Physica status solidi. Subject and Author Index 1990: Physica Status Solidi (b) Basic research, Volumes 157 to 162. Physica Status Solidi (a) Applied research, Volumes 117 to 122 [Reprint 2021 ed.] 9783112483961, 9783112483954

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physica status solidi Cb) basic research

Volumes 157 to 162

Subject and Author Index 1990 Volumes 117 to 122

physica status solidi (a) applied research

AKADEMIE VERLAG ISSN 0370-1972/0031-8965 phys. stat. sol. (b)/(a), Berlin R23 (1990) 1 - 5 6 4

Substance Classification*) 51.

Transition metals and their alloys and compounds (for oxides, see S10) 51.1. Fe 51.2. Other 3d metals 51.3. Noble metals 51.4. Lanthanides 51.5. Actinides 51.61. Carbides, silicides, germanides 51.62. Nitrides, phosphides, arsenides 51.63. Sulfides, selenides, tellurides 52. Alkali metals and their alloys and compounds (for alkali halides, see S9.ll) 53. Alkaline earth metals and their alloys and compounds (for alkaline earth halides, see S9.12) 54. Other metals and their alloys 55. Nonmetallic elements 55.11. Silicon 55.12. Germanium S5.2 Solidified gases 56. Group IV compounds (for transition metal compounds, see SI.61) 57. Group V compounds (for transition metal compounds, see SI.62) S7.1. Ill—V compounds 57.11. Phosphides 57.12. Arsenides 57.13. Antimonides 57.15. Mixed crystals 57.16. Higher compounds 58. Chalcogenides (for transition metal compounds, see SI.63) S8.1. II—VI compounds 58.11. Sulfides 58.12. Selenides 58.13. Tellurides 58.15. Mixed crystals 58.16. Higher compounds 59. Halides 59.11. Alkali halides 59.12. Alkaline earth halides 59.15. Mixed crystals 59.16. Higher compounds 510. Oxides S10.1. Simple oxides SI0.15. Mixed crystals 511. Other higher compounds S11.1. Salts of oxy-acids SI 1.2. Spinels, garnets, ferrites 512. Organic compounds SI2.1. Quasi-one-dimensional systems

For comments on the use of the classification scheme see p. 13.

*) Outside the ICSTI Classification for Physics.

physica status solidi (b)

physica status solidi (a)

basic research

applied research

Board of Editors

Board of Editors

P. A I G R A I N , Paris, S. A M E L I N C K X , Mol-Donk, M. BALKANSKI, Paris, M. C A R D O N A , Stuttgart, W. DEKEYSER, Gent, W. F R A N Z , Münster. E. G U T S C H E , Berlin. R. KAISCHEW, Sofia, R. KUBO, Tokyo, P. T. L A N D S B E R G , S o u t h a m p t o n , S. L U N D Q V I S T , G ö t e b o r g , L. N É E L , Grenoble, L. PAL, Budapest, A. PIEKARA t , Warszawa, A. SEEGER, Stuttgart, F. SEITZ, New York, F. S T Ö C K M A N N , Karlsruhe, J. TAUC, Providence

S. A M E L I N C K X , Mol-Donk, J. A U T H , Berlin, H. BETHGE, Halle, K. W. BÖER, Newark, E. G U T S C H E , Berlin, P. HAASEN, Göttingen, G . M. H A T O Y A M A , Tokyo, B. T. K O L O M I E T S t , Leningrad, W. J. M E R Z , Zürich, G. O. M Ü L L E R , Berlin, A. SEEGER, Stuttgart, S. SHIONOYA, Tokyo, C. M. VAN VLIET, Montreal,

Editor-in-Chief

Editor-in-Chief

E. G U T S C H E

E. G U T S C H E

Advisory Board

Advisory Board

M. AVEROUS, Montpellier, P. C. BANBURY, Reading, M. B E R N A R D , Bagneux, W. BRAUER, Berlin, W. C O C H R A N , Edinburgh, R. COELHO, Gif-sur-Yvette, R. E N D E R L E I N , Berlin, W. HAUBENREISSER, Jena, G. JACOBS, Gent, H.-G. KAHLE, Karlsruhe. M. MATYÄS, Praha, H. D. M E G A W , Cambridge, E. N A G Y , Budapest, E. A. NIEKISCH, Jülich, H. M. R O S E N B E R G , Oxford, S. SHIONOYA, Tokyo, W. S T E I N M A N N , M ü n c h e n , H.-R. T R E B I N , S t u t t g a r t , I. M. TSIDILKOVSKII, Sverdlovsk, R. VAUTIER, Bellevue/Seine

L. N. A L E K S A N D R O V , Novosibirsk, W. A N D R Ä , Jena, H. BÄSSLER, Marburg, E. BAUER, Clausthal-Zellerfeld, G. C H I A R O T T I , Rom, H. C U R I E N , Paris, R. G R I G O R O V I C I , Bucharest, J. H E Y D E N R E I C H , Halle, F. B. H U M P H R E Y , Pasadena, A. A. K A M I N S K I I , Moskva, E. KLIER, Praha, Y. N A K A M U R A , Kyoto, J. N I H O U L , Mol, T. N . R H O D I N , Ithaca, New York, R. S I Z M A N N , München, J. STUKE, Marburg, J. T. W A L L M A R K , Göteborg

SUBJECT AND AUTHOR INDEX Volumes 157 to 162, 1990

Volumes 117 to 122, 1990

AKADEMIE VERLAG

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1991 by A k a d e m i e Verlag G m b H . Printed in the Federal R e p u b l i c of G e r m a n y .

A N ( E D V ) 20 831/20 735

Preface The twenty third index volume contains volumes 157 to 162 of "physica status solidi (b) — basic research" as well as volumes 117 to 122 of "physica status solidi (a) — applied research", i.e. all volumes having appeared in 1990 containing 1332 papers. Beginning from January 1986 the "International Classification System for Physics" (Condensed Matter, items 60 and 70) of the International Council for Scientific and Technical Information, Abstracting Board completed by item 85 and a Substance Classification (both outside the ICSTI Classification for Physics) will be used for quoting papers in physica status solidi. Nevertheless, before taking over these subject classifications into the index volume they were once more carefully revised and in some cases improved and completed in order to get a most uniform and clear classification for all papers. The average number of quotations per paper in this index volume is about 2.7. I have to express my thanks to the readers for their interest, and I will always readily take up any critical remarks and proposals for improvements. Berlin, August 1991 Karin Miiller

Contents International Classification System for Physics 6 Substance Classification (according to physica status solidi) 11 Some Comments on the Use of the Subject and Author Index 13 60. Condensed Matter: Structure, Mechanical, and Thermal Properties 17 61. Structure of Liquids and Solids; Crystallography 17 62. Mechanical and Acoustical Properties of Condensed Matter 63 63. Lattice Dynamics and Crystal Statistics 73 64. Equations of State, Phase Equilibria, and Phase Transitions 80 65. Thermal Properties of Condensed Matter 92 66. Transport Properties of Condensed Matter (Nonelectronic) 97 67. Quantum Fluids and Solids; Liquid and Solid Helium 103 68. Surfaces and Interfaces; Thin Films and Whiskers 104 70. Condensed Matter; Electronic Structure; Electrical, Magnetic, and Optical Properties 121 71. Electronic States 121 72. Electronic Transport in Condensed Matter 165 73. Electronic Structure and Electrical Properties of Surfaces, Interfaces, and Thin Films 186 74. Superconductivity 208 75. Magnetic Properties and Materials 222 76. Magnetic Resonances and Relaxation in Condensed Matter; Mossbauer Effect 246 77. Dielectric Properties and Materials 259 78. Optical Properties and Condensed-Matter Spectroscopy and Other Interactions of Matter with Particles and Radiation 266 79. Electron and Ion Emission by Liquids and Solids; Impact Phenomena . . . . 3 1 0 85. Devices 314 S. Substances 319 Author Index 475

International Classification System for Physics*) 60. Condensed matter : structure, mechanical and thermal properties 61. Structure of liquids and solids ; crystallography (see also 68.20. Solid surface structures, 71. Electron states) 61.10. X-ray determination of structures (for specific determinations, see 61.55 to 61.80) 61.12. Neutron determination of structures (for specific determinations, see 61.55 to 61.80) 61.14. Electron determination of structures (for specific determinations, see 61.55 to 61.80) 61.16. Other determination of structures (for specific determination, see 61.55 to 61.80) 61.20. Classical, semiclassical, and quantum theories of liquid structure (for electronic states, see 71 ; for liquid helium, see 67) 61.25. Studies of specific liquid structures 61.30. Liquid crystals 61.40. Amorphous and polymeric materials 61.50. Crystalline state (including molecular motions in solids) (for magnetic structure and spin systems, see 75.25) 61.55. Specific structures of elements and alloys 61.60. Specific structures of inorganic compounds 61.65. Specific structures of organic compounds 61.70. Defects in crystals (see also 61.80. Radiation damage, 62. Mechanical and acoustical properties, 71.55. Impurities and defect levels, 76.30. EPR of color centers and other defects, 78.50. Impurity and defect absorption in solids) 61.80. Radiation damage and other irradition effects (for techniques of structure determination, see 61.10 to 61.16; for electron and ion impact phenomena, see 79.20) 61.90. Other topics in structure of liquids and solids 62. Mechanical and acoustical properties of condensed matter (see also 61.70. Defects in crystals, 68.30. Surfaces and interfaces) 62.10. Mechanical properties of liquids (for viscosity of liquids, see also 66.20) 62.20. Mechanical properties of solids (related to microscopic structure) 62.30. Mechanical and elastic waves 62.40. Anelasticity, internal friction, and mechanical resonances For thermomechanical effects, see 65.70 For magnetomechanical effects, see 75.80 For piezoelectric effects, see 77.60 For elasto-optical effects, see 78.20 62.50. High-pressure and shock-wave effects in solids 62.60. Acoustical properties of liquids For lattice dynamics,¡phonons, see 63 For second sound in'quantum fluids, see 67.40 62.65. Acoustical properties of solids For magnetoacoustic effects in metals, see 75.80 For acoustoelectric effects, see 72.50 For acousto-optical effects, see 78.20 62.80. Ultrasonic relaxation (see also 74.30. Ultrasonic attenuation in superconductors) 62.90. Other topics in mechanical and acoustical properties of condensed matter *) Excerpt, reproduced with permission of International Council for Scientific and Technical Information (ICSTI).

Classification System

7

63. Lattice dynamics and crystal statistics (see also 65. T h e r m a l properties, 66.70. T h e r m a l conduction, 68.30. D y n a m i c s of surface and interface vibrations, 78.30. Infrared and R a m a n spectra) 63.10. General theory 63.20. P h o n o n s and vibrations in crystal lattices 63.50. Vibrational states in disordered systems 63.70. Statistical mechanics of lattice vibrations (see also 65. T h e r m a l properties of condensed matter, and 66.70. T h e r m a l conduction) 63.75. Statistical mechanics of displacive phase transitions F o r o r d e r - d i s o r d e r and statistical mechanics of model systems, see 64.60 F o r crystallographic aspects of polymorphic and o r d e r - d i s o r d e r t r a n s f o r m a t i o n s , see 61.50 63.90. Other topics in lattice dynamics and crystal statistics

64. E q u a t i o n s of state, phase equilibria, and phase transitions 64.10. General theory of equations of state and phase equilibria 64.30. Equations of state of specific substances (see also 65.70. T h e r m a l expansion) 64.60. General studies of phase transitions (for magnetic, superconducting, and q u a n t u m fluid critical p h e n o m e n a , see 75, 74, and 67, respectively) 64.70. Phase equilibria, phase transitions, a n d critical points of specific substances 64.75. Solubility, segregation, and mixing 64.80. O t h e r phase properties of systems 64.90. O t h e r topics in equations of state, phase equilibria, a n d phase transitions

65. T h e r m a l properties of condensed matter (see also 63. Lattice d y n a m i c s ; for t h e r m o d y n a m i c properties of q u a n t u m fluids, see 67.40; for thermal properties of solid helium, see 67.80) 65.20. Heat capacities of liquids 65.40. H e a t capacities of solids (for specific heat of superconductors, see 74.30; for specific heat of magnetic systems, see 75.40) 65.50. T h e r m o d y n a m i c properties and entropy 65.70. T h e r m a l expansion and thermomechanical effects (see also 64.30. Equations of state) F o r thermal conduction in nonmetallic liquids, see 66.60; for nonmetallic solids, see 66.70 F o r electronic thermal conduction, see 72.10 and 72.20 F o r thermal conductivity of superconductors, see 74.30 F o r pyroelectric and electrocaloric effects, see 77.70 65.90. O t h e r topics in thermal properties of condensed matter

