Continuing inductively, with possible reindexing, π 1 β Β· Β· Β· β ππ β ππβπ β Β· Β· Β· β ππ β π. Therefore, π β©½ π. If π = π, then π is essential. If not, weβd have an essential complement π β² and π β π β² would be a sum of π + 1 nonzero submodules, contradiction. Likewise, each ππ is uniform: otherwise, it would have a nonessential submodule ππβ² with essential complement ππβ²β² , so we would again get a direct sum of π + 1 submodules. β‘ Corollary 21.7: If π has finite Goldie rank π, then every submodule in π with the same Goldie rank π is essential. Corollary 21.8: The Goldie rank can also be defined as the maximal number of ππ β 0 β π such that Example 21.9: For semisimple modules, the Goldie rank is the number of simple summands.
61
Γ π
ππ β π.
21.3
Regular elements in essential ideals
Remark 21.10: Suppose π β π
consists only of regular elements. Then the localization of an essential (resp. uniform) ideal at π is essential (resp. uniform). Theorem 21.11: An essential right ideal in a semi-prime, right Noetherian ring contains a regular element. This will imply the first statement in Goldieβs theorem: let π be the regular elements. Given π β π, π π
π
so it has the same Goldie rank as π
(as a right module over itself) and is essential in π
(use Corollary 21.7). Hence, for any π β π
, the preimage of π π
under the map π₯ β¦β ππ₯ is an essential right ideal (Lemma 21.2) and contains a regular element π‘. Thus ππ β© π π
β β
, which implies O1; O2 is vacuous for regular elements. To prove the theorem, we first start with a weaker claim. Lemma 21.12: Let π
be a right Noetherian, semi-prime ring and πΌ β π
an essential right ideal. Then the left annihilator of πΌ is zero. Proof. Let π½ be the left annihilator of πΌ . We know π½ 2 β 0 because π
is semi-prime (if πΌ 2 = 0, then (π½ π
) 2 = 0 for the two-sided ideal π½ π
). Replace πΌ by rAnn(π½ ); WLOG we can assume that πΌ is maximal among right annihilators using the Noetherian property. Since π½ 2 β 0, pick π₯, π¦ β π½ such that π₯π¦ β 0. Then π¦π
β© πΌ β 0 since πΌ is essential, so there exists π with π¦π = π§ β πΌ and π₯π¦π = 0. Then π β rAnn(πΌ ), π β rAnn(π₯π¦) β rAnn(π₯π¦) β rAnn(π¦) β πΌ which contradicts the maximality of πΌ .
β‘
Proposition 21.13: Any right ideal πΌ contains an element π₯ with rAnn(π₯) β© πΌ = 0. This proposition implies Theorem 21.11. Let πΌ be an essential ideal. Then we can find π β πΌ with rAnn(π₯) β© πΌ = 0. Since πΌ is essential, this means rAnn(π ) = 0 and ππ
is free. In particular, it has the same Goldie rank as π
, so ππ
is essential in π
. Then by the lemma, lAnn(ππ
) = lAnn(π ) = 0. So π is regular. 22
22.1
May 2 - Goldie Theorem, PI rings
Finishing up Goldie Theorem
Proof (of Proposition 21.13). First, we prove the claim when πΌ is uniform (see Definition 20.19). Again, πΌ 2 β 0 since π
is semi-prime, so pick π₯, π¦ β πΌ , π₯π¦ β 0. Then we claim that rAnn(π₯) β© πΌ = 0. Otherwise, rAnn(π₯) β© πΌ is essential in πΌ . Consider the homomorphism of (right) π
-modules πΏπ¦ : π
β πΌ given by π§ β¦β π¦π§. It follows from Lemma 21.2 that the preimage πΏπ¦β1 (rAnn(π₯) β© πΌ ) is essential in π
. So {π§ β π
| π¦π§ β rAnn(π₯)} is essential in π
. But then its left annihilator is zero by the above lemma, but π₯ β 0 is in the annihilator, contradiction. In general, choose a maximal subideal π½ β πΌ such that there exists π£ β π½ with rAnn(π£) β© π½ = 0 (via the right Noetherian property). If rAnn(π£) β© πΌ β 0, pick a uniform ideal π β rAnn(π£) β© πΌ . There exists π’ β π with rAnn(π’) β© π = 0. Set π₯ = π’ + π£. Since π β rAnn(π£), π β© π½ = 0. So if π₯ β rAnn(π’ + π£), then π₯ β rAnn(π’) β© rAnn(π£). Suppose π₯ = π’ β² + π£ β² β π β π½ . Then π’π’ β² + π’π£ β² = 0, π£π’ β² + π£π£ β² = 0. But π£π’ β² = 0 since π β rAnn(π£), so π£π£ β² = 0 β π£ β² = 0. So π’π’ β² = 0 and π’ β² = 0 by assumption on π’. Thus, π½ β π is a larger subideal in πΌ containing an element π’ + π£ whose right annihilator has zero intersection with the ideal, contradicting the maximality of π½ . β‘ Proof (of Theorem 20.17). To finish proving the Goldie theorem, we need to show that π
π is Artinian semisimple. This is equivalent to π
π being semisimple as a right module over itself, which is equivalent to saying that π
π has no proper essential ideals. Suppose that πΌ β π
π is essential. Then πΌ β© π
is essential in π
: π
β©β π
π because π consists of regular elements, so the preimage of πΌ β π
π , which is πΌ β© π
is essential. Then πΌ β© π
contains a regular element (Theorem 21.11), i.e., π
β© πΌ β© π is nonempty, so πΌ = π
π . β‘
62
22.2
Goldie rings
The statement of Goldieβs theorem required π
to be semi-prime right Noetherian. However, the proof only uses the fact that π
has 1) finite Goldie rank as a right module over itself (split ascending chains of right ideals stabilize) and 2) chains of right annihilators stabilize. This is because even though we invoked the Noetherian property to find a maximal ideal π½ β πΌ with π£ β π½ such that rAnn(π£) β© π½ = 0, the proof found an ideal of the form π½ β π , so it suffices to use that split chains terminate. Definition 22.1: If π
has finite Goldie rank as a right module over itself and chains of right annihilators stabilize, we say that π
is a (right) Goldie ring. Example 22.2: Not every right Goldie ring is right Noetherian. For example, every commutative domain where every annihilator of a nonzero element is zero and every nonzero ideal is essential is a right Goldie ring but not necessarily right Noetherian.
22.3
Applications of Goldieβs Theorem
Proposition 22.3: Let π
be a semi-prime Goldie ring and π the set of its regular elements. Then if πΌ β π½ is an essential subideal, the localizations πΌπ and π½π coincide. Also, if πΌ is uniform then πΌπ is irreducible. Proof (Sketch). Essential embeddings and uniformity survive after localization. Over semi-simple Artinian rings, uniform modules are irreducible and essential embeddings are isomorphisms. β‘ Hence, Goldie rank is a measure of the size of an infinite-dimensional algebra (say, for algebras over a field) and itβs an interesting question to understand it better and compare it with other measures. Example 22.4: What is the Goldie rank of π
as a module over itself? For example, if π
is prime (in particular, if it is primitive), then π
π Matπ (π·), and the Goldie rank will be π. A very interesting story is related to the study of this invariant for π
= π (π€)/πΌ where π€ is a complex simple finitedimensional Lie algebra (e.g. π°π©(π)) and πΌ is a primitive ideal. Then the answer is given by the βGoldie rank polynomialβ; the classification of ideals involves a parameter π on which the answer depends polynomially. This is largely understood due to the work of various authors, including David Vogan, George Lusztig, Tony Joseph, and, more recently, Ivan Losev. Another famous question related to noncommutative localization and Lie theory is the Gelfand-Kirillov conjecture. This states that for a large class of Lie algebras, including those mentioned above, the fraction field of π (π€) (a domain of polynomial growth, hence an Ore domain) is isomorphic to the fraction field of a ring of the form ππ [π₯ 1, . . . , π₯π ] where ππ is the Weyl algebra. This turned out to be false in general, but true for π€ = π°π©(π). However, if πΒ― = π (π€)/πͺπ (π€), where πͺ is a maximal ideal in the center of π (π€), then the fraction field of πΒ― is indeed isomorphic to the fraction field of ππ for every simple complex Lie algebra.
22.4
PI rings
Definition 22.5: A ring π
is a polynomial identity (PI) ring if there exists a nonzero element in the free algebra π β Zβ¨π₯ 1, . . . , π₯π β© such that π (π 1, . . . , ππ ) = 0 for all π 1, . . . , ππ β π
(i.e., there is a polynomial identity that all elements satisfy). Likewise, if π΄ is an algebra over a field (or commutative ring) π, it is a polynomial identity (PI) algebra if there exists a nonzero π β π β¨π₯ 1, . . . , π₯π β© such that any evaluation of π in π΄ vanishes. Example 22.6: Commutative rings are PI rings: take π (π₯, π¦) = π₯π¦ β π¦π₯. Example 22.7: Boolean rings (rings where every element is idempotent) are also PI rings with π (π₯) = π₯ 2 β π₯.
63
Example 22.8: Let ππ (π₯ 1, . . . , π₯π ) =
βοΈ
(β1) |π | π₯π (1) Β· Β· Β· π₯π (π) .