66. T r a n s p o r t properties of condensed matter (nonelectronic) 66.10. D i f f u s i o n and ionic conduction in liquids 66.20. Diffusive m o m e n t u m transport (for viscosity of liquids, see also 62.10) 66.30. Diffusion in solids 66.60. T h e r m a l conduction in nonmetallic liquids (for thermal conduction in liquid metals, see 72.15) 66.70. Nonelectronic thermal conduction and heat-pulse p r o p a g a t i o n in nonmetallic solids (for thermal conduction in solid metals, see 72.15; for statistical mechanics of lattice vibrations, see 63.70) 66.90. Other topics in nonelectronic transport properties

8

Classification System

67. Q u a n t u m fluids a n d solids; liquid and solid helium 67.20. Q u a n t u m effects on the structure and dynamics of nondegenerate fluids 67.40. Boson degeneracy and superfluidity of helium-4 67.50. Fermi fluids; liquid helium-3 67.60. Mixed systems; liquid helium-3, -4 mixtures 67.70. Films (including physical a d s o r p t i o n ) 67.80. Solid helium a n d related q u a n t u m crystals 67.90. Other topics in q u a n t u m fluids (e.g., n e u t r o n - s t a r matter)

68. Surfaces and interfaces; thin films and whiskers (for impact p h e n o m e n a , see 79; for crystals growth, see 61.50) 68.10. Fluid surfaces and fluid-fluid interfaces 68.15. Liquid thin films 68.20. Solid surface structures 68.25. Mechanical and acoustical properties of solid surfaces and interfaces 68.30. D y n a m i c s of solid surfaces and interface vibrations 68.40. Surface energy of solids ; t h e r m o d y n a m i c properties 68.45. Solid-fluid interface processes 68.48. Solid-solid interfaces (including bicrystals) (for grain boundaries, see 61.70) 68.55. Thin film growth, structure, and epitaxy 68.60. Physical properties of thin films: nonelectronic 68.70. Whiskers and dendrites: growth, structure, and nonelectronic properties 68.90. Other topics in the structure and nonelectronic properties of surfaces and thin films

70. Condensed m a t t e r : electronic structure; electrical, magnetic, and optical properties 71. Electronic states (see also 63. Lattice dynamics, 73. Electronic structure and electrical properties of surfaces, interfaces, and thin films) 71.10. General theories and c o m p u t a t i o n a l techniques 71.20. Electronic density of states determinations (including energy states of liquid semiconductors) (see also 65.40. Electronic heat capacity) 71.25. Nonlocalized single-particle electronic states 71.30. M e t a l - i n s u l a t o r transitions 71.35. Excitons and related p h e n o m e n a (including electron-hole drops) 71.36. Polaritons (including p h o t o n - p h o n o n and p h o t o n - m a g n o n interactions) 71.38. P o l a r o n s a n d e l e c t r o n - p h o n o n interactions (see also 63.20, p h o n o n - e l e c t r o n interactions in lattices) 71.45. Collective effects 71.50. Localized single-particle electronic states (excluding impurities) 71.55. I m p u r i t y a n d defect levels 71.60. Positron states (see also 78.70. Positron annihilation) 71.70. Level splitting and interactions (see also 75.10. — in magnetic p h e n o m e n a , 75.30. Exchange and superexchange interactions, 73.20. Electronic surface states) 71.90. Other topics in electron states

Classification System

9

72. Electronic transport in condensed matter (for surfaces, interfaces, and thin films, see 73) 72.10. Theory o f electronic transport; scattering mechanism 72.15. Electronic conduction in metals and alloys 72.20. Conductivity phenomena in semiconductors and insulators (for nonelectronic conduction, see 66.70) 72.30. High-frequency effects; plasma effects 72.40. Photoconduction and photovoltaic effects; photodielectric effects 72.50. Acoustoelectric effects 72.55. Magnetoacoustic effects 72.60. Mixed conductivity and conductivity transitions 72.70. Noise processes and phenoma 72.80. Conductivity o f specific semiconductors and insulators 72.90. Other topics in electronic transport in condensed matter

73. Electronic structure and electrical properties o f surfaces, interfaces, and thin films 73.20. Electronic surface states (for emission and impact phenomena, see 79) 73.25. Surface conductivity 73.30. Surface double layers, Schottky barriers, and work functions 73.40. Interfaces 73.60. Electronic properties o f thin films 73.90. Other topics in electrical properties o f surfaces, interfaces, and thin films

74. Superconductivity 74.10. Occurrence, critical temperature 74.20. T h e o r y 74.30. General properties 74.40. Fluctuations and critical effects 74.50. Tunneling phenomena, Josephson effect, and proximity effects 74.55. Type-I superconductivity 74.60. Type-II superconductivity 74.70. Superconducting materials 74.90. Other topics in superconductivity

75. Magnetic properties and materials 75.10. General theory and models o f magnetic ordering (see also 71.25. Nonlocalized single-particle electronic states, 71.70. Level splitting and interactions) 75.20. Diamagnetism and paramagnetism 75.25. Spin arrangements in magnetically ordered materials (neutron studies, etc.) 75.30. Magnetically ordered materials, other intrinsic properties (for critical-point effects, see 75.40) 75.40. Critical-point effects, specific heats, short-range order (see also 65.40. Heat capacities) 75.50. Studies o f specific magnetic materials 75.60. D o m a i n effects, magnetization curves, and hysteresis 75.70. Magnetic films and plates 75.80. For For 75.90.

Magnetomechanical and magnetoelectric effects, magnetostriction galvanomagnetic effects, see 72.15 and 72.20 magneto-optical effects, see 78.20 Other topics in magnetic properties and materials

Classification System

10

76. Magnetic resonances and relaxation in condensed matter; Môssbauer effect 76.20. General theory of resonances and relaxation 76.30. Electron paramagnetic resonance and relaxation 76.40. Diamagnetic and cyclotron resonances 76.50. Ferromagnetic, antiferromagnetic, and ferrimagnetic resonances; spin-wave resonance (see also 75.30. Spin waves) 76.60. Nuclear magnetic resonance and relaxation 76.70. Magnetic double resonances and cross effects 76.80. Môssbauer effect; other y-ray spectroscopy 76.90. Other topics in magnetic resonances and relaxation 77. Dielectric properties and materials (for conductivity phenomena, see 72.20 and 72.80) 77.20. Permittivity 77.30. Polarization and depolarization effects 77.40. Dielectric loss and relaxation 77.50. Dielectric breakdown and space-charge effects 77.55. Dielectric thin films 77.60. Piezoelectricity and électrostriction (for piezo-optical effects, see 78.20) 77.70. Pyroelectric and electrocaloric effects 77.80. Ferroelectricity and antiferroelectricity 77.85. Electrical resonances 77.90. Other topics in dielectric properties and materials 78. Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation (for phonon spectra, see 63) 78.20. Optical properties and materials 78.30. Infrared and Raman spectra and scattering 78.35. Brillouin and Rayleigh scattering 78.40. Visible and ultraviolet spectra 78.45. Stimulated emission 78.50. Impurity and defect absorption in solids 78.55. Photoluminescence 78.60. Other luminescence and radiative recombination For photoconduction and photovoltaic effects, see 72.40 78.65. Optical properties of thin films 78.70. Other interactions of matter with particles and radiation 78.90. Other topics in optical properties of condensed matter and other interactions of matter with particles and radiation 79. Electron and ion emission by liquids and solids; impact phenomena 79.20. Impact phenomena, including electron spectra and sputtering 79.40. Thermoionic emission 79.60. Photoemission and photoelectron spectra 79.70. Field emission and field ionization 79.75. Exoelectron emission 79.80. Resonance tunneling 79.90. Other topics in emission and impact phenomena in condensed matter 85. Devices*) *) Outside the ICSTI Classification for Physics.

Classification System

Substance Classification (according to physica status solidi)*) 51.

Transition metals and their alloys and compounds (for oxides, see S10) 51.1. Fe 51.2. Other 3d metals 51.3. Noble metals 51.4. Lanthanides 51.5. Actinides 51.61. Carbides, silicides, germanides 51.62. Nitrides, phosphides, arsenides SI .63. Sulfides, selenides, tellurides

52.

Alkali metals and their alloys and compounds (for alkali halides, see S9.11)

53.

Alkaline earth metals and their alloys and compounds (for alkaline earth halides, see S9.12)

54.

Other metals and their alloys

55.

Nonmetallic elements 55.11. Silicon 55.12. Germanium S5.2. Solidified Gases

56.

Group IV compounds (for transition metal compounds, see S 1.61)

57.

Group V compounds (for transition metal compounds, see SI.62) S7.1. Ill—V compounds 57.11. Phosphides 57.12. Arsenides 57.13. Antimonides 57.15. Mixed crystals 57.16. Higher compounds

58.

Chalcogenides (for transition metal compounds, see SI.63) S8.1. II—VI compounds 58.11. Sulfides 58.12. Selenides 58.13. Tellurides 58.15. Mixed crystals 58.16. Higher compounds

59.

Halides 59.11. Alkali halides 59.12. Alkaline earth halides 59.15. Mixed crystals 59.16. Higher compounds

S10. Oxides S10.1. Simple oxides S 10.15. Mixed crystals SI 1. Other higher compounds SI 1.1. Salts of oxy-acids SI 1.2. Spinels, garnets, ferrites SI2. Organic compounds S12.1 Quasi-one-dimensional systems *) Outside the ICSTI Classification for Physics.

11

Some Comments on the Use of the Subject and Athor Index

13

Some Comments on the Use of the Subject and Author Index The "International Classification System for Physics" (the condensed matter items 60 and 70) completed by item 85 and a Substance Classification (according to physica status solidi) is used. On cover two the second-level headings of the condensed matter items and on pages 6 to 10 the third-level headings are reproduced. As a help for using the subject index on pages 14 and 15 in addition also a series of important fourth-level headings is given. The substance classification is published on cover three and on page 11. All papers will be quoted under each relevant section. There is made a distinction between one or two principal entries (refering to the main subject matter of the paper) and secondary entries (refering to subsidiary subject matter and substance, respectively). On the line following the title the subject classification is given in the same manner as in the volumes. Each entry gives the volume, the number of the issue, the initial and final page numbers. A paper of physica status solidi (b) or physica status solidi (a) is marked by (b) or (a) in front of the line, respectively. The letter " K " before the page numbers indicates a short note published in the offset part of the journal. The entries for review articles, original papers, short notes, and errata are made together in a single list for each subject. These are ordered according to data of publication, irrespective of being a paper of physica status solidi (b) or physica status solidi (a). Original papers are sometimes published in several parts under the same principal title (in general with special subtitles). The various parts of papers of this type are treated separately and each part is classified according to its particular contents. The author index gives the names of the authors in alphabetical order. Each name is followed by the bibliographic details of the paper. A paper of physica status solidi (b) or physica status solidi (a) is again marked by (b) or (a) in front of the number of the volume, respectively. In the last column the subject classification of the paper is presented in the same manner as in the volumes. When several papers have been published by the same author they are arranged according to data of publication, irrespective of being a paper of physica status solidi (b) or physica status solidi (a). To find a paper of your interest please choose first the special entry of the subject index and then use the volume number and page.

14

Some Comments on the Use of the Subject and Author Index

In using the subject index attention should be given to the following details: 61.10. to 61.16. Theory and experimental techniques of determination of structures — for specific determinations see 61.55 to 61.80 61.16. Other determination of structures — electron microscopy and field-ion microscopy determinations — EPR and N M R determinations 61.25. Studies of specific liquid structures — macromolecular and polymer solutions — molten salts — liquid metals 61.40. Amorphous and polymeric materials — glasses, polymers, elastomers, plastics 61.50. Crystalline state (including molecular motions in solids) — physics of crystal growth — crystal symmetry: models, space groups, crystalline systems and classes — crystal morphology and orientation — crystallographic aspects of polymorphic and order-disorder transformations 61.70. Defects in crystals — grain and twin boundaries — stacking faults and other planar or extended defects — doping and implantation of impurities — impurity concentration, distribution, and gradients 61.80. Radiation damage and other irradiation effects — channeling, blocking, energy loss of particles — X-rays, y-rays, electrons and positrons, neutrons, atoms and molecules, ions — for ion implantation see 61.70 63.20. Phonons and vibrations in crystal lattices — phonon-phonon, phonon-electron, and phonon-defect interactions 64.60. General studies of phase transitions — order-disorder and statistical mechanics of model systems — equilibrium properties near single critical points, critical exponents — dynamic critical phenomena — multicritical points — metastable phases 64.80. Other phase properties of systems — stoichiometry and homogeneity — microstructure 66.30. Diffusion in solids — theory of diffusion and ionic conduction in solids — self-diffusion and ionic conduction in non-metals — diffusion, migration, and displacement of impurities and other defects 71.25. Nonlocalized single-particle electronic states — techniques of band-structure calculation — measurements of Fermi surface parameters (including dHvA, magnetoacoustic, positron annihilation, and cyclotron resonance studies, etc.) — effective mass and g-factors — band structure of crystalline metals, semiconductors, and insulators 71.45. Collective effects — exchange, correlation, dielectric and magnetic functions, plasmons — Fermi-Thomas models — calculations of total electronic binding energy 71.70. Level splitting and interactions — crystal and ligand fields — spin-orbit coupling, Zeeman, Stark, and strain splitting — exchange interactions — nuclear states and interactions

Some Comments on the Use of the Subject and Author Index

15

72.10. Theory of electronic transport; scattering mechanism — general formulation of transport theory — scattering by phonons, magnons, and other nonlocalized excitations — scattering by point defects, dislocations, surfaces, and other imperfections (including Kondo effect) 72.15. Electronic conduction in metals and alloys — galvanomagnetic and other magnetotransport effects — thermomagnetic and thermoelectric effects — collective modes — scattering mechanism and Kondo effect 72.20. Conductivity phenomena in semiconductors and insulators — scattering mechanism — piezoresistance — galvanomagnetic and other magnetotransport effects — thermomagnetic and thermoelectric effects 73.40. Interfaces — contact resistance, contact potential, rectification — tunneling: general — p-n junctions — MIS, MIM, MSM, SIS, and SMS structures 75.30. Magnetically ordered materials, other intrinsic properties — saturation moments and magnetic susceptibility — spin waves — exchange and superexchange interactions — anisotropy — magnetic impurity interactions — magnetic phase boundaries — magnetocaloric effect 75.50. Studies of specific magnetic materials — ferromagnetism — antiferromagnetics, ferrimagnetics — amorphous magnetic materials — magnetic liquids 75.60. Domain effects, magnetization curves, and hysteresis — high coercitivity materials — fine-particle systems — magnetic aftereffects — magnetic annealing and temperature-hysteresis effects 78.20. Optical properties and materials — general theory — optical constants and parameters — optical rotatory power — birefringence — piezo-, elasto-, acousto-, electro-, magneto-, and thermo-optical effects 78.60. Other luminescence and radiative recombination — electroluminescence — cathodo- and iono-luminescence — thermoluminescence — sono- and tribo-luminescence — chemiluminescence 78.70. Other interactions of matter with particles and radiation — positron annihilation — X-ray scattering, absorption, and emission — microwave and radiofrequency (including resonances) 79.20. Impact phenomena, including electron spectra and sputtering — electron impact: Auger and secondary emission — atom, molecule, and ion impact — atomic and molecular beam interactions

Subject Index 60. Condensed Hatter: Structure, Mechanical, and Thermal Properties 61. Structure of Liquids and Solids; Crystallography (see also 68.20. Solid surface structures, 71. Electron states) 61.10. X-ray determination of structures (for specific determinations, see 61.55 to 61.80) S. MATTHIES, K. HELMING, and K. KUNZE On the Representation of Orientation Distributions in Texture Analysis by sigma-Sections. I. General Properties of ... 61.10; 61.12; 61.14 (b) Vol.157,No.1, 71-84 V. GEIST, D. STEPHAN, and D. FINK The Effect of the Lateral and Longitudinal Spread of Fast Protons on Strain Production in GaP and GaAs 61.10 and 61.80; S7.ll; S7.12 (a) Vol.117,No.1, 67-72 S.K. PLACHKOVA, L.E. SHELIMOVA, and O.G. KARPINSKII X-Ray Study of the Structural Phase Transitions in Ge 1 _ x Ag x y 2 B: '-x/2 Te Solid Solutions 64.70; 61.10; S8 (a) Vol.117,No.1, 155-162 S. MATTHIES, K. HELMING, and K. KUNZE On the Representation of Orientation Distributions in Texture Analysis by sigma-Sections. II. Consideration of Crystal ... 61.10; 61.12; 61.14 (b) Vol.157,NO.2, 489-508 A.M. AFANASEV, S.S. FANCHENKO, and A.V. MASLOV On the Equivalent Strain and Damage Distributions of Thin Subsurface Layers in the Triple-Crystal X-Ray Diffractometry 61.10; 68.20 (a) Vol.117,No.2, 341-350 A.O. ABOYAN, A.A. KHZARDZHYAN, P.A. BEZIRGANYAN, and S.E. BEZIRGANYAN X-Ray Interferometric Pictures of Dislocations 61.10 and 61.70 (a) Vol.118,No.1, 11-20

2 physica, Reg.-Bd. 23

Subject Index 60. Condensed Hatter: Structure, Mechanical, and Thermal Properties 61. Structure of Liquids and Solids; Crystallography (see also 68.20. Solid surface structures, 71. Electron states) 61.10. X-ray determination of structures (for specific determinations, see 61.55 to 61.80) S. MATTHIES, K. HELMING, and K. KUNZE On the Representation of Orientation Distributions in Texture Analysis by sigma-Sections. I. General Properties of ... 61.10; 61.12; 61.14 (b) Vol.157,No.1, 71-84 V. GEIST, D. STEPHAN, and D. FINK The Effect of the Lateral and Longitudinal Spread of Fast Protons on Strain Production in GaP and GaAs 61.10 and 61.80; S7.ll; S7.12 (a) Vol.117,No.1, 67-72 S.K. PLACHKOVA, L.E. SHELIMOVA, and O.G. KARPINSKII X-Ray Study of the Structural Phase Transitions in Ge 1 _ x Ag x y 2 B: '-x/2 Te Solid Solutions 64.70; 61.10; S8 (a) Vol.117,No.1, 155-162 S. MATTHIES, K. HELMING, and K. KUNZE On the Representation of Orientation Distributions in Texture Analysis by sigma-Sections. II. Consideration of Crystal ... 61.10; 61.12; 61.14 (b) Vol.157,NO.2, 489-508 A.M. AFANASEV, S.S. FANCHENKO, and A.V. MASLOV On the Equivalent Strain and Damage Distributions of Thin Subsurface Layers in the Triple-Crystal X-Ray Diffractometry 61.10; 68.20 (a) Vol.117,No.2, 341-350 A.O. ABOYAN, A.A. KHZARDZHYAN, P.A. BEZIRGANYAN, and S.E. BEZIRGANYAN X-Ray Interferometric Pictures of Dislocations 61.10 and 61.70 (a) Vol.118,No.1, 11-20

2 physica, Reg.-Bd. 23

Subject Index

18

A.O. ABOYAN, P.A. BEZIRGANYAN, and A.A. KHZARDZHYAN Study of X-Ray Diffraction Pictures of Crystal Imperfections by Means of Triple Interferometer 61.10

(a) Vol.118,No.1, 21-28

M. ERMRICH and H. HERMANN Microabsorption Correction in Quantitative Phase Analysis. Experimental Results 61.10; 61.50 (a) Vol.118,No.1, K1-K4 H. SCHAEBEN, H. SIEMES, and S. AUERBACH Entropy Optimization in Texture Goniometry. II. Practical Applications 61.50; 61.10; 61.12 (b) Vol.158,No.2, 407-426 N.M. OLEKHNOVICH and A.V. PUSHKAREV Birefringence and Depolarization Effects of X-Ray Scattering in Laue Geometry for Highly Distorted Crystals 61.10; 61.70; S9.ll (a) Vol.119,No.1, 27-34 A. CATICHA and S. CATICHA-ELLIS Dynamical Diffraction of X-Rays by Thin Crystals at Bragg Angles near TT/2 61.10; SI.2 (a) Vol.119,No.1, 47-54 A. CATICHA and S. CATICHA-ELLIS A Fabry-Perot Interferometer for Hard X-Rays 61.10 and 78.70 (a) Vol.119,No.2, 643-654 P. ZAUMSEIL and U. WINTER Characterization of Boron Implanted Silicon by X-Ray Triple-Crystal Diffractometry 61.10 and 61.70; S5.il (a) Vol.120,No.1, 67-76 V.V. ARISTOV, V.N. MORDKOVICH, A.YU. NIKULIN, A.A. SNIGIREV, U. WINTER, YU.N. EROKHIN, and P. ZAUMSEIL Possibilities of X-Ray Interference Diffractometry for the Investigation of Ion-Doped Layers 61.10 and 61.70; S5.ll (a) Vol.120,No.1, K1-K6

6 1 . 1 0 . X - r a y d e t e r m i n a t i o n of

structures

N . N . F A L E E V , L . I . F L A K S , S.G. K O N N I K O V , I.K. S O L O M I N , and S.V. BATASHOVA T h e I n f l u e n c e of t h e D i r e c t e d D i s p l a c e m e n t of A t o m i c P l a n e s the X-Ray Diffraction Rocking Curves 61.10 and 68.55; S7.12; S7.15 (a) V o l . 1 2 0 , N o . 2 , 3 2 7 - 3 3 8 0.

PACHER0VÂ T h e C a l c u l a t i o n of t h e C o p l a n a r F o u r - B e a m X - R a y Diffraction 61.10; S5.12 (a) V o l . 1 2 0 , N o . 2 , 3 3 9 - 3 5 0

on

Dynamical

V . I . K H R U P A , D . O . G R I G O R E V , V . V . N I K O L A E V , L.I. D A T S E N K O , and V.B. MOLODKIN I n f l u e n c e of D e f e c t s o n t h e T h i c k n e s s D e p e n d e n c e s of I n t e g r a l R e f l e c t i v i t y of D i s l o c a t i o n - F r e e S i l i c o n C r y s t a l s 61.10 and 61.70; S5.ll (a) V o l . 1 2 1 , N o . 1 , 11-20 M. G U Y M O N T , A. T O M A S , M . J U L I E N - P O U Z O L , S. J A U L M E S , and M. GUITTARD S t r u c t u r e a n d V a c a n c y O r d e r i n g in C u 2 E r 2 ^ 3 ^ 2 * E l e c t r o n a n d X - R a y D i f f r a c t i o n a n d H i g h R e s o l u t i o n E l e c t r o n M i c r o s c o p y ... 6 1 . 6 0 ; 6 1 . 1 0 ; S8 (a) V o l . 1 2 1 , N o . 1 , 21-28 E.L.

GARTSTEIN M u l t i b e a m C a l c u l a t i o n of t h e I n t e n s i t y D i s t r i b u t i o n for a n I m p e r f e c t C r y s t a l in L a u e G e o m e t r y 6 1 . 1 0 ; 6 1 . 7 0 ; S7.12 (a) V o l . 1 2 1 , N o . 1 , 37-44

E.A. K O N D R A S H K I N A , D.V. N O V I K O V , a n d S . A . S T E P A N O V S t u d y of X - R a y S u r f a c e B a c k D i f f r a c t i o n . R e c o r d i n g of a Diffracted Beam 6 1 . 1 0 ; 6 8 . 2 0 ; S5.12 (a) V o l . 1 2 1 , N o . 1 , K 9 - K 1 4 M.YA. GAMARNIK S i z e C h a n g e s of L a t t i c e P a r a m e t e r s in U l t r a d i s p e r s e and Silicon 61.55; 61.10; S5; S5.ll (b) V o l . 1 6 1 , N o . 2 , 4 5 7 - 4 6 2 D. W A N G a n d P.D. B R I S T O W E C a l c u l a t i o n of D i f f r a c t i o n E f f e c t s D u e t o D o u b l e i n (111) G o l d B i c r y s t a l s 6 1 . 7 0 ; 6 1 . 1 0 ; SI.3 (b) V o l . 1 6 1 , N o . 2 , 501-512

Diamond

Positioning

Subject

20

C. L A N D R O N , D. R U F F I E R , B. D U B O I S , P. O D I E R , D. B O N N I N , a n d H. D E X P E R T E t u d e p a r E X A F S d u r ô l e d e s p r é c u r s e u r s d a n s la s y n t h è s e Zr02-Y203 61.10 a n d 6 1 . 5 5 ; S 1 0 . 1 5 (a) V o l . 1 2 1 , N o . 2 , 3 5 9 - 3 6 8 K . W O K U L S K A , J. H A E R T W I G , a n d S. G R O S S W I G T h e B o n d M e t h o d U s e d t o D e t e r m i n e t h e V a l u e of t h e Parameters a for alpha-Fe 68.70; 61.10; Sl.l (a) V o l . 1 2 1 , N o . 2 , 5 3 9 - 5 4 6