π βππ
We claim that this holds in every finite-dimensional algebra π΄ over a field π of char π β 2 when π > dimπ (π΄). This is because evaluation of ππ is a skew-symmetric multilinear functional, hence is a map Ξπ (π΄) β π΄. But if π > dimπ (π΄), then Ξπ (π΄) = 0.
22.5
Amitsur-Levitzki Theorem
Theorem 22.9 (Amitsur-Levitzki): The identity π 2π holds in the ring Matπ (π
) for any commutative ring π
. Moreover, no (nonzero) homogeneous identity of smaller degree holds (assuming π
β 0). The second part of the theorem is easier and follows from the next two lemmas. Lemma 22.10 (Staircase Lemma): Matπ (π
) does not satisfy a multilinear identity of degree π < 2π. Proof. Consider the following 2π β 1 elementary matrices: π 11, π 12, π 21, π 22, . . . , ππβ1,πβ1, ππβ1,π , ππ,π Their product in this order is an elementary matrix, namely π 1π , but their product in any other order vanishes. The first π matrices in that list for π < 2π β 1 satisfy the same property. A multilinear polynomial is a linear combination of multi-homogeneous monomials with coefficients in π
. If a degree π monomial π₯ 1 Β· Β· Β· π₯π is in the polynomial, substitute the above elementary matrices for π₯π and zero for the other variables (if any). Then our sum has exactly one nonzero summand, so the sum is nonzero. β‘ Lemma 22.11: a) If a ring satisfies an identity π of degree π, then it satisfies a multilinear identity of the same degree. Γ b) If an algebra π΄ over an infinite field π satisfies a polynomial identity π = ππ where ππ is homogeneous of degree π, then each ππ is also an identity satisfied by π΄. Proof.
a) Let π = π (π₯ 1, . . . , π₯π ) be a degree π identity. We do double induction on the top degree of π in each variable and the number of variables in which it has that degree. Suppose π > 1 is the top degree and WLOG that π has degree π in π₯ 1 . Then consider π (π₯ 0, . . . , π₯π ) = π (π₯ 0 + π₯ 1, π₯ 2, . . . , π₯π ) β π (π₯ 0, π₯ 2, . . . , π₯π ) β π (π₯ 1, . . . , π₯π ). π holds in our ring and has degree less than π in both π₯ 0, π₯ 1 . For the other variables, their degree is most that of π. Note that π is not identically zero: this is because for monomials π of degree π, the noncommutative polynomials π β² = π (π₯ 0 + π₯ 1, π₯ 2, . . . , π₯π ) β π (π₯ 0, π₯ 2, . . . , π₯π ) β π (π₯ 1, . . . , π₯π ) are linearly independent over π
. This is because the monomials in π β² which are linear in π₯ 0 will enter π β² with multiplicity 1, and we can reconstruct π from such a monomial by replacing π₯ 0 by π₯ 1 . Therefore, by induction we can find an identity π which has degree one in each variable. Suppose there is a variable π₯π appearing in π in which π is not linear (so π₯π appears in some monomials but not in others). Then π (π₯ 1, . . . , π₯π , . . . , π₯π ) β π (π₯ 1, . . . , π₯π β1, 0, π₯π+1, . . . , π₯π )
is also an identity and is nonzero and linear in π₯π . Repeating this inductively, we get a multilinear identity of the same total Γdegree. b) For π β π, ππ = ππ π π is also a polynomial identity. Choosing distinct π1, . . . , ππ with π > deg(π), the linear span of πππ will contain ππ because the Vandermonde determinant doesnβt vanish. β‘ 64
This furnishes a proof of the second part of the theorem.
22.6
Amitsur-Levitzki Theorem and the cohomology of π€π©(π)
We will sketch the proof of the Amitsur-Levitzki Theorem via this Lie algebra cohomology story. To simplify notation, we work over C. Notice that the identity π 2π holding in Matπ (π) is equivalent to Tr(π 2π+1 (π₯ 1, . . . , π₯ 2π+1 )) = 0 for all π₯ 1, . . . , π₯ 2π+1 β Matπ (π). To see this, note that trace is cyclically invariant (tr(πππ) = tr(πππ), etc.), so for each monomial in π 2π+1 , we can cyclically permute the variables until π₯ 1 is at the left. Factoring π₯ 1 out, we obtain Tr(π₯ 1π 2π (π₯ 2, . . . , π₯ 2π+1 )) = 0. Since the trace pairing is nondegenerate, this implies that π 2π (π₯ 2, . . . , π₯ 2π+1 ) = 0. Now view Matπ (C) as a Lie algebra, so π€π©π (C). The multilinear functional (π₯ 1, . . . , π₯ 2π β1 ) β¦β Tr(π 2π β1 (π₯ 1, . . . , π₯ 2π β1 )) defines an element
ππ = ππ,π β Ξ2π β1 π€β
invariant under conjugation by πΊ = GLπ (C), so ππ β (Ξ2π β1 π€β )πΊ . For πΊ = GLπ (C) and other complex reductive groups, there are isomorphisms (Ξβ’π€β )πΊ π» β’ (π€) π» β’ (πΊ, C) π» β’ (πΎ, C). Here π» β’ (π€) is the Lie algebra cohomology, i.e. Extπβ’ (π€) (C, C) (parallel to the definition of group cohomology). π» β’ (πΊ, C) is the cohomology of πΊ viewed as a topological space, while πΎ β πΊ is a maximal compact subgroup and π» β’ (πΎ, C) is the cohomology for πΎ viewed as a topological space. For πΊ = GLπ (C), the maximal compact subgroup πΎ is the group π (π) of unitary matrices, and π» β (π (π), π) = Ξ[π 1,π , π 2,π , . . . , ππ,π ], deg(ππ,π ) = 2π β 1. This is graded and skew-commutative so ππ2 = 0. This follows from induction and the fact that π (π)/π (π β 1) = π 2πβ1 (the (2π β 1)-dimensional sphere). The restriction map π» β’ (π€π©(π)) β π» β’ (π€π©(π β 1)) sends ππ,π β¦β ππ,πβ1 when π β©½ π β 1 and ππ,π β¦β 0. This gives a proof of the Amitsur-Levitski Theorem as follows: We want to show that ππ,π = 0 for π > π. We induct on π, so assume ππ,πβ1 = 0 for π > π β 1. So in particular ππ+1,π β ker(π» 2π+1 (π€π©(π)) β π» 2π+1 (π€π©(π β 1))). We claim this map is injective: the kernel of the restriction map π» β’ (π€π©(π)) β π» β’ (π€π©(π β 1)) is generated by an element of degree 2π β 1 and π» 2 (π€π©(π)) = 0, so there is nothing in the kernel in degree 2π + 1. So ππ+1,π = 0. It remains to show that ππ,π = 0 for π > π + 1. The vanishing of ππ,π is equivalent to π 2π being an identity in Matπ (C). But if the identity ππ holds, so does ππ for π > π because one can sum over the symmetric group Ξ£π by first summing over the Ξ£π -cosets in Ξ£π . This completes the induction. Remark 22.12: π» β’ (π€π©(π)) is in fact freely generated by π1,π , . . . , ππ,π, .
65
23
23.1
May 9 - Another proof of Amitsur-Levitski, PI algebras
Proof of Amitsur-Levitski Theorem
We now give a self-contained proof of the first part of Theorem 22.9 using Cayley-Hamilton, due to Rossett. Theorem 23.1 (Cayley-Hamilton): Let π₯ β Matπ (π
) be an π Γ π matrix with coefficients in π
and ππ₯ (π‘) β π
[π‘] be its characteristic polynomial. Then ππ₯ (π₯) = 0. Proof (Sketch). The βeasiest to rememberβ proof is to first reduce to π
= Z by noting that the entries ππ₯ (π₯) = 0 will be polynomials in the entries of π₯ with integer coefficients. Then it suffices to show this for π
= C. But over C all matrices can be put in Jordan normal form, and for such a matrix ππ₯ (π₯) = 0. β‘ Proof. A more aesthetically appealing proof: every matrix π΄ has an adjoint matrix π΅ such that π΄π΅ = π΅π΄ = det(π΄)Β·πΌπ where πΌπ is the identity π Γ π matrix. Then in Matπ (π
[π‘]), letting π΄ = π‘ Β· πΌπ β π₯, by definition det(π΄) = ππ₯ (π‘) and there exists π΅ such that π΅π΄ = π΄π΅ = ππ₯ (π‘) Β· πΌπ . Let Matπ (π
[π‘]) = Matπ (π
) [π‘] act on Matπ (π
) where Matπ (π
) acts via left multiplication and π‘ acts by right multiplication by π₯. Then π΄.πΌπ = 0 β (ππ₯ (π‘) Β· πΌπ ).πΌπ = 0 so ππ₯ (π₯) = 0.