Index

de

Lattice

P. Z A U M S E I L , U. W I N T E R , I.A. V A R T A N Y A N T S , a n d I.YU. K H A R I T O N O V Comparison between Two X-Ray Methods for Deformation Profile Determination 61.10; S5.ll (a) V o l . 1 2 1 , N o . 2 , K 1 4 9 - K 1 5 4 E.Z. A R S H A K Y A N a n d A . O . A B O Y A N I n v e s t i g a t i o n of I n t e r n a l S t r e s s e s in S i l i c o n S e m i c o n d u c t o r C r y s t a l s in C o n s t a n t E l e c t r i c a n d M a g n e t i c F i e l d s by M e a n s . . 61.10 (a) V o l . 1 2 2 , N o . 1 , 43-50 V . G . B A R Y S H E V S K I I a n d S.A. S T E P A N O V E f f e c t of T w o C r i t i c a l A n g l e s of X - R a y S u r f a c e D i f f r a c t i o n Secondary Emission Yield 61.10 a n d 7 8 . 7 0 ; 68.20 (a) V o l . 1 2 2 , N o . 1 , 69-72

on

V.L. INDENBOM and V.M. KAGANER X - R a y A n a l y s i s of I n t e r n a l S t r e s s e s i n C r y s t a l s . II. L a t t i c e D i s t o r t i o n s D u e t o R e s i d u a l S t r a i n s i n C r y s t a l s G r o w n ... 6 1 . 7 0 ; 61.10 (a) V o l . 1 2 2 , N o . 1 , 9 7 - 1 1 0 V.I. KUSHNIR and E.V. SUVOROV X-Ray Backscattering on Perfect 7 8 . 7 0 ; 6 1 . 1 0 ; S 5 . l l ; S5.12 (a) V o l . 1 2 2 , N O . 1 , 391-404

Crystals

V . H O L Y , J . K U B E N A , a n d K. P L O O G X - R a y A n a l y s i s of S t r u c t u r a l D e f e c t s in a Superlattice 61.10 a n d 6 1 . 7 0 ; S7.12 (b) V o l . 1 6 2 , N o . 2 , 3 4 7 - 3 6 2

Semiconductor

61.10. X - r a y d e t e r m i n a t i o n of

structures

V.I. PUNEGOV, A . P . PETRAKOV, a n d N.A. T I K H O N O V X-Ray Diffraction on Laser Disturbed Near-Surface Layers 61.10; S 5 . l l (a) V o l . 1 2 2 , N o . 2 , 449-458

Crystal

A.M. A F A N A S E V a n d O.G. M E L I K Y A N A M o d i f i e d D y n a m i c a l T h e o r y (MDT) of X - R a y D i f f r a c t i o n Extremely Asymmetric Schemes 61.10 (a) V o l . 1 2 2 , N o . 2 , 459-468 P. YANG, S.-S. J I A N G , a n d D. FENG T h e B e h a v i o u r of t h e First Fringes in t h e X - R a y T o p o g r a p h s of P l a n a r Defects. I. G e n e r a l C a s e 61.10 a n d 61.70 (a) V o l . 1 2 2 , N o . 2 , 475-480

in

Diffraction

C. B O U L E S T E I X , Z.C. RANG, P. A U D I B E R T , S. N I T S C H E , a n d O. M O N N E R E A U E v o l u t i o n of B i S r C a C u O (2212) S a m p l e s by A i r E x p o s u r e , S h o w i n g a D r a s t i c C h a n g e of M o d u l a t i o n V e r y L i k e l y D u e to W a t e r . . 61.10; S 1 0 . 1 5 (a) V o l . 1 2 2 , N o . 2 , K101-K104

61.12. N e u t r o n d e t e r m i n a t i o n of s t r u c t u r e s (for specific determinations, see 61.55

to

61.80)

S. M A T T H I E S , K. H E L M I N G , a n d K. K U N Z E O n t h e R e p r e s e n t a t i o n of O r i e n t a t i o n D i s t r i b u t i o n s in T e x t u r e A n a l y s i s by s i g m a - S e c t i o n s . I. G e n e r a l P r o p e r t i e s of ... 61.10; 61.12; 61.14 (b) V o l . 1 5 7 , N o . 1 , 71-84 S. M A T T H I E S , K. HELMING, a n d K. K U N Z E O n t h e R e p r e s e n t a t i o n of O r i e n t a t i o n D i s t r i b u t i o n s in T e x t u r e A n a l y s i s by s i g m a - S e c t i o n s . II. C o n s i d e r a t i o n of C r y s t a l ... 61.10; 61.12; 61.14 (b) V o l . 1 5 7 , N o . 2 , 489-508 P.S. GOYAL, R. C H A K R A V A R T H Y , B.A. D A S A N N A C H A R Y A , S.K. K U L S H R E S H T H A M . S . SASTRY, a n d J. T O M K I N S O N N e u t r o n I n c o h e r e n t I n e l a s t i c Scattering from (NH.) R b 1 _ v H , P O . 64.60; 61.12; Sll (b) V o l . 1 5 7 , N o . 2 , 547-556 H. SCHAEBEN, H. SIEMES, a n d S. A U E R B A C H E n t r o p y O p t i m i z a t i o n in T e x t u r e G o n i o m e t r y . II. Applications 61.50; 61.10; 61.12 (b) V o l . 1 5 8 , N o . 2 , 407-426

Practical

22

Subject Index

G.R. AUGST and YU.I. VLADISLAVSKII A Theoretical Study of Diffuse Scattering by Clusters in Alkali Halides 61.12 and 61.70; S9.ll (b) Vol.160,No.1, 71-82

61.14. Electron determination of structures (for specific determinations, see 61.55 to 61.80)

S. MATTHIES, K. HELMING, and K. KUNZE On the Representation of Orientation Distributions in Texture Analysis by sigma-Sections. I. General Properties of ... 61.10; 61.12; 61.14 (b) Vol.157,No.1, 71-84 J.G. WEN and R. WANG Two-Beam Dynamical Theory of the Displacement and Splitting of Diffraction Fringes Caused by a Stacking Fault 61.14 and 61.70; S5 (a) Vol.117,No.1, 73-84 S. MATTHIES, K. HELMING, and K. KUNZE On the Representation of Orientation Distributions in Texture Analysis by sigma-Sections. II. Consideration of Crystal ... 61.10; 61.12; 61.14 (b) Vol.157,No.2, 489-508 E. TAMURA, R. FEDER, G. WALLER, and U. GRADMANN Determination of the Surface Magnetization of Fe(110) by Spin-Polarized Low-Energy Electron Diffraction 68.20 and 75.30; 61.14; Sl.l (b) Vol.157,No.2, 627-634 N.A. SEMIKOLENOVA, V.A. BOGDANOVA, and A.S. SEMIKOLENOV The Ordering Phenomenon in the Highly Doped III-V Semiconductor Materials 61.14; S7.1 (a) Vol.120,No.2, K121-K124 R.K. KARAKHANYAN, P.L. ALEKSANYAN, and Y.K. MANUCHAROVA On Electron Double Diffraction in the Formation of Kikuchi Patterns 61.14; S5.ll (a) Vol.121,No.1, K1-K4 N.I. BORGARDT and W. SCHROETER Effect of Defocusing on Black-and-white Contrast of Small Defects 61.14 and 61.70 (a) Vol.121,No.2, 369-382

61.14. E l e c t r o n d e t e r m i n a t i o n of

23

structures

R. PEREZ O n t h e C h a r a c t e r i z a t i o n of C r y s t a l l i n e D e f e c t s U s i n g C B E D Techniques 61.14 a n d 61.70; SI.3; S5.ll (a) V o l . 1 2 2 , N o . 1 , 51-68 M. M A E D E R , J. R I C H T E R , a n d A. ZEHE S u r f a c e R e o r d e r i n g of (111)Si 7x7 to lxl R e c o n s t r u c t i o n In-Situ Annealing 6 8 . 2 0 ; 6 1 . 1 4 ; S5.ll (a) V o l . 1 2 2 , N o . 2 , K133-K134

61.16. O t h e r d e t e r m i n a t i o n of s t r u c t u r e s (for specific determinations, see 61.55

to

during

61.80)

T. K A M I N O , M. T O M I T A , I. OHTSUKA, a n d H. SAKA High Resolution Transmission Electron Microscopy Observation of t h e M o t i o n of a Surface D i s l o c a t i o n o n a G o l d P a r t i c l e 6 1 . 1 6 ; 61.70; SI.3 (a) V o l . 1 2 2 , N o . 2 , K105-K108 W. G R U E N E W A L D a n d J. U L L M A N N Cross-Sectional Transmission Electron Microscopy I n v e s t i g a t i o n s of R F - S p u t t e r e d a - C Films 68.55; 61.16; 6 8 . 6 0 ; S5 (a) V o l . 1 2 2 , N o . 2 , K129-K132

61.20. C l a s s i c a l , semiclassical, and q u a n t u m t h e o r i e s of liquid structure (for electron states, see 71; for liquid helium, see 67) R.V. G O P A L A R A O a n d R. V E N K A T E S H T h e o r e t i c a l M e t h o d of E v a l u a t i o n of H e a t s of V a p o r i s a t i o n of F u s e d Salts 61.20; 65.50; S9.ll (b) V o l . 1 5 7 , N o . 1 , 65-70 YU.M. M I S H I N a n d I.M. R A Z U M O V S K I I A M o d e l of M e t a l M e l t i n g and P r e m e l t i n g 61.20 a n d 61.70; 61.50 (a) V o l . 1 1 7 , N o . 1 , 91-98 T. DAS, L.B. BHUIYAN, a n d R.N. J O A R D E R A s h c r o f t - L a n g r e t h P r e s c r i p t i o n for E f f e c t i v e Core D i a m e t e r Liquids: A Variational Analysis 61.20; S2; S5.2 (b) V o l . 1 6 1 , N o . 2 , 473-482

in

Subject

24

61.25. S t u d i e s of s p e c i f i c liquid

Index

structures

A. D E R O U I C H E a n d J.L. B R E T O N N E T T h e L o n g - W a v e l e n g t h L i m i t of the S t r u c t u r e F a c t o r of L i q u i d Alkali Metals Using a One-Component Plasma System 61.25; 65.50; S2 (b) V o l . 1 5 7 , N o . 1 , 61-64 A.K. M I S H R A , B.B. SAHAY, a n d K.K. M U K H E R J E E S t r u c t u r e a n d E l e c t r i c a l R e s i s t i v i t y of A l k a l i - A l k a l i L i t h i u m - B a s e d L i q u i d Binary A l l o y s 61.25; 7 2 . 1 5 ; S2 (b) V o l . 1 5 7 , N o . 1 , 85-92

and

T. DAS, T. N A M M A L V A R , L.B. BHUIYAN, a n d R.N. J O A R D E R C o m p u t a t i o n of V a c a n c y F o r m a t i o n E n e r g y of L i q u i d M e t a l s 61.25; 61.70; S2; S4 (b) V o l . 1 5 7 , N o . 1 , 93-100 R.V. G O P A L A R A O a n d U. BANDYOPADHYAY A p p l i c a t i o n of t h e O n e - C o m p o n e n t P l a s m a A p p r o x i m a t i o n to S t r u c t u r a l S t u d i e s of Like C h a r g e s in M o l t e n S a l t s 61.25; S9.12 (a) V o l . 1 1 8 , N o . 2 , 365-370 R.V. G O P A L A R A O a n d A. C o m p u t a t i o n of t h e Sb, Bi, Ga, a n d Sn 61.25; S4 (b) V o l . 1 5 9 , N o . 2 ,

SATPATHY S t r u c t u r e F a c t o r s of the P e c u l i a r M e t a l s U s i n g L e b o w i t z s S o l u t i o n of H a r d - S p h e r e ... 545-550

O. A K I N L A D E A Study of t h e S t r u c t u r e and T h e r m o d y n a m i c s of L i q u i d M e t a l s B a s e d o n Some R e f e r e n c e Systems 61.25 a n d 65.50; S2; S3; S4 (b) V o l . 1 6 1 , N o . 1 , 75-84

61.40. A m o r p h o u s a n d p o l y m e r i c m a t e r i a l s Y.F. C H E N a n d C.K. W O N G M i c r o s c o p i c M o d e l of M e t a s t a b l e C h a n g e s in H y d r o g e n a t e d Amorphous Silicon 61.40; S 5 . l l (b) V o l . 1 5 7 , N o . 1 , 101-106 A.

CZACHOR Locally Compensated Orderless 61.40 a n d 61.50 (b) V o l . 1 5 7 , N o . 1 , K1-K6

Structures

61.40. Amorphous and polymeric

materials

V. S R E E R A M A L U , V . R A V I N D R A C H A R Y , H . R . S R E E P A D , A . C H A N D R A S H E K A R A , S. G O P A L , H. S A N J E E V A I A H , a n d B. V I S W A N A T H A N S t r u c t u r a l R e l a x a t i o n a n d C r y s t a l l i z a t i o n of M e t a l l i c G l a s s e s F e 3 5 C o 5 2 v i 3 an2 L a y e r s in H i g h - T c Superconductors 7 4 . 2 0 a n d 74.70 (b) V o l . 1 6 1 , N o . 2 , K 9 5 - K 9 8

R. H E I D I N G E R , H. A P P E L , G. T H E N , a n d W . - G . T H I E S O b s e r v a t i o n of R a d i a t i o n D a m a g e in H f V 2 a n d Its H y b r i d e s TDPAC 6 1 . 8 0 ; 6 4 . 8 0 ; 7 4 . 7 0 ; 7 6 . 8 0 ; SI.2 (a) V o l . 1 2 1 , N o . 2 , 445-454 HONG

ZHANG P o s i t r o n T r a p p i n g in Y B a 2 C u 3 _ x F e x O , 74.70 and 78.70; S10.15 (a) V o l . 1 2 1 , N o . 2 , K 2 0 7 - K 2 1 0

N. G U S K O S , G . P . T R I B E R I S , M. C A L A M I O T O U , CH. T R I K A L I N O S , A. K O U F O U D A K I S , C. M I T R O S , H. G A M A R I - S E A L E , a n d D. N I A R C H O S T e m p e r a t u r e D e p e n d e n c e of t h e E P R S p e c t r a of G d B a 2 C u 3 0 7 _ Compounds in O r t h o r o m b i c a n d T e t r a g o n a l P h a s e 72.20 and 74.70; 76.30; S10.15 (b) V o l . 1 6 2 , N o . 1 , 2 4 3 - 2 5 0

by

Subject

220

Index

O . Y U . P O L Y A K , R . K H . T U K H V A T U L I N , K I M G E N C H A N , E.M. G A S A N O V , a n d E.M. I B R A G I M O V A E f f e c t of g a m m a - I r r a d i a t i o n o n Y B a 2 C u 3 0 7 _ x C e r a m i c s a n d M o n o c r y s t a l s in t h e S u p e r c o n d u c t i n g S t a t e 74.70; S10.15 (a) V o l . 1 2 2 , N o . 1 , K 4 5 - K 5 0 R. H E R G T , W. A N D R A E , a n d W. S C H U E P P E L P i n n i n g of V o r t i c e s a t T w i n B o u n d a r i e s in Y B a 2 C u 3 0 7 _ x Crystals 74.60 a n d 7 4 . 7 0 ; 6 1 . 7 0 ; S 1 0 . 1 5 (a) V o l . 1 2 2 , N o . 1 , K 5 1 - K 5 4

Single

J. SHA, C . F . ZHU, Z.H. HE, X . - G . LI, Z.P. SU, L.Z. C A O , Q . R . Z H A N G , H . R . YI, a n d H . C . LI N o n l i n e a r I - V C h a r a c t e r i s t i c s of G d B a 2 C u 3 O v E p i t a x i a l F i l m s Related with the Flux Creep 74.60 a n d 7 4 . 7 0 ; S 1 0 . 1 5 (a) V o l . 1 2 2 , N o . 1 , K 5 5 - K 5 8 N. G U S K O S , M. C A L A M I O T O U , S.M. P A R A S K E V A S , A. K O U F O U D A K I S , C. M I T R O S , H. G A M A R I - S E A L E , J. K U R I A T A , L. S A D L O W S K I , a n d M. O n t h e I n f l u e n c e of O x y g e n D e f i c i e n c y on E P R S p e c t r a of NdBa2Cu307_(J76.30; 74.70; S10.15 (b) V o l . 1 6 2 , N o . 2 , K 1 0 1 - K 1 0 6 E.I. T O C H I T S K I I , O.G. S V I R I D O V I C H , E.M. G O L O L O B O V , and D.M. TURTSEVICH P h a s e T r a n s f o r m a t i o n s in Y 1 B a 2 C u 3 0 7 _ x F i l m s P r e p a r e d by Laser Deposition 64.70 a n d 6 8 . 5 5 ; 7 4 . 7 0 ; S 1 0 . 1 5 (a) V o l . 1 2 2 , N o . 2 , 5 5 5 - 5 6 2

WABIA

Pulsed

M. P O P E S C U , G. A L D I C A , C. S A R B U , P. P A U S E S C U , E. C R U C E A N U , F. V A S I L I U , a n d M. A P O S T O L C r y s t a l l i n e P h a s e s in S u p e r c o n d u c t i n g B i : S r : C a : C u 2 : O x C e r a m i c 61.60 a n d 7 4 . 7 0 ; S 1 0 . 1 5 ( a ) V o l . 1 2 2 , N o . 2 , 637-644 P. S E I D E L , M. T U R T E N W A L D , a n d T. B U E S C H E L T e m p e r a t u r e D e p e n d e n c e of t h e S t r u c t u r e s C h a r a c t e r i s t i c s of H i g h - T c J u n c t i o n s 74.70; 74.50 (a) V o l . 1 2 2 , N o . 2 , 6 4 5 - 6 5 0

in t h e

Tunneling

X . A . C H E N G , Z.H. HE, H. ZHANG, X.Y. ZHOU, S.X. W A N G , M . H . F A N G , J . S . X I A , J. SHA, Z.P. SU, a n d Q.R. ZHANG C r y s t a l S t r u c t u r e a n d S u p e r c o n d u c t i v i t y of Y 1 _ x P r x B a 2 C u 3 0 7 _ Compounds 74.70; S10.15 (a) V o l . 1 2 2 , N o . 2 , K 1 5 1 - K 1 5 6

74.70. Superconducting materials

221

S. MOHAN, T. RADJA KOUMAR, and M. GAL High T c Superconductivity of Ba 2 ErCu 3 0 74.70; S10.15 (a) Vol.122,No.2, K157-K160 W. ANDRAE, J. BETZ, B. BRUNNER, R. HERGT, H. LENGFELLNER, K.F. RENK, W. SCHUEPPEL, and K. STEENBECK In-Plane Rotational Magnetic Losses in a Laser Deposited YBa 2 Cu 3 0 7 _ x Film 74.60; 74.70; S10.15 (a) Vol.122,No.2, K161-K164

74.90. Other topics in superconductivity

F. GOLEK, P.W. KLAMUT, B. SUJAK, A.J. ZALESKI, M. CISZEK, and J. OLEJNICZAK Thermally Stimulated Charge Emission from the High Temperature Superconductor YBa 2 Cu 3 0 7 _ x 74.90 and 79.75; S10.15 (a) Vol.117,No.1, K43-K46 B.D. FAINBERG Real Time Optical Spectroscopy of Superconducting-Gap Excitations 74.90 and 78.30 (b) Vol.160,No.2, K169-K172 B.D. FAINBERG Erratum to Real Time Optical Spectroscopy of Superconducting Gap Excitations (phys. stat. sol. (b) 160, K169 (1990)) 74.90 and 78.30 (b) Vol.162,No.1, K67-K68

Subject Index

222 75. Magnetic Properties and Materials 75.10. General theory and models of magnetic

ordering

(see also 71.25. Nonlocalized single-particle electronic states, 71.70. Level splitting and interactions)

L. WANG Two-Dimensional Electron Gas in a Magnetic Field. The Non-Degenerate Limit 71.25; 75.10 (b) Vol.157,No.1, 247-252 V. JANIS Mean-Field Theory for Spin Glasses with Many Macroscopic States 75.10 and 75.40 (b) Vol.157,No.1, 425-430 L.G. GRECHKO, V.M. OGENKO, and A.YU. SEMCHUK Field Influence on the Parameters of Ferromagnetic Semiconductor Superlattices Formed by Coherent Light Beams 71.25 and 75.10 (b) Vol.157,No.1, 451-458 J.M. WESSELINOWA On the Influence of the s-f Exchange Interaction on the Relaxation Time in Ferromagnetic Semiconductors 75.10 (b) Vol.157,No.1, K47-K50 P. PAWLICKI Magnetoelastic Effects in the Exactly Solvable Vaks-Larkin-Ovchinnikov Model of Ising Spins 75.10 and 75.80 (b) Vol.157,No.1, K51-K54 M. KOTRLA and V. DRCHAL Mean-Field Solution Strongly Correlated Systems Using Hubbard Atomic Operators. Hubbard Model with Infinite U 71.10; 75.10 (b) Vol.157,No.2, 635-640 A. URBANIAK-KUCHARCZYK, T. BALCERZAK, J. MIELNICKI, and G. WIATROWSKI The Magnetic Contribution to Electrical Resistivity in Diluted Ising Ferromagnets 72.10 and 75.10 (b) Vol.157,No.2, K103-K108

7 5 . 1 0 . G e n e r a l t h e o r y a n d m o d e l s of m a g n e t i c

ordering

223

A.P. MIKHAILOVSKII, A.M. POLUBOTKO, V.D. PROCHUKHAN, and YU.V. Gapless State in CuFeS, 7 1 . 2 5 a n d 7 5 . 1 0 ; S8 (b) V o l . 1 5 8 , N o . 1 , 2 2 9 - 2 3 8

RUD

G. F I S C H E R a n d A . H E R R M e a n M a g n e t i c M o m e n t s of P o l y c r y s t a l l i n e C e C o m p o u n d s in a Tetragonal Crystal Field 7 5 . 1 0 ; SI.4 (b) V o l . 1 5 9 , N o . 1 , K 2 3 - K 2 6 J. U L N E R a n d K. D U R C Z E W S K I S t a b l e P h a s e s a n d Q u a d r u p o l a r E x c i t a t i o n s in a n O r d e r e d of J = 1 P a r a m a g n e t 75.10 and 75.30 (b) V o l . 1 5 9 , N O . 1 , K 2 7 - K 3 2 S H A O P I N G LI a n d L . E . C R O S S A n a l y s i s of M a g n e t o s t a t i c M o d e s M o d i f i e d by E x c h a n g e Anisotropy Energies 68.30 a n d 7 5 . 1 0 ; 75.70 (b) V o l . 1 5 9 , N o . 2 , 8 6 1 - 8 7 2 R. P I N T A N E L a n d R. F E R R E R Random Magnetic Anisotropy Model with Biquadratic 75. 10 (b) V o l . 1 5 9 , N o . 2 , K 9 3 - K 9 6

Phase

and

Exchange

I.A. V A K A R C H U K a n d V . M . T K A C H U K E n e r g y S p e c t r u m a n d E l e m e n t a r y E x c i t a t i o n D a m p i n g in t h e S t r u c t u r a l l y D i s o r d e r e d Ising M o d e l in a T r a n s v e r s e F i e l d 7 5 . 1 0 ; 7 5.40 (b) V o l . 1 6 0 , N o . 1 , 3 2 1 - 3 2 8 J I A - L I N ZHONG, J I A - L I A N G LI, a n d C H U A N - Z H A N G Y A N G A m o r p h i z a t i o n of t h e T r a n s v e r s e I s i n g M o d e l w i t h 75.10 (b) V o l . 1 6 0 , N o . 1 , 3 2 9 - 3 3 6 E.F. S A R M E N T O a n d T. K A N E Y O S H I S u r f a c e M a g n e t i c P r o p e r t i e s of a T r a n s v e r s e Diluted Surface 73.20 and 75.10 (b) V o l . 1 6 0 , N o . 1 , '337-348 P.