β‘
Corollary 23.2: If ππ₯ (π‘) = π‘ π , then π₯ π = 0. Proof (of Theorem 22.9). It suffices to consider π
= Z since multilinear identities are inherited by the extension of scalars. Since Matπ (Z) β Matπ (Q), it is enough to consider π
= Q. We will show for a certain matrix π₯ that Tr(π₯ π ) = 0 for π = 1, . . . , π β 1, which will imply that ππ₯ (π‘) = π‘ π . Consider an auxiliary ring Ξ = Ξβ’ (Q2π ) (exterior algebra of Q2π ) where Q2π has basis π 1, . . . , π 2π . For π₯ 1, . . . , π₯ 2π β Matπ (Q) let π = π 1π₯ 1 + Β· Β· Β· + π 2π π₯ 2π β Matπ (Ξ) = Matπ (Q) βQ Ξ. Amitsur-Levitski will hold iff
π 2π = π 1 β§ Β· Β· Β· β§ π 2π Β· ππ (π₯ 1, . . . , π₯π ) = 0.
Notice that the even-degree wedges Ξev form a commutative ring, so Cayley-Hamilton applies here! Decompose Ξev = Q β Ξ2 β Β· Β· Β· β Ξ2π . So it remains to check that the coefficients of the characteristic polynomial of π 2 vanish, i.e. Tr(π 2π ) = 0. But this is true because Tr(π₯ 1 Β· Β· Β· π₯ 2π ) = Tr(π₯ 2π π₯ 1 Β· Β· Β· π₯ 2π β1 ) and this cycle is an odd permutation because the number of letters is even.
23.2
β‘
Primitive algebras and Kaplanskyβs theorem
Theorem 23.3 (Kaplansky): Let π΄ be a primitive PI algebra over a field π with a homogeneous identity of degree π. Then it is simple of degree π β©½ π/2 over its center, which is a (possibly different) field πΎ. Proof. Let πΏ be a faithful simple module over π΄ and π· := Endπ΄ (πΏ). First, dimπ· (πΏ) β©½ π/2. If not, the image of π΄ β End(πΏ) would contain Matπ (π·) as a subquotient for π > π/2 (pick some collection of π > π/2 linearly independent vectors in πΏ and consider the subalgebra π΄β² of π΄ that preserves vector space generated by these vectors, it then follows from the density theorem 3.3 that π΄β² surjects onto Matπ (π·)), which contradicts the easy part of Amitsur-Levitski. Then we claim that π· is finite over its center πΎ. If not, pick a maximal commutative subfield πΉ β π·, which exists 66
by Zornβs lemma. As we discussed earlier, WLOG we can assume the identity is multilinear, so itβs inherited by extension of scalars and also holds in πΉ βπΎ π·. By Azumaya-Nakayama, πΉ βπΎ π· is a simple ring. Moreover, by having π· act by left multiplication and πΉ by right multiplication, we get an action of πΉ βπΎ π· on π·, and π· is a simple module over πΉ βπΎ π· with EndπΉ βπΎ π· (π·) = π π· (πΉ ) = πΉ . So by the argument in the previous paragraph, π· is finite-dimensional over πΉ . πΉ βπΎ π· β EndπΉ (π·) is finite over πΎ because πΉ βπΎ π· simple impiles π· is a faithful πΉ βπΎ π·-module. Thus, π· is finite over πΎ. Finally, to get the degree bound, let πΈ be a splitting field of π·. Then Matπ (π·) βπΎ πΈ = Matπβdeg π· (πΈ) β 2π deg(π·) β©½ π via the easy part of Amitsur-Levitski.
23.3
β‘
Prime PI algebras and Posner theorem
Theorem 23.4 (Posner): Let π΄ be a prime PI algebra. Then its center π = π (π΄) is a domain. Moreover, π΄ βπ Frac(π ) Matπ (π·) for some skew field π· that is finite-dimensional over πΎ = Frac(π ). The proof follows from another fact about semi-prime PI algebras, which follows from Kaplanskyβs Theorem. Theorem 23.5 (Rowen): Let π΄ be a semi-prime PI algebra. Then every nonzero two-sided ideal meets the center. Corollary 23.6: A prime PI ring π΄ whose center is a field πΎ is a central simple algebra over πΎ. Proof. By Rowenβs theorem, every nonzero two-sided ideal in π΄ meets π . Thus, π΄ is simple, and Kaplanskyβs theorem shows π΄ is finite-dimensional over πΎ. β‘ Proof (of Theorem 23.4). π is a domain, since if π§ 1π§ 2 = 0 for central elements π§ 1, π§ 2 β π , then π΄π§ 1 Β· π΄π§ 2 = 0, contradiction. Homogeneous polynomial identities are inherited by extension of scalars, so π΄ β πΎ is simple by the Corollary 23.6. β‘
23.4
Central polynomials
The proof of Rowenβs theorem is via central polynomials, which are noncommutative polynomials that take values in the center. We will be interested in Razmyslovβs central polynomials, which, when you plug in π Γ π matrices, give back a scalar matrix (and are not identically zero). First, we start with a linear algebra construction. Recall that π = Matπ (π) has a nondegenerate trace pairing β¨π₯, π¦β© = Tr(π₯π¦). This corresponds to the element π β π βπ, π = Lemma 23.7: For π₯ β Matπ (π),
β π ππ π₯ππ
Γ
β π ππ βππ
Γ
(coevaluation) where the ππ and ππβ are dual bases.
= Tr(π₯)πΌπ .
Proof. We use the cyclicity of trace. Let π (π₯) denote the LHS. Since β¨ππ, πβ© = β¨π, ππβ©, we have ππ (π₯) = π (π₯)π. Likewise, since β¨ππ, πβ© = β¨π, ππβ©, π (ππ₯) = π (π₯π) for all π β Matπ (π). Therefore, there exists π β π such that π (π₯) = π Tr(π₯)πΌπ . If we plug in π 11 for π₯, we see that the RHS is πΌπ , so π = 1. 67
β‘
Now we will look for noncommutative polynomials in π 2 variables such that π (π 1, . . . , ππ2 ) is an element of the dual basis. Definition 23.8: The Capelli polynomial is πΆ (π₯ 1, . . . , π₯ π , π¦0, . . . , π¦π ) =
βοΈ
(β1) |π | π¦0π₯π (1) π¦1 Β· Β· Β· π₯π (π ) π¦π .
π βΞ£π
Itβs like π π , but it inserts βseparatingβ variables π¦π . Lemma 23.9: Let ππ be a basis of Matπ (π) and ππβ be its dual basis (w.r.t. the trace pairing). Define πΆπ := ππ (πΆ) where ππ is a linear endomorphism on the space of multilinear noncommutative polynomials defined by ππ (π’π₯π π£) = π£π’. Then for π 0, . . . , ππ2 any matrices, Tr(πΆ (ππ , ππ ))ππβ = πΆπ (ππ , ππ ). Proof. Let π‘ = Tr(πΆ (ππ , ππ )). We need to prove that Tr(π π πΆπ (ππ , ππ )) =
0, π β π . π‘, π = π
Using that Tr(π π (π£π’)) = Tr(π’π π π£), each monomial recovers the trace from the corresponding ππ (i.e., Tr(π π ππ (πΆ)) = Tr πΆ (..., π₯π = π π , ...)). When π β π, we get Tr(πΆ (π 1, . . . , ππ β1, π π , ππ+1, . . . , ππ )) = 0 (here we have replaced ππ with π π and used that πΆ is antisymmetric to conclude that the resulting trace is zero). When π = π, we get π‘. Moreover, plugging in the elementary matrices, we get that π‘ is not uniformly zero. β‘ Definition 23.10: The Razmyslov polynomial is ππ (π₯ 1, . . . , π₯π2 , π¦0, . . . , π¦π2 , π§) =
βοΈ
π₯π π§πΆπ (π₯ 1, . . . , π₯π2 , π¦0, . . . , π¦π2 ).
π 2
Theorem 23.11: The map Matπ (π) 2π +2 β Matπ (π) sending π₯ 1, . . . , π₯π2 , π¦0, . . . , π¦π2 , π§ to ππ (π₯π , π¦π , π§) takes values in the scalar matrices and is not identically zero. Proof. The previous lemmas tell us that ππ (π₯π , π¦π , π§) = Tr(πΆ (π₯π , π¦π )) Tr(π§)πΌπ . So we should find π₯π , π¦π for which Tr(πΆ (π₯π , π¦π )) β 0. Let π 1, . . . , ππ2 be the π 2 elementary matrices. Now if we have ππ = πππ and ππ+1 = ππ β²π β² , let π¦π := πππ β² , π = 1, . . . , π 2 β 1 and saying π 1 = πππ and ππ2 = ππ β² 1 , let
π¦0 := ππ β²π .
Now setting π₯π = ππ , the monomial corresponding to the identity permutation evaluates to π 11 while all the other monomials evaluate to 0. Therefore, ππ is nonzero here. β‘
23.5
Rowenβs Theorem for semi-primitive algebras
To prove Rowenβs Theorem, first we prove a version for semi-primitive PI algebras that uses the central polynomials above.
68
Proposition 23.12: Let π΄ be a semi-primitive PI algebra. Then every nonzero two-sided ideal meets the center. Proof. Let πΏ be an irreducible π΄-module. Then for π· = Endπ΄ (πΏ) and πΎ = π (Endπ΄ (πΏ)), Kaplanksyβs theorem, gives us a bound on π (πΏ) := dimπ· (πΏ) Β· deg(π·). The image π΄Β―πΏ of the map π΄ β End(πΏ) is isomorphic to Matπ (π·), and choosing a splitting field πΉ of π·, we get π΄Β―πΏ βπΎ πΉ Matπ (πΏ) (πΉ ). Let π be the maximal π (πΏ) such that πΌ β Ann(πΏ). Then we claim that our central polynomial π = ππ (π₯π , π¦π , π§) for π§ β πΌ lies in the center of π΄. We show that it will go to a central element in any irreducible πΏ; this is enough because π΄ is semi-primitive. If π (πΏ) > π, then π acts by zero in πΏ because π§ does. If π (πΏ) < π, then π also maps to zero because ππ is an identity in Matπ (π) for π < π. If π (πΏ) = π, π§ becomes a scalar matrix after extending scalars to πΉ as above, so it lands in πΎ. The last thing is to show that π β 0. To do so, pick πΏ with π (πΏ) = π, πΌπΏ β 0. Then πΌ maps onto π΄Β―πΏ = Matπ (π·) so it suffices to show that ππ is not an identity in Matπ (π·). But since identities are preserved by extension of scalars and ππ is not an identity in Matπ (πΉ ), ππ is nonzero in Matπ (π·). β‘
23.6
Proof of Rowenβs Theorem (for real)
Rowenβs theorem follows from the above weaker version and Theorem 23.13: If π
is a semi-prime PI algebra, then π
[π‘] is a semi-primitive PI algebra. Proof (of Theorem 23.5). If π
is a semi-prime PI algebra then π
[π‘] is a PI algebra since extension of scalars to π
[π‘] preserves multi-linear identities, hence the PI property. Now if πΌ β π
is a nonzero ideal, then πΌ [π‘] β π
[π‘] will meet the center of π
[π‘] (by Theorem 23.13). But if πΌ [π‘] meets the center, then so does πΌ . β‘ Theorem 23.13 will follow from the following. Definition 23.14: A nil ideal is an ideal consisting of nilpotent elements. Theorem 23.15 (Amitsur): If π
has no nonzero nil ideals, then π
[π‘] is semi-primitive. Proposition 23.16: A semi-prime PI algebra contains no nil ideals. Γ Proof (of Theorem 23.15). Let π½ β π
[π‘] be the Jacobson radical and suppose π (π‘) = ππ π‘ ππ β π½ is a nonzero element of the Jacobson radical. WLOG, we can assume that the length of this sum is the minimal possible for a nonzero π β π½ . Then the ππ must pairwise commute; otherwise, [ππ , π] will be a shorter nonzero polynomial in π½ . This implies that 1 + π‘π (π‘) is invertible in π
[π‘], and the coefficients of (1 + π‘π (π‘)) β1 β π
[[π‘]] lie in the commutative subring π β π
generated by the ππ . But for a commutative ring π, 1 + π‘π (π‘) β π [π‘] is invertible iff all its coefficients are nilpotent: otherwise, we could find a maximal ideal πͺ β π such that π β πͺ[π‘] and π would be invertible over (π/πͺ) [π‘], but nonconstant polynomials over fields cannot be invertible. Γ Therefore, each ππ is nilpotent. Then the set of all π 1 such that π(π‘) = ππ π‘ ππ β π½ for some π 2, . . . , ππ is a nil ideal in π
. So π½ = 0. β‘ Finally, we prove Proposition 23.16. Lemma 23.17: Suppose that a ring π
satisfies the ascending chain termination condition for right annihilators. If π
is semi-prime, then every nil left ideal is zero. Proof. Suppose πΌ is a nil left ideal. WLOG we can assume that πΌ = π
π for some π β π
. Let π½ = rAnn(π) β π
for π β πΌ, π = π₯π be maximal among right annihilators of (nonzero) elements in πΌ . Then if π π β 0, then rAnn(π π ) β rAnn(π) β rAnn(π π ) = rAnn(π). Hence π 2 = 0; otherwise for π β©Ύ 2 we have π π β 0 and π π+1 = 0, so π β rAnn(π π ) and π β rAnn(π). 69
We also claim ππ
π = 0. To see this, fix π¦ β π
and consider π = π¦π β 0. Pick π such that π π β 0, π π+1 = 0. Then π β rAnn(π π ), rAnn(π π ) β rAnn(π) β rAnn(π π ) = rAnn(π). Then π β rAnn(π) β ππ¦π = 0. Thus, π
ππ
is a nonzero nilpotent ideal, contradicting that π
is semi-prime.
β‘
Lemma 23.18: A prime PI ring satisfies the ascending chain termination condition for right and left annihilators. Γ Proof. Suppose π (π₯ 1, . . . , π₯π ) = ππ π₯π (1) Β· Β· Β· π₯π (π) is a multilinear identity holding in π
and πΌ 1 β πΌ 2 β Β· Β· Β· is an infinite ascending chain of left annihilators. Let π½π = rAnn(πΌπ ), so πΌπ β lAnn(π½π ). Now evaluate π at π₯π β πΌπ . WLOG we can assume π is the smallest degree of an identity holding for such a choice of variable values. So for π¦ β π½πβ1 , π (π₯ 1, . . . , π₯π )π¦ = 0. Also π₯π (1) Β· Β· Β· π₯π (π) π¦ = 0 when π (π) β π since π¦ β π½πβ1 , π₯π (π) β πΌπ (π) , and πΌπ (π) π½πβ1 = 0. So we can write π = π (π₯ 1, . . . , π₯πβ1 )π₯π + monomials not ending in π₯π . The previous paragraph shows that for any π₯ π β πΌπ , π (π₯ 1, . . . , π₯πβ1 )πΌπ π½πβ1 = 0. But π
is prime, so πΌπ π½πβ1 β 0. Hence π (π₯ 1, . . . , π₯πβ1 ) = 0, which contradicts the degree minimality assumption. β‘ Weβve now proved Rowenβs theorem if π
is prime. If π
is semi-prime, we need this last lemma: Lemma 23.19: A semi-prime ideal is an intersection of prime ideals. Β― π β 0. Since π
Β― is semi-prime, Proof. Let πΌ β π
be a semi-prime ideal, i.e., π
Β― := π
/πΌ is semi-prime. Let π β π
, Β― π π
) Β― 2 β 0). Let π½ be a there exists π 1 = π and ππ+1 = ππ π₯π ππ such that ππ β 0 (construct ππ inductively, using that (π
π maximal ideal in π
Β― not containing ππ for any π β©Ύ 1; this exists by Zornβs lemma. Β― is not prime), so π₯ π
π¦ Β― β π½ for some π₯, π¦ β π½ . Then for some π, ππ β π
π₯ Β― π
Β― + π½ and Suppose π½ is not prime (i.e. ring π
/π½ Β― π
Β― + π½ (use that if ππ lies in some ideal then ππ for every π β©Ύ π lies in the same ideal). But then ππ β π
π¦ Β― π
π¦ Β― π
Β― + π½ = π½ ππ+1 β π
π₯ which contradicts our choice of π½ . So π β π½ and π½ is prime. Since we can find such π½ for each π β 0, then πΌ is an intersection of these prime ideals.
β‘
Therefore, a semi-prime ring π
can be realized as a subring in the product of prime rings π
/π½ . If π
is a PI ring, then each π
/π½ is such, so a nil ideal in π
has zero image in π
/π½ for all π½ , thus, it is zero. This finally proves Rowenβs theorem. 24
24.1
May 11 - Gelfand-Kirillov dimension
Growth of algebras and Gelfand-Kirillov dimension
Recall that we defined the growth of a (finitely generated) algebra as follows: pick a finite-dimensional space of generators π , which gives us a (surjective) homomorphism ππ β π΄ and induces a filtration of π΄ by setting ! Γ βπ π΄ β©½π = im π . π β©½π
Let
π (π) := dim(π΄ β©½π ).
Then we saw that the order of growth was independent of π . Recall that π΄ has β’ subexponential growth if π (π)βοΈ< πππΌ for some π for all πΌ > 1 β’ exponential growth if lim sup π π (π) > 1 β’ polynomial growth if there exists π, πΏ such that π (π) β©½ πππΏ .
70
Definition 24.1: The Gelfand-Kirillov dimension of an algebra π΄ is inf {πΏ | βπ, π (π) β©½ πππΏ }. That is, GKdim(π΄) β Rβ©Ύ0 βͺ {β}, and this is well-defined since another function π β² such that there exists π β©Ύ 1 with π β² (π/π) β©½ π (π) β©½ π β² (ππ) will lead to the same value. Example 24.2: The GK dimension of π [π₯ 1, . . . , π₯π ] is π. Remark 24.3: There are similar definitions for finitely generated groups; if they have exponential growth, then theyβre called hyperbolic groups. (There is not much similarity in the methods and theorems though.) Remark 24.4: If π΄ β©½π+1 = π΄ β©½π , then π΄ = π΄ β©½π and π (π) will eventually be dim π΄. Hence, if dim π΄ < β, GKdim(π΄) = 0. Otherwise, weβll always have π (π) β©Ύ π + 1, so the GK dimension will be β©Ύ 1. Lemma 24.5: a) If GKdim(π΄) < 1, then π΄ is finite-dimensional so GKdim(π΄) = 0. b) GKdim(π΄[π‘]) = GKdim(π΄) + 1 c) GKdim(π΄[π β1 ]) = GKdim(π΄) if π is central and regular. a) If π (π + 1) = π (π) for some π, then π΄ β©½π+1 = π΄ β©½π . So π΄ = π΄ β©½π and π (π) will eventually be dim π΄. Hence, if dim π΄ < β, GKdim(π΄) = 0. Otherwise, weβll always have π (π + 1) β©Ύ π (π) + 1, so π (π) β©Ύ π and the GK dimension will be β©Ύ 1. b) Let π΅ = π΄[π‘] and ππ΅ = ππ΄ β ππ‘. Then π΅ β©½π = π‘ π π΄ β©½0 β π‘ πβ1π΄ β©½1 β Β· Β· Β· β π΄ β©½π , so dim π΅ β©½π β©½ (π + 1) dim π΄ β©½π . Also, dim π΅ β©½π β©Ύ π dim π΄ β©½π , so GKdim(π΄[π‘]) = GKdim(π΄) + 1. c) Again, add π β1 to the space of generators, Then dim π΄ β©½π β©½ dim(π΅ β©½π ) β©½ dim(π΄ β©½2π ) because π΅ β©½π β©β π΄ β©½2π via multiplication by ππ . So GKdim(π΄[π β1 ]) = GKdim(π΄). β‘
Proof.