Spin-l

Ising Model with a

PAWLICKI Exactly Solvable Ising Model with Spin-Pseudospin 75.10 (b) V o l . 1 6 0 , N o . 1 , K 5 7 - K 6 0

Interactions

224

Subject

Index

T. B A L C E R Z A K , J. M I E L N I C K I , a n d G. W I A T R O W S K I T h e M a g n e t i c P r o p e r t i e s of T h i n F i l m s w i t h F l u c t u a t i o n s of t h e Exchange Integral 75.10; 75.30 (b) V o l . 1 6 0 , N o . 1 , K 6 1 - K 6 4 A . U R B A N I A K - K U C H A R C Z Y K , T. B A L C E R Z A K , J. M I E L N I C K I , a n d G. W I A T R O W S K I The M a g n e t i c Contribution to Electrical Resistivity in the Ising Ferromagnet with Fluctuating Exchange Integral 72.10 a n d 7 5 . 1 0 (b) V o l . 1 6 0 , N o . 2 , K 1 2 9 - K 1 3 2 A . S . T . P I R E S a n d B.V. C O S T A P h e n o m e n o l o g i c a l C a l c u l a t i o n of t h e S o l i t o n D e n s i t y i n t h e O n e - D i m e n s i o n a l A n t i f e r r o m a g n e t in a n E x t e r n a l F i e l d 75.10; 75.25 (b) V o l . 1 6 0 , N o . 2 , K 1 6 5 - K 1 6 8 J. M I E L N I C K I , T . B A L C E R Z A K , a n d G. W I A T R O W S K I D i s c u s s i o n of t h e F e r r o m a g n e t i c S i m p l e - C u b i c I s i n g w i t h F l u c t u a t i n g E x c h a n g e I n t e g r a l (S=l/2) 75.10 (b) V o l . 1 6 1 , N o . 1 , 335-344 A.S.T. PIRES S o l i t o n in a C a n t e d O n e D i m e n s i o n a l 75.10; 75.25 (b) V o l . 1 6 1 , N o . 1 , K 4 5 - K 4 8

Lattice

Antiferromagnet

A.YU. SEMCHUK, L.G. GRECHKO, and V.M. OGENKO T h e o r y of T r a n s p o r t P h e n o m e n a in F e r r o m a g n e t i c S e m i c o n d u c t o r s w i t h S u p e r l a t t i c e P r o d u c e d by C o h e r e n t L i g h t B e a m s 72.10 a n d 7 5 . 1 0 (b) V o l . 1 6 2 , N o . 2 , 539-544 I. J A E G E R The Ising Antiferromagnet with Competing Interactions : Locating the Tricritical Point 75.10; 68.45 (b) V o l . 1 6 2 , N o . 2 , 575-584 D. ^OKCEVIC' a n d V . Z L A T I C Pertubation Approach to the Periodic Anderson H a m i l t o n i a n k-Dependent Hybridization 7 1 . 1 0 ; 7 1 . 2 0 ; 75.10 (b) V o l . 1 6 2 , N o . 2 , K8 3 - K 8 6

with

75.10. General theory and models of magnetic ordering

225

C.Z. YANG and W.J. SONG Mean Field Renormalization Group and Path-Integral Methods for the Disordered Transverse Ising Model 75.10 (b) Vol.162,No.2, K113-K118

75.20. Diamagnetism and paramagnetism

D. BANERJEE/CHAKRAVORTY and R. BHATTACHARYA Magnetic Properties of Single Crystals of Bismuth Doped with Lead and Tin 75.20; S4 (b) Vol.157,No.1, 443-450 G.B. TAGGART Field Dependence of Dilute Ising Paramagnets 75. 20 (b) Vol.157,No.2, 711-722 B. SUKUMAR and K. NAVANEETHAKRISHNAN Diamagnetic Susceptibility of a Donor in a GaAs/Ga-^^Alj^As Quantum Well Heterostructure and Its Pressure Dependence 73.40 and 75.20; 71.55; S7.12; S7.15 (b) Vol.158,No.1, 193-200 N.S. AVERKIEV, V.M. ASNIN, A.A. ROGACHEV, A.YU. SILOV, and V.l. STEPANOV Photoluminescence Studies of Anomalous Diamagnetic Properties of the 2D e-h System on GaAs Surface 75.20 and 78.55; 73.40; S7.12 (b) Vol.159,No.1, 471-476 S. BISWAS and R. BHATTACHARYA Magnetic Properties of Single Crystals of Bismuth Telluride Doped with 0.2 at% Lead and Its Thermoelectric P'ower 75.20; 71.25; 72.20; S8 (b) Vol.159,No.2, 851-860 K.P. GHATAK and M. MONDAL On a Simplified Analysis of the Magnetic Susceptibilities of Electrons in Ultrathin Films of Non-Parabolic ... 7 5.20 and 75.70; 71.25; S7.16 (b) Vol.160,No.2, 673-682

15

phv-iir.n,

Rog.-Bd.

21

Subject

226

75.25. Spin arrangements (neutron studies,

in m a g n e t i c a l l y o r d e r e d etc.)

Index

materials

K. M E L Z E R , J. S U W A L S K I , a n d M. i U K A S I A K M o e s s b a u e r S t u d y o n t h e S p i n A r r a n g e m e n t in B a F e ^ ^ O ^ g

and

BaCo

0.8Ti0.8Fe10.4°19 75.25 and 76.80; S11.2 (a) V o l . 1 1 8 , N o . 1 , K 3 5 - K 3 8 L.I. KURKINA and O.V. FARBEROVICH E l e c t r o n S t r u c t u r e a n d M a g n e t i c P r o p e r t i e s of S m a l l Particles 7 1 . 5 0 ; 7 3 . 2 0 ; 7 5 . 2 5 ; Sl.l (b) V o l . 1 6 0 , N o . 1 , K 3 7 - K 4 2

Iron

A.S.T. PIRES and B.V. COSTA Phenoroenological C a l c u l a t i o n of t h e S o l i t o n D e n s i t y in t h e O n e - D i m e n s i o n a l A n t i f e r r o m a g n e t in a n E x t e r n a l F i e l d 75.10; 75.25 (b) V o l . 1 6 0 , N o . 2 , K 1 6 5 - K 1 6 8 A.S.T. PIRES S o l i t o n in a C a n t e d O n e D i m e n s i o n a l 75.10; 75.25 (b) V o l . 1 6 1 , N o . 1 , K 4 5 - K 4 8

Antiferromagnet

N . H . L U O N G , N . P . T H U Y , L . T . T A I , a n d N.V. H O A N G E f f e c t of Y S u b s t i t u t i o n o n t h e S p i n R e o r i e n t a t i o n in Compound 7 5 . 2 5 ; 7 5 . 3 0 ; S I . 2 ; SI.4 (a) V o l . 1 2 1 , N o . 2 , 6 0 7 - 6 1 0

75.30. Magnetically ordered materials, other intrinsic effects, see 75.40) (for critical-points

NdFe^Ti

properties

L.I. KOROLEVA and T.V. VIROVETS C r i t i c a l B e h a v i o u r of S e m i c o n d u c t o r S p i n G l a s s e s ( C u C r 2 S e 4 ) x ( C o 0 _ 5 M e 0 _ 5 C r 2 S e 4 ) 1 - x (Me=In,Ga, 0 < x < 0 . l ) 75.30; S8.16 (b) V o l . 1 5 7 , N o . 1 , 4 3 1 - 4 4 2 I.V. M A N Z H O S a n d I.E. C H U P I S G e n e r a t i o n of S p i n - W a v e s by F e r r o e l e c t r i c W a l l E x c i t a t i o n s a Ferroelectric Ferromagnet 75.30 (b) V o l . 1 5 7 , N o . 1 , K 6 5 - K 6 8

in

75.30. Magnetically ordered materials

227

YU.N. DEVYATKO, V.N. TRONIN, and V.l. TROYAN K i n e t i c s of t h e N e w P h a s e N u c l e u s G r o w t h o n a M a g n e t n e a r Curie Point 6 1 . 5 0 ; 7 5 . 3 0 ; SI.2 (a) V o l . 1 1 7 , N o . 1 , 61-66

the

G.E. ABROSIMOVA, N.I. NOVOKHATSKAYA, and A.V. SEREBRYAKOV The Magnetic Field Effect on the Creep-Induced Structural A n i s o t r o p y of A m o r p h o u s C o - F e - N i - S i - B A l l o y s 7 5 . 3 0 ; SI.2 (a) V o l . 1 1 7 , N o . 1 , K 6 7 - K 7 0 E. T A M U R A , R. F E D E R , G. W A L L E R , a n d U. G R A D M A N N D e t e r m i n a t i o n of t h e S u r f a c e M a g n e t i z a t i o n of Fe(llO) Spin-Polarized Low-Energy Electron Diffraction 68.20 a n d 7 5 . 3 0 ; 6 1 . 1 4 ; Sl.l (b) V o l . 1 5 7 , N o . 2 , 627-634 T I E S O N G Z H A O , Z H O N G Z H I FAN, a n d H A N M I N J I N M a g n e t i z a t i o n P r o c e s s e s of t h e R a r e - E a r t h a n d Fe in R 2 F e 1 4 B ( R = T b , D y , H o , E r , a n d Tm) 7 5 . 3 0 ; 7 5 . 6 0 ; S l . l ; SI.4 (b) V o l . 1 5 7 , N o . 2 , 677-684 Y O U XU, G U I - L I N G Y A N G , D A - P I N G CHU, a n d H O N G - R U T h e o r y of t h e S i n g l e I o n M a g n e t o c r y s t a l l i n e of 3 d I o n s 75.30; S11.2 (b) V o l . 1 5 7 , N o . 2 , 685-694 D.

SKRZYPEK C r i t i c a l B e h a v i o u r of t h e M a g n e t i c R e s o n a n c e 75.30 a n d 7 6 . 3 0 ; S9 (b) V o l . 1 5 7 , N o . 2 , 6 9 5 - 7 0 0

by

Sublattices

ZHAI Anisotropy

in K N i M n ,

F

P. N O Z A R , V . S E C H O V S K Y , M . S O L A N K I - M O S E R , E. B A U E R , a n d E. G R A T Z Point-Contact Spectroscopy on the C e ( C u x A l 1 - x ) 5 System 7 1 . 2 0 ; 7 2 . 2 0 ; 7 5 . 3 0 ; SI.2; SI.4 (a) V o l . 1 1 7 , N o . 2 , 5 0 1 - 5 0 8 R . Z . V A L I E V , Y A . D . V I S H N Y A K O V , R . R . M U L Y U K O V , a n d G.S. F A I N S H T E I N O n t h e D e c r e a s e of C u r i e T e m p e r a t u r e in S u b m i c r o n - G r a i n e d Nickel 7 5 . 3 0 ; 7 3 . 4 0 ; SI.2 (a) V o l . 1 1 7 , N o . 2 , 549-554 M. H I D A K A , H. F U J I I , M. N I S H I , a n d B.M. W A N K L Y N M a g n e t i c P h a s e T r a n s i t i o n in t h e L a y e r C o m p o u n d 75.30; S9.16 (a) V o l . 1 1 7 , N o . 2 , 5 6 3 - 5 7 0

CsVF

228

Subject

N. S C H E L U D K O a n d M . M I K H O V I n v e s t i g a t i o n of M a g n e t o c r y s t a l l i n e A n i s o t r o p y of Compounds 7 5 . 3 0 ; S I . 2 ; SI.4 (a) V o l . 1 1 7 , N O . 2 , 5 7 1 - 5 7 6 T.

PALEWSKI Metamagnetism in UAs-YSe Solid 75.30; SI.5 (a) V o l . 1 1 7 , N o . 2 , K 1 5 1 - K 1 5 4

Index

Mm2Co17_xZrx

Solution

A.Z. MENSHIKOV, A.P. VOKHMYANIN, and YU.A. DOROFEEV M a g n e t i c S t r u c t u r e a n d P h a s e T r a n s f o r m a t i o n s in M n 5 S i 75.30; 61.55; SI.61 (b) V o l . 1 5 8 , N o . 1 , 3 1 9 - 3 2 8 T. I W A S H I T A a n d N. U R Y U M a g n e t i c S u s c e p t i b i l i t y of a n I s i n g F e r r o m a g n e t Biquadratic Exchange and Uniaxial Anisotropy 75. 30 (b) V o l . 1 5 8 , N o . 1 , 3 4 7 - 3 5 8

with

A. U R B A N I A K - K U C H A R C Z Y K a n d H. Z E Y A D A T h e H y p e r f i n e F i e l d D i s t r i b u t i o n in D i l u t e d I s i n g 75.30; 75.70 (b) V o l . 1 5 8 , N o . 1 , K 5 9 - K 6 2

Ferromagnet

K.G. N I K I F O R O V , M . B A R A N , V . K . B E L Y A E V , L . Y A . P A S E N K O , S.I. R A D A U T S A N , a n d A . W I S N I E W S K I Magnetization and Chromium Ions with Minority Valence C d C r 2 S 4 and HgCr2Se4 Magnetic Semiconductors 75.30; 75.60; S11.2 (b) V o l . 1 5 8 , N o . 1 , K 6 3 - K 6 8 R.M. C H O R B A D J I A N a n d J. P O Z O E l e m e n t a r y E x c i t a t i o n in A m o r p h o u s 75.30 (b) V o l . 1 5 8 , N o . 2 , K 1 9 1 - K 1 9 4

in

Ferromagnets

Z.A. M A T Y S I N A , M . I . M I L Y A N , D.R. R I Z D V Y A N E T S K I I , a n d S.YU. Z A G I N A I C H E N K O T h e S u r f a c e A t o m i c a n d M a g n e t i c O r d e r in C r y s t a l s 68.2 0 a n d 7 5.30 (b) V o l . 1 5 9 , N o . 1 , K 7 - K 1 2 J. U L N E R a n d K. D U R C Z E W S K I Stable Phases and Quadrupolar Excitations of J = 1 P a r a m a g n e t 75.10 a n d 7 5 . 3 0 (b) V o l . 1 5 9 , N o . 1 , K 2 7 - K 3 2

in a n O r d e r e d

Phase

75.30. Magnetically ordered materials J. P I E C H O T A a n d A . P A J A C Z K O W S K A M a g n e t i c P r o p e r t i e s of YBa,(Cu-, 75.30; 74.70; S10.15 ^ (a) V o l . 1 1 9 , N o . 1 , 2 7 1 - 2 7 8

vNiv) x

229

,07

K.M. MUKIMOV, B.YU. SOKOLOV, and U.V. VALIEV T h e F a r a d a y E f f e c t of R a r e - E a r t h I o n s in G a r n e t s 78.20; 75.30; Sil.2 (a) V o l . 1 1 9 , N o . 1 , 3 0 7 - 3 1 6 N . P . K O L M A K O V A , I.B. K R Y N E T S K I I , M . M . L U K I N A , a n d A . A . M U K H I N C r y s t a l F i e l d a n d M e t a m a g n e t i c B e h a v i o r of R a r e E a r t h Orthoaluminates: DyAlOj 7 5 . 3 0 ; 7 1 . 7 0 ; S10 (b) V o l . 1 5 9 , N o . 2 , 8 4 5 - 8 5 0 O.M.