Part b) implies that GKdim(π [π₯ 1, . . . , π₯π ]) = π.
24.2
Warfieldβs Theorem
The GK dimension of a noncommutative ring can take any value β©Ύ 2. Theorem 24.6 (Warfield): For any real πΏ β©Ύ 2, there exists an algebra with 2 generators whose GK dimension is πΏ. Proof. Part b) of Lemma 24.1 implies we only have to show this for πΏ β (2, 3). We will construct a quotient of π β¨π₯, π¦β© by monomials. Fix a monotonically increasing sequence πΎπ , π = 1, . . . ,, let πΌ β π β¨π₯, π¦β© be the ideal spanned by the monomials of degree at least 3 in π¦ and the monomials π₯ π π¦π₯ π π¦π₯ π , π < πΎπ , π = π + π + π. The quotient π β¨π₯, π¦β©/πΌ is a graded algebra π΄; let π΄π be the component of degree π. Then π + 2 β πΎπ dim(π΄π ) = 1 + π + 2 where the 1 + π comes from monomials of degree 0, 1 in π¦. If we take π β (0, 1) and set πΎπ = π β [ππ ], then GKdim(π΄) = max(2, 2π + 1). Hence this gives you anything in (2, 3). β‘
71
Remark 24.7: This doesnβt happen for finitely presented monomial algebras. Notice that for every finitely generated algebra π΄, one can find a finitely generated monomial algebra π΄Β― with the same growth function by setting π΄Β― to be the associated graded for a filtration on π΄. But the same construction for π΄ finitely presented does not imply that π΄Β― is finitely presented.
24.3
Bergman gap theorem
The proof of this theorem is presented in [12] chapter 2. Theorem 24.8 (Bergman gap): There is no finitely generated algebra whose GK dimension is strictly between 1 and 2. Proof. The theorem follows from the below proposition. To reduce to a graded algebra generated in degree 1, we can reduce to π΄ = π β¨π₯ 1, . . . , π₯π β©/π½ where π½ is a monomial ideal. Then take the associated graded, first by total degree, then by lexicographical order. Then either dim π΄π β©Ύ π, which implies that the GK dimension is at least 2, or there exists π with dim π΄π < π, which (by the proposition) implies that dim π΄π is bounded by a constant and the GK dimension is at most 1. β‘ Proposition 24.9: If π΄ is a graded algebra generated in degree 1 and there exists π such that dim π΄π < π, then GKdim(π΄) β©½ 1. Proof. WLOG we can assume that all relations are monomial in degree π. To prove this, we define βallowed wordsβ, where a word is allowed iff all its subwords of length π are allowed. Let π be the set of allowed words of degree π and suppose |π | β©½ π. Then the number of allowed words of degree π is bounded. This reduces to Lemma 24.10: Assume that there at most π allowed words of length π. Then for π β©Ύ 2π, every allowed word of length π has the form π€ = π€ 1π€ 2π€ 3 where π€ 2 is π-periodic for π β©½ π, |π€ 1 |, |π€ 3 | β©½ π β π, and |π€ 2 | β©Ύ π + π. (A finite word π₯ 1 Β· Β· Β· π₯π is π-periodic if π₯π+π = π₯π when π, π + π β [1, . . . , π].) Proof. We induct on |π€ |. The base case is |π€ | = 2π. Such a word will have π + 1 subwords of length π, but since there are only π distinct allowed words, at least two of these coincide and we have the desired periodicity. Now we need the following: Lemma 24.11: If a periodic word with minimal period π contains two equal subwords of length β©Ύ π β 1, then they are ππ letters apart. Proof. Extend the word to an infinite π-periodic word. Suppose the equal subwords are π₯π+1 Β· Β· Β· π₯π+π and π₯ π+1 Β· Β· Β· π₯ π+π with π β©Ύ π β 1. Then the subwords π₯π π₯π+1 Β· Β· Β· π₯π+π β1 and π₯ π π₯ π+1 Β· Β· Β· π₯ π+π β1 are each a full period of the word π₯. Since π₯π+π = π₯ π+π for all 1 β©½ π β©½ π , then π₯π = π₯ π also. So π₯ also has equal subwords π₯π Β· Β· Β· π₯π+π β1, π₯ π Β· Β· Β· π₯ π+π β1 . Let the word have length π and 1 β©½ β β©½ π, and let π‘ be an integer such that β + π‘π = π + π for 0 β©½ π β©½ π β 1. Then π₯ β+( π βπ ) = π₯ β+( π βπ )+π‘π = π₯π+π +( π βπ ) = π₯ π+π = π₯π+π = π₯ β+π‘π = π₯ β so π₯ has period π βπ. Thus π₯ has period equal to the greatest common divisor of π, π βπ and the minimality of π implies that π | π β π as desired. β‘ Now we finish the proof of the lemma. Write π€ = π₯ 1π€ β² and π€ β² = π€ 1β² π€ 2β² π€ 3β² . If |π€ 1β² | < π β π, thereβs nothing to do. Otherwise, in π₯ 1π₯ 2 Β· Β· Β· π₯π , find two coinciding length π words. These intersect π€ 2 by at least π β 1, so their intersections with π€ 2β² differ by a shift by π and π |π. One of them ends at π₯ 2π βπ (or to the left) so it contains π₯π βπ+1 . Hence π₯π βπ+1 = π₯π βπ+1+π = π₯π+1 . β‘ This finishes the proof of the proposition.
β‘
72
24.4
Ufnarovskii graph
Another way of working with allowed words is via the overlap graph, called the Ufnarovskii graph; the proof of the theorem can also be interpreted via the graph. Consider an oriented graph π whose vertices are allowed length π words and which has an edge between π€ 1 and π€ 2 iff π€ 2 is obtained from π€ 1 by removing the first letter and adding a letter at the end. Then paths of length π β π correspond to allowed words of degree π β©Ύ π. The proof of the Bergman gap theorem can be restated as follows: if there are at most π allowed words of length π, show that π contains at most one oriented cycle. Then any path in the graph enters the cycle at most once, traverses the cycle, then leaves the cycle; this is the factorization π€ = π€ 1π€ 2π€ 3 in the lemma above (see [1, Section VI.4]).
24.5
Smoktunowicz and Berele theorems
We state without proof two related results: Theorem 24.12 (A. Smoktunowicz): The Gelfand-Kirillov dimension of a graded domain cannot fall within the open interval (2, 3). Theorem 24.13 (Berele): Finitely generated PI algebras have finite GK dimension.
24.6
GK dimension of a module
Definition 24.14: We can likewise define the Gelfand-Kirillov dimension of a finitely generated module over π΄ by defining ππ (π) = dim πβ©½π where we pick generators π β π and πβ©½π = π΄ β©½π Β· π , and setting GKdim(π) = inf {πΏ | βπ, ππ (π) β©½ πππΏ }. Again, this is not dependent on the choices of π . Definition 24.15: We say that the GK dimension is exact for modules over an algebra π΄ if for π β π , GKdim(π) = max(GKdim(π ), GKdim(π/π )). Example 24.16: GK dimension is exact for finitely generated modules over Noetherian PI algebras. Suppose that π΄ is an algebra with commutative associated graded (which also is then automatically finitely generated, hence Noetherian). Then the GK dimension is exact for (f.g. modules over) π΄, because Proposition 24.17: In this case, GKdim(π) is the dimension of the support of the gr(π΄) module gr(π) = Γ πβ©½π /πβ©½π β1 . Β― Given an In fact, there is a closer relation between the commutative and noncommutative pictures. Let gr π΄ = π΄. Γ Β― increasing filtration on π΄ such that π΄ is commutative, let a good filtration on π be a filtration such that π = πβ©½π , Γ πβ©½π = 0, π΄ β©½1 πβ©½π β πβ©½π+1 , and gr π = πΒ― is a finitely generated π΄Β― module. Β― Lemma 24.18: For π΄, π as above, the (set theoretic) support supp(gr π) β Spec(π΄) and does not depend on the Β― Β― choice of filtration. Moreover, the class of π in πΎ π΄-modπ (the Grothendieck group) is independent of the choice Β― Β― of the filtration, where π΄-mod π is the category of finitely generated π΄-modules with set-theoretic support contained in π.
73
Β― Remark 24.19: The expression βset-theoretic supportβ refers to thinking of finitely generated π΄-modules as Β― Β― Β― and π is coherent sheaves on Spec(π΄). Closed subsets π β Spec(π΄) correspond to radical ideals πΌπ β π΄, set-theoretically supported on π iff every element of π is annihilated by some power of πΌπ . Note that being scheme-theoretically supported on π would instead mean that π is annihilated by πΌπ , which is stronger. β² , find π such that Proof (of lemma, sketch). Given two good filtrations πβ©½π and πβ©½π β² πβ©½π βπ β πβ©½π β πβ©½π βπ+1 .
Inducting on π, we can reduce to the situation when π = 0 and β² πβ©½π β πβ©½π β πβ©½π+1 .
Let π =
Γ
β² β² πβ©½π /πβ©½π β1, π =
Γ
β² πβ©½π /πβ©½π .
Then there are short exact sequences 0 β π β² β πΒ― β π β 0 0 β π β πΒ― β² β π β² β 0 which shows both statements.
β‘
Β― Remark 24.20: πΒ― is naturally graded, but the class of πΒ― in the Grothendieck group of graded π΄-modules may depend on the choice of the filtration. This is because one can equip π , π β² with a grading so that the first displayed SES is one of the graded modules, but the arrows in the second one will not agree with the grading.
24.7
Poincare series
Theorem 24.21 (Stephenson-Zhang): If π΄ is right (or left) Noetherian, it has subexponential growth. Lemma 24.22: β a) π΄ has exponential growth iff ππ = dim(π΄π ) has exponential growth iff lim sup π ππ > 1. b) For a sequence π(π) of exponential growth, there exist 0 < π 1 < π 2 < Β· Β· Β· such that π(ππ )
2π .
β‘
Proof (of theorem). Apply this to π(π) = dim π΄π . Inductively choose π₯π β π΄ππ such that π₯π β Theorem 24.23: Let π΄ = π β Then
Γ
π β©Ύ1 π΄π
Γπ β1 π=1
π₯π π΄π βπ .
be right (or left) Noetherian of right (or left) finite homological dimension. β(π‘) =
1 , π(π‘) β Z[π‘] π(π‘)
where β(π‘) is the Hilbert series and π(π‘) is a polynomial whose roots are all roots of unity.
74
β‘
Proof. We must have π(π‘) =
βοΈ
(β1)π dim Torππ΄ (π, π)π‘ π
(i.e. the graded Euler characteristic of Torπ΄ (π, π)). Γ All the roots π§π of π(π‘) must have |π§π | β©Ύ 1; otherwise, ππ π‘ π has radius of convergence < 1 and π΄ has exponential Γ growth. But π§π = 1 because their product will be 1/the leading coefficient of π(π‘). So all the roots satisfy |π§π | = 1. Since they are roots of a polynomial in Z[π‘], they are roots of unity. β‘ Conjecture 24.24 (Polishchuk-Positselski): The Hilbert series of a Koszul algebra is rational. Moreover, if both π΄ and π΄! have finite GK dimension, then they have the Hilbert series of a symmetric tensor exterior. Conjecture 24.25 (Anick): Assume π΄ is right Noetherian. If both GKdim(π΄) and hdim(π΄) are finite, then the Hilbert series of π΄ equals that of the symmetric algebra. 25
May 16 - Final class: noncommutative geometry
Recall that commutative algebra is closely related to algebraic geometry. A commutative ring π
corresponds to the affine scheme Spec π
, and modules over π
correspond to sheaves on Spec π
. In algebraic geometry these concepts are extended to more general non-affine schemes, while also creating powerful geometric intuition and techniques that have had a strong impact on commutative algebra. Noncommutative geometry is an area that grew out of attempts to tie noncommutative algebra to geometry in a similar way. This has not led to as comprehensive a theory as exists in the commutative case. However, it did lead to emergence of a number of different directions, some leading to impressive results. In this lecture we will briefly survey some of these directions. Our list is by no means complete; for example we donβt discuss the direction involving tools from functional analysis (πΆ β -algebras) developed by A. Connes et al.
25.1
Representation varieties
Β― Then π-points of Spec(π
) correspond to the homomorLet π
be a finitely generated commutative ring over π = π. phisms of π-algebras Hom(π
, π) i.e. to one-dimensional representations of the algebra π
. Note that every simple module over a finitely generated commutative algebra π
is one-dimensional (Hilbertβs Nullstellensatz). If π
is instead a finitely generated noncommutative algebra over π, it is natural to consider the space of all finite-dimensional representations of π
. Let us describe this space (to be denoted Rep(π
)). Γ First of all note that Rep(π
) = πβZβ©Ύ0 Repπ (π
), where Repπ (π
) is the space of π-dimensional representations of π
. Every element of Repπ (π
) corresponds to a homomorphism π : π
β Matπ (π) i.e. π β Hom(π
, Matπ (π)). Two homomorphisms π 1 , π 2 define isomorphic representations iff they lie in the same orbit of GLπ , acting naturally on the space Hom(π
, Matπ (π)) (via its action on Matπ (π)). Since π
is finitely generated, π
= π β¨π₯ 1, . . . , π₯π β©/πΌ , and 2
2
Hom(π
, Matπ (π)) β (Matπ )π = π π π = Aπ π is a subset of the affine variety (Matπ )π cut out by polynomial equations. We can consider this subset as an alge2 braic subvariety of Aπ π . We see that Repπ (π
) = Hom(π
, Matπ (π))/GLπ (π) is the quotient of the algebraic variety Hom(π
, Matπ (π)) by the action of the algebraic group GLπ (π). Space Repπ (π
) is an example of an algebraic stack. This is a replacement for Spec(π
). Preprojective algebras are examples of explicit algebras with interesting representation varieties Rep π
. Let π be an oriented quiver and let π be the corresponding double quiver. For an edge π of π we will denote by π + , π β the corresponding edges of π. Let π (π) be the quiver algebra of π modulo the relation βοΈ βοΈ π βπ+ β π +π β = 0. (3) π
π
75
For example, let π be a cyclic quiver consisting of π vertices labeled by the elements of Z/πZ (vertices [π], [π + 1] are connected by the edge). Quiver π has vertices labeled by Z/πZ, edges of this quiver are [π] β [π +1] and [π +1] β [π], [π] β Z/πZ. Pick π β π of order π and consider the action Z/πZ β· π [π₯, π¦] given by [1] Β· π₯ = π π₯, [1] Β· π¦ = π β1π¦. We have βΌ (Z/πZ)#π [π₯, π¦] ββ π (π), the isomorphism is given by: βοΈ βοΈ βοΈ 1 β π₯ β¦β π [π+1]β[π ] , 1 β π¦ β¦β π [π ]β[π+1] , [1] β 1 β¦β π π π [π ] . [π ] βZ/πZ
[π ] βZ/πZ
[π ] βZ/πZ
The isomorphism above induces the equivalence between the categories of π (π) and (Z/πZ)#π [π₯, π¦]-modules. Let Γ us describe this equivalence explicitly. Module (π [π ] ) [π ] βZ/πZ over π (π) goes to π := [π ] βZ/πZ π [π ] , where the π action of [1] β Z/πZ on π [π ] is given by π and the action of π₯ : π [π ] β π [π+1] is given by π [π+1]β[π ] , the action of Γ Γ π¦ : π [π+1] β π [π ] is given by π [π ]β[π+1] . The condition [π ] βZ/πZ π [π ]β[π+1] π [π+1]β[π ] = [π ] βZ/πZ π [π+1]β[π ] π [π ]β[π+1] precisely corresponds to the fact that π₯ and π¦ commute. This example can be generalized as follows. Recall that finite subgroups Ξ in SL(2, π) correspond to simply laced b be the affine Dynkin graph; the vertices Dynkin graphs π· (this is known as McKay correspondence, see [15]). Let π· b of π· are in bijection with irreps of Ξ (see [15]). Then (see [7]) b βΌ Ξ#π [π₯, π¦] π ( π·) Γ where the βΌ is Morita equivalence. It sends a Ξ#π [π₯, π¦]-module π to π£ ππ£ , where ππ£ = [π : π π£ ] = HomΞ (π π£ , π) and π π£ is the irreducible representation of Ξ corresponding to the vertex π£. b Ξ#π [π₯, π¦] are not isomorphic in general (they are isomorphic for Remark 25.1: Note that the algebras π ( π·), Ξ = Z/πZ). Let us describe the representation variety of the algebra π
= π (π). Let us first of all recall that π (π) is a certain quotient of the path algebra of the quiver π so every representation of π (π) can be considered as a representation Γ of the quiver π such that (3) holds. So, Rep(π (π)) = π π£ βZβ©Ύ0 Repπ π£ (π (π)), where Repπ π£ (π (π)) is the space of representations (ππ£ ) of π such that (3) holds and dim ππ£ = π π£ (considered up to an isomorphism). Explicitly, let Γ g π (π (π)) β (4) Rep Matπ π£ ,π π£β² Γ Matπ π£β² ,π π£ π£ π : π£βπ£ β²
be the subvariety consisting of collections of maps such that (3) holds. Then Γ g π (π (π))/ Repπ π£ (π (π)) = Rep GL(π π£ ). π£ π£ β Note now that the RHS Γof (4) is a symplectic vector space (we identify Matπ π£ ,π π£β² Γ Matπ π£β² ,π π£ with π Matπ π£ ,π π£β² via the trace form), and πΊ = GL(π π£ ) acts on it preserving the symplectic structure; the equations (3) are zeroes of the Γ Γ Γ moment map π : π : π£βπ£ β² π β Matπ π£ ,π π£β² β π£ Matπ π£ for the π£ GLπ π£ action. So, Repπ π£ (π (π)) is obtained from the RHS by Hamiltonian reduction i.e. Γ Repπ π£ (π (π)) = π β1 (0)/ GLπ π£ π£
is the Hamiltonian reduction of the symplectic vector space
76
Γ
π : π£βπ£ β² π
β Mat π π£ ,π π£ β²
by
Γ
π£
GLπ π£ .