TOLKACHEV S p i n F l u c t u a t i o n M e c h a n i s m for t h e T e m p e r a t u r e - I n d u c e d M a g n e t i c M o m e n t (TIMM) in t h e E l e c t r o n L i q u i d of Y 2 N i 7 A l l o y 7 5 . 3 0 ; SI.2 (b) V o l . 1 5 9 , N o . 2 , K 1 1 5 - K 1 1 8

M . A H M A D a n d S.J. G L A D Y S Z T h e D y n a m i c S p i n S u s c e p t i b i l i t y a n d 1 = 0 . 1 S p i n W a v e s in a C h a r g e d F e r m i L i q u i d of A l k a l i M e t a l s in a D C M a g n e t i c F i e l d 7 5 . 3 0 ; 6 7 . 5 0 ; S2 (b) V o l . 1 5 9 , N o . 2 , K 1 1 9 - K 1 2 4 T. B A L C E R Z A K , J. M I E L N I C K I , a n d G. W I A T R O W S K I T h e M a g n e t i c P r o p e r t i e s of T h i n F i l m s w i t h F l u c t u a t i o n s of Exchange Integral 7 5 . 1 0 ; 75.30 (b) V o l . 1 6 0 , N o . 1 , K 6 1 - K 6 4 M.

AHMAD S p i n W a v e s w i t h A r b i t a r y 1 in T w o - D i m e n s i o n a l C h a r g e d L i q u i d I m m e r s e d in a DC M a g n e t i c F i e l d 6 7 . 5 0 a n d 75.30 (b) V o l . 1 6 0 , N o . 1 , K 6 5 - K 7 0

the

Fermi

S.I. K L O K I S H N E R , A . V . K O R Y A C H E N K O , a n d B . S . T S U K E R B L A T C h a r g e O r d e r i n g of M u l t i e l e c t r o n i c C l u s t e r s in M i x e d - V a l e n c e Molecular Crystals 7 1 . 7 0 a n d 7 5 . 3 0 ; 6 4 . 6 0 ; S10 (b) V o l . 1 6 0 , N o . 2 , 6 4 1 - 6 4 8 M A I S U A N LI P h a s e D i a g r a m a n d S u s c e p t i b i l i t y of a F r u s t r a t e d F e r r i m a g n e t in Z e r o M a g n e t i c F i e l d 75.30 and 75.40 (b) V o l . 1 6 0 , N o . 2 , K 1 5 9 - K 1 6 4

Ising

230

Subject

U . - C . B O E H N K E , H. B O E R N E R , J . H E R R M A N N , B. L I P P O L D , CH. L. W A L D O E S T L , a n d M . W U R L I T Z E R Some Investigations on Praseodymium-Substituted Yttrium-Barium-Copper-Oxide 74.70; 61.60; 75.30; S10.15 (a) V o l . 1 2 0 , N o . 2 , 5 5 7 - 5 6 6

Index

SEMMELHACK,

S. S O E D E R H O L M , J . H E L L B E R G , J. K R Z Y S T E K , G . O L O V S S O N , I. O L O V S S O N , a n d J.U. V O N S C H U E T Z E l e c t r o n i c P r o p e r t i e s a n d C r y s t a l S t r u c t u r e of a M e t h y l t h i o Substituted Naphthalene C a t i o n Radical Salt: ( D M b T N ) 3 ( C 1 0 4 ) 2 61.65 a n d 7 2 . 2 0 ; 7 1 . 5 5 ; 7 5 . 3 0 ; 7 6 . 3 0 ; S 1 2 . 1 (b) V o l . 1 6 1 , N o . 1 , 2 4 5 - 2 5 6 MAI SUAN LI S t u d y of F r u s t r a t e d I s i n g 75.30 a n d 7 5 . 4 0 (b) V o l . 1 6 1 , N o . 1 , 3 4 5 - 3 5 6

Ferrimagnets

T. I W A S H I T A a n d N. U R Y U Ising Ferromagnet with Three-Site Four-Spin 75.30 (b) V o l . 1 6 1 , N o . 1 , 3 6 7 - 3 7 8 Y.

Interaction

ENDO P h a s e T r a n s i t i o n s of H e i s e n b e r g F e r r o m a g n e t i c 7 5 . 3 0 ; 7 5 . 5 0 ; 75.70 (b) V o l . 1 6 1 , N o . 1 , 3 7 9 - 3 8 6

Superlattices

Z H I - D O N G Z H A N G , X . K . SUN, Z H U O N G - W U Z H A N G , Y.C. C H U A N G , a n d F.R. D E B O E R E f f e c t s of P a r t i a l C o S u b s t i t u t i o n o n M a g n e t i c P r o p e r t i e s (Nd,Gd)2Fe14B 75.30; 75.60; Sl.l (a) V o l . 1 2 1 , N o . 1 , 2 4 1 - 2 4 8 B. L I P P O L D , J. H E R R M A N N , W . R E I C H E L T , a n d H. O P P E R M A N N Preparation and Magnetic Investigations on M n 2 M o 3 0 g Crystals 75.30; 75.50; SI.2; S10.15 (a) V o l . 1 2 1 , N o . 1 , K 9 1 - K 9 4

Single

B A O - G E N S H E N , H U I - Q U N GUO, L I N - Y U A N Y A N G , J U N - X I A N Z H A N G , and JIAN-GAO ZHAO C r y s t a l l i z a t i o n of A m o r p h o u s C o 8 4 _ x B x Z r 1 6 A l l o y s a n d I t s Influence on Hard Magnetic Properties 7 5 . 3 0 ; 6 1 . 4 0 ; 7 5 . 6 0 ; SI.2 (a) V o l . 1 2 1 , N o . 1 , K 1 0 5 - K 1 1 0

of

75.30. Magnetically ordered materials G . S . C H A D D H A a n d J. S I N G H S p i n - 1 E x c h a n g e I n t e r a c t i o n M o d e l of 75.30 (b) V o l . 1 6 1 , N o . 2 , 8 3 7 - 8 4 2

231

Ferromagnetism

N.H. LUONG, N.P. THUY, L.T. TAI, and N.V. HOANG E f f e c t of Y S u b s t i t u t i o n o n t h e S p i n R e o r i e n t a t i o n i n Compound 7 5 . 2 5 ; 7 5 . 3 0 ; S I . 2 ; SI.4 (a) V o l . 1 2 1 , N o . 2 , 6 0 7 - 6 1 0

NdFe^Ti

Z H I - D O N G Z H A N G , X . K . SUN, Y.C. C H U A N G , a n d R . J . R A D W A N S K I A M o d e l B a s e d o n S i n g l e - I o n T h e o r y . I. T h e o r e t i c a l O u t l i n e 7 5 . 5 0 ; 7 5 . 3 0 ; S I . 2 ; SI.4 (a) V o l . 1 2 1 , N o . 2 , 6 1 1 - 6 1 6 Z H I - D O N G ZHANG,, X . K . SUN, Y.C. C H U A N G , F.R. D E B O E R , and R.J. RADWANSKI A M o d e l B a s e d o n S i n g l e - I o n T h e o r y . II. P r e f e r e n t i a l Substitution and Local-Environment Effects at Different 7 5 . 5 0 ; 7 5 . 3 0 ; S l . l ; SI.2 (a) V o l . 1 2 1 , N o . 2 , 6 1 7 - 6 2 6 N . S . A L Y , I. M A H M O U D , M . E . B A S S I O U N I , H . A . M O T A W E H , and A.S. ILYUSHIN M a g n e t i c P h a s e D i a g r a m of t h e T b 1 _ x N d x F e 2 Q u a s i b i n a r y 75.30; Sl.l (a) V o l . 1 2 1 , N o . 2 , K 2 1 9 - K 2 2 2 H. W A D A , T. I N O U E , M . H A D A , M. S H I G A , a n d Y. N A K A M U R A E f f e c t of M a g n e t i c P h a s e T r a n s i t i o n o n t h e E l e c t r o n i c H e a t C o e f f i c i e n t of L u ( C o 1 _ x A l x ) 2 6 5 . 4 0 ; 7 5 . 3 0 ; S I . 2 ; SI.4 (b) V o l . 1 6 2 , N o . 2 , 4 0 7 - 4 1 2

...

System

Specific

JUN-XIAN ZHANG, BAO-GEN SHEN, and WEN-SHAN ZHAN M a g n e t i c P r o p e r t i e s of A m o r p h o u s N d 4 F e g 6 _ x B x A l l o y s a n d I n f l u e n c e s of H e a t T r e a t m e n t o n Its H a r d M a g n e t i c P r o p e r t i e s 75.30; 75.60; Sl.l (a) V o l . 1 2 2 , N o . 2 , 6 5 1 - 6 5 6 A. G R U S K O V A , J. L I P K A , J. S L A M A , I. T O T H , M . S E B E R I N I , a n d P. K A B O S M o e s s b a u e r E f f e c t a n d Its A p p l i c a t i o n in t h e I n v e s t i g a t i o n of t h e S u b s t i t u t e d Li F e r r i t e s O b t a i n e d f r o m t h e L i q u i d P h a s e 75.30 a n d 7 5 . 5 0 ; 7 6 . 8 0 ; S11.2 (a) V o l . 1 2 2 , N o . 2 , K 1 7 1 - K 1 7 6

232

Subject

75.40. Critical-point effects, specific heats, short-range (see also 65.40. Heat capacities)

Index

order

B.A. A R O N Z O N a n d I.M. T S I D I L K O V S K I I M a g n e t i c - F i e l d - I n d u c e d L o c a l i z a t i o n of E l e c t r o n s in F l u c t u a t i o n - P o t e n t i a l W e l l s of I m p u r i t i e s (Review A r t i c l e ) 71.30; 72.20; 75.40; S7.13; S8.15 (b) V o l . 1 5 7 , N o . 1 , 17-60 M . L . M A R f W , M . O R T U N O , A . H E R N A N D E Z , a n d J. A B E L L A N P e r c o l a t i v e T r e a t m e n t of t h e V e r w e y T r a n s i t i o n in C o b a l t - I r o n and Nickel-Iron Ferrites 71.30 a n d 7 5 . 4 0 ; S 1 1 . 2 (b) V o l . 1 5 7 , N o . 1 , 2 7 5 - 2 8 0 V.