Remark 25.2: Ginzburg introduced a notion of a quiver with potential (see [8, Section 4.2]). Potential is an element of the vector subspace πΉ cyc of the quiver algebra πΉ = ππ of a quiver π generated by cyclic paths. π : πΉ cyc β πΉ defined as follows: given a cyclic path Ξ¦ = ππ 1 ππ 2 . . . πππ , we For any edge π β π· there exists a map ππ put βοΈ πΞ¦ := πππ +1 πππ +2 . . . πππ ππ 1 ππ 2 . . . πππ β1 . ππ {π | πππ =π }
πΞ¦ One can then consider the quotient algebra π(π, Ξ¦) := πΉ /( πΞ¦ ππ )π βπ , where ( ππ )π βπ· is the two-sided ideal generated by the elements πΞ¦ ππ β πΉ (see [8, Equation (4.2.1)]). g π π(π, Ξ¦) can be described as follows. Consider the space Rep g π (πΉ ) (that is just a vector space), The variety Rep π£ π£ Γ g b element Ξ¦ defines a map Ξ¦ : Repπ π£ (πΉ ) β π£ Matπ π£ sending a representation π to π (Ξ¦) (recall that Ξ¦ β πΉ cyc ). g π (πΉ ) β C. One can show that the variety Rep g π π(π, Ξ¦) is the critical We obtain a functional π := tr b Ξ¦ : Rep π£ π£ b locus of tr Ξ¦ (cf. [8, Section 2.3]). Let us describe how to obtain preprojective algebras via algebras with potentials (see [8, Example 4.3.3]). Con-
sider the quiver π
loop
obtained from π by attaching an additional edge loop, π‘ π£ , for every vertex π£. We can loop
identify the quiver algebra ππ with Γ ππ β π [π‘], where β corresponds to the free product of associative πalgebras (this isomorphism sends π‘ to π£ π‘ π£ ). Consider the potential βοΈ βοΈ βοΈ Ξ¦ := π‘π£ Β· (π +π β β π β π + ) = π‘ (π +π β β π β π + ). π£
π
π
loop g π (π (π)) Γ g π π(ππ loop, Ξ¦) = π
ππ We then have π(ππ , Ξ¦) = π (π) [π‘] (see [8, Equation (4.3.4)]), so Rep π£ π£ Γ π£ Matπ π£ . The potential π that we construct above is given by the formula: Γ Γ π β Matπ π£ ,π π£β² Γ Matπ π£ β (π£, π) β¦β tr(π (π£)π) β C π : π£βπ£ β²
π£
in this case.
25.2
Weyl algebra and deformations
Many interesting algebras have no nonzero finite-dimensional representations (in particular, Rep π
= {0} is not interesting in this case). For example, the Weyl algebra π = Cβ¨π₯, π¦β©/β¨π₯π¦ βπ¦π₯ β 1β© doesnβt. You can see this by noting that tr(π₯π¦ β π¦π₯) = 0 (on every finite-dimensional representation), while tr(1π ) = π. We can study noncommutative geometry by deforming from the commutative case, this procedure is also called deformation quantization. Consider πβ = C[β] β¨π₯, π¦β©/β¨π₯π¦ β π¦π₯ β ββ©. When we take β = 1, we recover π , and when we take β = 0, we get C[π₯, π¦], which is commutative. Other examples of deformations: If π is a smooth affine algebraic variety over a field π, we can consider Diff β (π ), the asymptotic differential operators. This is π when π = A1 . If β = 0, we get O (π βπ ) = Sym O (π ) (Der(O (π ))). If π€ is a Lie algebra, let π β (π€) = π β¨π€β©/π₯π¦ β π¦π₯ = βπ₯. If π€ = π€π©π , then define πΒ―β (π€) = π β βπ (πβ (π€) ) π [β] so
πΒ―0 = O (N )
where N is the nilpotent matrices. Thereβs also the spherical rational double affine Hecke algebra (DAHA) π΄β , also called rational Cherednik algebra, where π΄0 = O ((A2 )π /ππ ). 77
How can we define deformations for non-affine varieties? Previously we deformed the algebra of functions on π , now we need to deform the structure sheaf of π . There is no obvious way to make a deformation into a sheaf. Here are some ways: a) We can work with a formal parameter. If π΄ is flat over π [[β]] and complete in the β-topology, let π΄0 = π΄/β, which is commutative. Exercise: a) if πΒ― = π (mod β) is invertible, then so is π. b) If π β Spec(π΄) is open, then Β― π is invertible} is a localizing class. c) Localizations form a Zariski sheaf on Spec(π΄). {π β π΄|π| b) Diff (π ) can be made into a sheaf on π βπ with conical topology (π β Spec(π βπ ) is open in a conical topology if it is open in Zariski topology and invariant under dilation). c) In characteristic π, for π = π β¨π₯, π¦β©/π₯π¦ β π¦π₯ = 1 has π₯ π , π¦ π β π (π ). Hence, π is a sheaf on Spec π [π₯ π , π¦ π ].
25.3
Coh(π ) and π· β (Coh(π ))
The previous two subsections described approaches closely tied to the usual commutative algebraic geometry. The next relies on it as a source of motivation for conjectures rather than trying to relate a noncommutative structure to a specific commutative ring or variety. An algebraic variety π can be studied via the category Coh(π ) on π· β (Coh(π )). Γ If π = Spec(π
) is affine, then Coh(π ) = π
-mod. If π is projective over π and π = Proj(π΄), π΄ = πβ₯0 π΄π , π΄0 = π, then Coh(π ) is the Serre quotient of graded finitely generated π΄-modules by graded finite-dimensional π΄-modules. Theorem 25.3 (Serre): Let π be an algebraic variety over a field π. Then π is smooth iff Coh(π ) has finite homological dimension, i.e. Extπ (πΉ, πΊ) = 0 for all π > π and all πΉ, πΊ β Coh(π ). It is also known that π is projective iff Extπ (πΉ, πΊ) is finite-dimensional for all π, πΉ, πΊ β Coh(π ). Let π be a smooth affine variety. Then Ξ©ππ , the π-forms, is HHπ (O (π )). Recall that HHπ and HHπ are Morita invariant. They can also be defined starting from a category: HHπ = Extπ (Id, Id) where Id is the identity functor, while HHπ relates to the tensor of bimodules. For π smooth and projective, HHπ (Coh(π )) =
Γ
π π» π (π, Ξ©π ) β π» dR (π )
πβπ=π
where the last equivalence is from the Hodge theorem, and the first one is known as the Hochschild-KostantRosenberg isomorphism. β for nonprojective π , we can use cyclic homology. The bar complex for HH has cyclic symmeTo recover π» dR β try: πΆ : π 0 β Β· Β· Β· ππ β (β1)π ππ β π 0 Β· Β· Β· β ππβ1 .
Then Bar/(πΆ β Id)Bar inherits the differential from the bar complex. Its cohomology is Γ πβ2π HCπ (π΄) = Ξ©π /π Ξ©πβ1 β π» dR (π ) π β₯1
and per
HCπ = lim HCπ+2π =
β Γ
β
π+2π π» dR (π ).
π=ββ
For a smooth projective dimension π variety π we have Serre duality: Extπ (πΉ, πΊ) β Extπβπ (πΊ, πΉ β πΎ Γ ) β .
78
Definition 25.4 (Bondal-Kapranov): Let C be a finite type π-linear triangualated category. (Finite type means dimπ Extβ (π΄, π΅) < β βπ΄, π΅.) For example, C = π· β (π΄-mod) where π΄ is finite-dimensional and of finite homological dimension. A Serre functor is a functor π : C β C and an isomorphism Hom(π΄, π΅) β Hom(π΅, π (π΄)) β . The Yoneda lemma implies that if π exists, it is unique. Example 25.5: For C = π· β (Coh(π )), π : πΉ β¦β πΉ β πΎπ₯ [π] is a Serre functor. per
The Hodge theorem can be restated as a claim that a spectral sequence HHβ (Coh(π )) =β HCβ (Coh(π )) degenerates for smooth projective π . The following striking generalization was proposed (in a slightly different form) by Kontsevich and Soibelman (see [11]). Conjecture 25.6: The above spectral sequence degenerates for any dg-category of finite type over π. This was partly proved by Dmitry Kaledin and Akhil Mathew, see [10], [14].
25.4
Artin-Schelter regular algebras and noncommutative projective geometry
A projective variety π β Pππ is determined by its homogeneous coordinate ring π΄, a graded commutative ring such that π = πππ π (π΄). An important invariant of π is the abelian category πΆπβ(π ) of coherent sheaves on π . It can ππ ππ ππ be realized as a Serre quotient π΄ β πππ π π /π΄ β πππ π π where π΄ β πππ π π is the category of finitely generated graded ππ π΄-modules and π΄ β πππ π π is the Serre subcategory of finite dimensional graded modules. One can study noncommutative graded ring that share basic features with commutative ones, thinking of them as homogeneous coordinate rings of (yet to be defined) noncommutative projective varieties. Some beautiful results in that direction were obtained by Artin, Schelter and others in 1990βs. So consider a nonnegatively graded algebras over a field π΄ = βπ΄π , π΄0 = π. Assuming π΄ is Noetherian, the category ππ ππ ππ π΄ β πππ π π is abelian, so one can consider π΄ β πππ π π /π΄ β πππ π π , the category of coherent sheaves on the purported noncommutative πππ π of π΄. One defines a point module over π΄ as a cyclic graded module with Poincare series 1/(1 β π‘). In the case when π΄ is commutative and generated by π΄1 point modules are in bijection with points of π = πππ π (π΄). Several important classification results are achieved by considering point modules and a usual (commutative) algebraic variety arising as the moduli space of point modules. We briefly mention a sample classification problem. Recall that a commutative π΄ as above has finite homological dimension (equivalently, is regular) iff it is a polynomial algebra. Assuming it is generated by π΄1 , we get the homogeneous coordinate ring of π = Pππ . Generalization of this simplest projective variety leads to the following definition. An algebra π΄ as above is called Artin-Schelter regular if it has finite homological dimension π, a finite GK dimension and πΈπ₯π‘π΄π (π, π΄) = 0 for π β π, while πΈπ₯π‘π΄π (π, π΄) is one dimensional. The work of Artin-Schelter and Artin-Tate-van den Bergh achieved classification of AS regular algebras of dimensions two and three (noncommutative projective lines and planes). We will not present the answer, but mention that it involves beautiful and rather elementary algebro-geometric data, such as an elliptic curve with an automorphism (see [17] and references therein), arising in the process of classification of point modules over π΄.
79
Index πΆπ field, 48
delta functor, 29 universal, 29 denominator set, 56 Density Theorem, 9 descending chain condition, 9 distributive lattice of subspaces, 34
Akizuki-Hopkins-Levitzki Theorem, 17 algebra bar complex, 37 exponential growth, 59 Gelfand-Kirillov dimension, 71 Hochschild (co)homology, 37 Koszul, 33 quadratic, 33 dual, 33 subexponential growth, 59 Veronese subalgebra, 33 Amitsur cohomology, 54 Amitsurβs Theorem, 69 Amitsur-Levitzki Theorem, 64 Anick Conjecture, 75 Artin-Wedderburn Theorem, 43 ascending chain condition, 9 associated graded, 11 Azumaya algebra, 52 Azumaya-Nakayama, 40
essential surjection, 17 formally smooth ring homomorphism, 53 functor adjoint, 26 equivalence of categories, 20 essentially surjective, 20 faithful, 20 fully faithful, 20 generator, 28 Goldieβs theorem, 59 Grothendieck group, 11 ideal
left, 5 right, 5 two-sided, 5 invariant basis number property, 5 isotypic component, 8
Berele Theorem, 73 Bergman gap Theorem, 72 Brauer group, 39 index of an element, 47 Brauer group of a ring, 52
Jordan-H¨older Theorem, 11
Capelli polynomial, 68 Cartan matrix, 30 categorical product, 21 category abelian, 28 additive, 27 filtered, 28 Grothendieck, 28 Cayley-Hamilton Theorem, 66 central simple algebra, 39 period, 47 Chevalley-Warning Theorem, 49 compact object, 28 composition series, 10 coproduct, 21 cosocle filtration, 12 cross-product algebra, 45 cross-product extension, 45
Kaplanskyβs Theorem, 66 Koszul complex, 33 Krull-Schmidt Theorem, 14 matrix algebra, 4 module, 4 Artinian, 10 bi-, 5 descent data, 53 essential, 60 essential complement, 60 free, 5 rank of a, 5 Gelfand-Kirillov dimension, 73 Goldie rank, 60, 61 indecomposable, 13 injective dimension, 30 irreducible, 6 length of a, 10 Noetherian, 10 projective, 17 projective cover of a, 17 projective dimension, 30
deformation formal, 38 nth order, 38 polynomial, 38 80
semisimple, 6 simple, 6 uniform, 60 Morita context, 24 Morita equivalence, 19 Morita context derived, 24
local, 13 localization at multiplicative subset, 56 Noetherian, 9 opposite, 4 polynomial identity, 63 prime, 59 primitive, 15 quotient, 5 semi-prime, 59 semi-primitive, 15 simple, 9 unital, 4 Rowenβs Theorem, 67
Ore conditions, 56 Ore domain, 58 Ore set, 56 Poincare series, 36 Polishchuk-Positselski Conjecture, 75 Posnerβs Theorem, 67 projective generator, 19
Schurβs Lemma, 6 Serre subcategory, 25 Skolem-Noether Theorem, 42 Smoktunowicz Theorem, 73 socle, 7 socle filtration, 12 Stephenson-Zhang Theorem, 74
Razmyslov polynomial, 68 reduced trace, 48 reduced norm, 48 regular element, 57 ring, 4 eΒ΄ tale homomorphism, 55 Artinian, 9 center of a, 22 cocenter of a, 22 division, 4 faithfully flat, 53 flat, 53 Goldie, 63 homological dimension, 30 Jacobson radical of a, 11
trace map, 23 universal abelian group for a, 23 Tsenβs Theorem, 49 Ufnarovskii graph, 73 Warfieldβs Theorem, 71 Wedderburnβs Theorem, 9 Yoneda Lemma, 21 References
[1] Michael Artin. Noncommutative Rings class notes. 1999. [2] Asher Auel, Eric Brussel, Skip Garibaldi, and Uzi Vishne. Transformation Groups, 16(1):219β264, 2011.
Open problems on central simple algebras.
[3] J. Backelin. On the rate of growth of the homologies of Veronese subrings. in Algebra, Algebraic Topology and their Interactions. J.-E. Roos ed., Lect. Notes Math., 1183, pp. 79β100, Springer-Verlag, Berlin/New York, 1986. [4] A.A. Beilinson, V.A. Ginzburg, and V.V. Schechtman. Koszul duality. Journal of Geometry and Physics, 5(3):317β 350, 1988. [5] Alexander Beilinson, Victor Ginzburg, and Wolfgang Soergel. Koszul Duality Patterns in Representation Theory. Journal of the American Mathematical Society, 9(2):473β527, 1996. [6] R. Bezrukavnikov. geom/9502021, 1995.
Koszul property and Frobenius splitting of Schubert varieties.
arXiv preprint alg-
[7] William Crawley-Boevey, Martin P. Holland. Noncommutative deformations of Kleinian singularities. Math. J. 92 (1998), no.3, 605β635. [8] Victor Ginzburg. Calabi-Yau algebras. arXiv:math/0612139. [9] Alexander Grothendieck. Sur quelques points dβalg`ebre homologique. Tohoku Mathematical Journal, 1957.
81
Duke
[10] D. Kaledin. Spectral sequences for cyclic homology. In Algebra, geometry, and physics in the 21st century, volume 324 of Progr. Math., pages 99β129. BirkhΒ¨auser/Springer, Cham, 2017. [11] Maxim Kontsevich and Yan Soibelman. Notes on A-infinity algebras, A-infinity categories and non-commutative geometry. I. arXiv preprint math/0606241 (2006). [12] GΒ¨unter R. Krause and Thomas H. Lenagan. Growth of Algebras and Gelfand-Kirillov Dimension. Number 22 in Graduate Studies in Mathematics. American Mathematical Society, 2000. [13] Saunders Mac Lane. Categories for the working mathematician. Number 5 in Graduate texts in mathematics. Springer-Verlag, 1971. [14] Akhil Mathew. Kaledinβs degeneration theorem and topological Hochschild homology. Geometry Topology 24.6 (2020): 2675-2708. [15] John McKay. Graphs, singularities, and finite groups. Proc. Symp. Pure Math. Vol. 37. No. 183. 1980 [16] Inamdar, S. P., Mehta, V. B. (1994). Frobenius splitting of Schubert varieties and linear syzygies. American Journal of Mathematics, 116 (6), 1569-1586. [17] Daniel Rogalski, Artin-Schelter Regular Algebras. arXiv:2307.03174, 2023. [18] Charles A. Weibel. An introduction to homological algebra. Number 38 in Cambridge studies in advanced mathematics. Cambridge Univ. Press, Reprint. 1997, transf. to digital print edition, 2003.
82
MIT OpenCourseWare https://ocw.mit.edu
18.706 Noncommutative Algebra Spring 2023
For information about citing these materials or our Terms of Use, visit: https://ocw.mit.edu/terms.