JANIS Mean-Field Theory for Spin Glasses w i t h Many Macroscopic 75.10 and 75.40 (b) V o l . 1 5 7 , N o . 1 , 4 2 5 - 4 3 0

S.K. P A L a n d A N I L K U M A R I n f l u e n c e of s - d I n t e r a c t i o n o n t h e C u r i e 75.40 and 75.60 (b) V o l . 1 5 7 , N o . 2 , K 1 3 1 - K 1 3 6

Temperature

V . N . B E R Z H A N S K I I , I.I. E V S T A F E V , a n d V . l . I V A N O V C h a r g e C a r r i e r T r a n s f e r in F e r r i t e S p i n e l s A f f e c t e d Magnetic Ordering 72.20; 75.40; Sil.2 (b) V o l . 1 5 8 , N o . 2 , 643-652 M. BiiASZAK a n d B. F E C H N E R S t o c h a s t i c S o l i t o n s in a D a m p e d H e i s e n b e r g 75.40 (b) V o l . 1 5 9 , N o . 2 , K 1 0 3 - K 1 0 6

States

by

Chain

M.A. ALDZHANOV, N.G. GUSEINOV, G.D. SULTANOV, and M.D. NADZHAFZADE M a g n e t i c H e a t C a p a c i t y a n d S u s c e p t i b i l i t y of t h e Pseudo-One-Dimensional Magnetic Systems TIFeS, and TIFeSe, 7 5 . 4 0 ; 7 5 . 5 0 ; S8 (b) V o l . 1 5 9 , N o . 2 , K 1 0 7 - K 1 1 0 I.A. V A K A R C H U K a n d V . M . T K A C H U K Energy Spectrum and Elementary Excitation Damping in the S t r u c t u r a l l y D i s o r d e r e d I s i n g M o d e l in a T r a n s v e r s e F i e l d 75.10; 75.40 (b) V o l . 1 6 0 , N o . 1 , 3 2 1 - 3 2 8

75.40. Critical-point effects, specific heats, short-range order S. K A H L , R . N E U H A U S , H. P I N K V O S , a n d CH. S C H W I N K T h e I n f l u e n c e of T e n s i l e D e f o r m a t i o n a n d A t o m i c S h o r t - R a n g e O r d e r o n t h e S u s c e p t i b i l i t y of C u M n S p i n G l a s s e s 62.20 a n d 7 5 . 4 0 ; 6 1 . 7 0 ; SI.2 (a) V o l . 1 2 0 , N o . 1 , 2 2 1 - 2 3 2 MAI SUAN LI P h a s e D i a g r a m a n d S u s c e p t i b i l i t y of a F r u s t r a t e d F e r r i m a g n e t in Zero M a g n e t i c F i e l d 75.30 a n d 7 5 . 4 0 (b) V o l . 1 6 0 , N o . 2 , K 1 5 9 - K 1 6 4 MAI SUAN LI S t u d y of F r u s t r a t e d I s i n g 75.30 and 75.40 (b) V o l . 1 6 1 , N o . 1 , 3 4 5 - 3 5 6

Ferrimagnets

D.A. G U S E I N O V a n d M . A . A L Y A N O V H e a t C a p a c i t y a n d T h e r m a l E x p a n s i o n of 6 5 . 4 0 ; 7 5 . 4 0 ; S11.2 (a) V o l . 1 2 1 , N o . 1 , K 5 1 - K 5 4

TiFe^Se*

I. S L E D Z I N S K A , A . M U R A S I K , a n d A . W I S N I E W S K I L i n e a r - C h a i n A n t i f e r r o m a g n e t i s m in a l p h a - N i C 2 0 4 61.60 a n d 7 5 . 4 0 ; S10 (b) V o l . 1 6 1 , N o . 2 , K 9 9 - K 1 0 2 V.

Ising

* 2 D,0

ILKOVIC T h e T e m p e r a t u r e of t h e M a g n e t i c P h a s e T r a n s i t i o n in W e a k l y Coupled Magnetic Layers 75.40 (b) V o l . 1 6 2 , N o . 2 , K 1 1 9 - K 1 2 2

W . A . K A C Z M A R E K , R. B R A M L E Y , a n d A. C A L K A E S R S t u d y of A m o r p h o u s M e t a l l i c A l l o y s b e l o w t h e Multicritical Point 75.50 and 76.30; 75.40; Sl.l; SI.2 (a) V o l . 1 2 2 , N o . 2 , 6 6 3 - 6 7 6

7 5 . 5 0 . S t u d i e s of s p e c i f i c m a g n e t i c

materials

B.X. GU, B . G . S H E N , a n d H . R . ZHAI M a g n e t i c P r o p e r t i e s a n d C r y s t a l l i z a t i o n of Nd

14Fe81B5 Al:Loys 75.50; 61.40; Sl.l (a) V o l . 1 1 7 , N o . 1 , 2 8 3 - 2 9 0

Magnetic

Amorphous

233

234

Subject

Index

E.P. E L S U K O V , Y U . N . V O R O B E V , A . V . T R U B A C H E V , a n d V . A . B A R I N O V S t r u c t u r e a n d M a g n e t i c P r o p e r t i e s of F e - P E l e c t r o d e p o s i t e d Alloys 61.55 and 75.50; 76.80; Sl.l (a) V o l . 1 1 7 , N o . 1 , 2 9 1 - 2 9 8 M. JURCZYK and O.D. CHISTYAKOV M a g n e t i c P r o p e r t i e s of S u b s t i t u t e d C o m p o u n d s (R=Tb o r Dy) 7 5 . 5 0 ; S l . l ; SI.2 (a) V o l . 1 1 7 , N o . 1 , 299-304

Nd2_xRx(Fe,Re,Co)14B

V . V . S I N G E R , A . E . V A F I N , L.M. S A N D R A T S K I I , L . P . M O K H R A C H E V A , S.V. K O N O V A L O V , I.Z. R A D O V S K I I , a n d P.V. G E L D M a g n e t i c S u s c e p t i b i l i t y a n d V a l e n c y of C e a n d P r in T h e i r L i q u i d B i n a r y A l l o y s w i t h M e t a l s of t h e I r o n S u b g r o u p 7 5 . 5 0 ; S l . l ; S I . 2 ; SI.4 (a) V o l . 1 1 7 , N o . 2 , 5 7 7 - 5 8 6 W.A. KACZMAREK, R. BRAMLEY, and A. CALKA I t i n e r a n t E l e c t r o n C o n t r i b u t i o n t o t h e M a g n e t i s m of N i - T M Glassy Metallic Magnets 7 5 . 5 0 a n d 7 6 . 3 0 ; S l . l ; SI.2 (a) V o l . 1 1 7 , N o . 2 , K 1 4 1 - K 1 4 6 A . M . M A N S A N A R E S , F . C . G . G A N D R A , E.C. DA S I L V A , H. V A R G A S , M. D O C A R M O , R . S . V A R E L L A , a n d F. G A L E M B E C K P h o t o a c o u s t i c D e t e c t i o n of M a g n e t i t e - C r y s t a l F o r m a t i o n Iron(III) H y d r o x i d e A c e t a t e 75.50 a n d 7 6 . 5 0 ; S12 (a) V o l . 1 1 7 , N o . 2 , K 1 5 5 - K 1 6 0

from

G. S E R F O Z O , E. K I S D I - K O S Z O , A . S L A W S K A - W A N I E W S K A , L. P O T O C K Y , S. J O N E L I U N A S , a n d M. B A R A N S t u d y of M e t a l l i c G l a s s e s R a p i d l y Q u e n c h e d in M a g n e t i c F i e l d 75.50; 76.50; Sl.l (a) V o l . 1 1 8 , N o . 1 , 3 0 7 - 3 1 0 A. G R A F , R. O B E R M A I E R , a n d W. G E B H A R D T S p i n G l a s s P r o p e r t i e s of Z n 1 _ x M n x S e 75.50; S8.15 (b) V o l . 1 5 8 , N o . 2 , 6 9 5 - 7 0 6 J. Z B R O S Z C Z Y K , W. C I U R Z Y N S K A , J. S W I E R C Z E K , S. S Z Y M U R A , B. WYSfcOCKI, M. B A R A N , a n d A. W I S N I E W S K I E f f e c t of S u r f a c e L a y e r T h i n n i n g o n A p p r o a c h t o M a g n e t i c S a t u r a t i o n in C o 6 4 F e i 4 s i i i B i i A m o r p h o u s A l l o y 7 5 . 5 0 ; S l . l ; SI.2 (a) V o l . 1 1 8 , N o . 2 , 5 2 5 - 5 3 0

75.50. S t u d i e s of s p e c i f i c m a g n e t i c m a t e r i a l s

235

1.0. T R O Y A N C H U K , S.N. P A S T U S H O N O K , A.K. B O G U S H , a n d V . I . P A V L O V M a g n e t i c P r o p e r t i e s of N o n s t o i c h i o m e t r i c O r t h o m a n g a n i t e s 7 5 . 5 0 ; Sll.l (a) V o l . 1 1 8 , N o . 2 , K111-K114 D.M. ZAYACHUK, D.D. IVANCHUK, R.D. IVANCHUK, S.S. M A S L Y A N C H U K , and V.l. MIKITYUK T h e E f f e c t of G a d o l i n i u m D o p i n g o n the P h y s i c a l P r o p e r t i e s of Lead Telluride 7 1 . 5 5 ; 72.80; 7 5 . 5 0 ; S8 (a) V o l . 1 1 9 , N o . 1 , 215-220 B A O - G E N SHEN, L I N - Y U A N YANG, J U N - X I A N ZHANG, FENG W O , T A I - S H A N NING, J I A N - G A O ZHAO, H U I - Q U N GUO, a n d W E N - S H A N ZHAN H a r d M a g n e t i c P r o p e r t i e s of H e a t T r e a t e d F e ? 2 8 C o 4 7 N d 4 B Alloy 7 5 . 5 0 ; 75.60; Sl.l (a) V o l . 1 1 9 , N o . 1 , K 6 3 - K 6 6 P. S V O B O D A , _ M . DIVIS, J. BISCHOF, Z. SMETANA, R. CERNY, a n d J. B U R I A N E K T h e M a g n e t i c P r o p e r t i e s of S m C u 5 7 5 . 5 0 ; SI.4 (a) V o l . 1 1 9 , N o . 1 , K67-K7 0 K. I W A U C H I a n d Y. IKEDA M a g n e t i c P r o p e r t i e s of S i n t e r e d 7 5 . 5 0 ; S10 (a) V o l . 1 1 9 , N o . 1 , K71-K74 A. R A O U F I a n d S. A R A J S A n i s o t r o p y of M a g n e t o r e s i s t i v i t y Ferromagnets 72.15 a n d 75.50; Sl.l (a) V o l . 1 1 9 , N o . 1 , K75-K78

Fe2TiO

in C r y s t a l l i n e a n d A m o r p h o u s

M.A. A L D Z H A N O V , N.G. GUSEINOV, G.D. SULTANOV, a n d M.D. N A D Z H A F Z A D E M a g n e t i c H e a t C a p a c i t y a n d S u s c e p t i b i l i t y of t h e P s e u d o - O n e - D i m e n s i o n a l M a g n e t i c S y s t e m s TlFeS2 a n d T l F e S e 2 7 5 . 4 0 ; 75.50; S8 (b) V o l . 1 5 9 , N o . 2 , K 1 0 7 - K 1 1 0 M. H R A B C A K a n d E. K I S D I - K O S Z O M o d i f i c a t i o n of M a g n e t i c P r o p e r t i e s of A m o r p h o u s R i b b o n s by F l a s h A n n e a l i n g 7 5 . 5 0 ; 75.60; Sl.l (a) V o l . 1 1 9 , N o . 2 , 601-606

Fe-Si-B

236

Subject

W.A.

KACZMAREK Magnetic Structure Rearrangement during Crystallization N i 7 3 M n 5 S i 1 0 B 1 2 Ribbons 7 5 . 5 0 a n d 7 6 . 3 0 ; SI.2 (a) V o l . 1 1 9 , N o . 2 , K 1 5 9 - K 1 6 2

E.P. NAIDEN, V.I. MALTSEV, and G.I. RYABTSEV Magnetic Structure and Spin-Orientational Transitions H e x a f e r r i t e s of t h e B a C o 2 _ x Z n x F e 1 6 0 2 7 S y s t e m 75.50; S11.2 (a) V o l . 1 2 0 , N o . 1 , 2 0 9 - 2 2 0 W.A.

KACZMAREK M a g n e t i c H y p e r f i n e I n t e r a c t i o n s in B a i n , 7 6 . 8 0 ; 7 5 . 5 0 ; S11.2 (a) V o l . 1 2 0 , N o . 1 , K 7 9 - K 8 4

5Fe,Q

5°i9

s / / G . D . M A K S I M O V I C , Z.S. P O P O V I C , F.R. V U K A J L O V I C , a n d K . M a g n e t i c P r o p e r t i e s of P d 3 F e 75.50; Sl.l (b) V o l . 1 6 0 , N o . 2 , 6 3 5 - 6 4 0 W. W A L Z a n d H . K R O N M U E L L E R P o i n t D e f e c t s in E l e c t r o n - I r r a d i a t e d S t o i c h i o m e t r i c 61.70 a n d 7 5 . 5 0 ; S10 (b) V o l . 1 6 0 , N o . 2 , 6 6 1 - 6 7 2

Index

in

of

Ferrite

/ VULETIC

Magnetite

A.YA. FISHMAN, M.A. IVANOV, V.YA. MITROFANOV, and A.A. SHEMYAKOV H y p e r f i n e I n t e r a c t i o n s of J a h n - T e l l e r I o n M n 3 + i n C u b i c Magnets with Spinel and Garnet Structures 7 5 . 5 0 ; 7 6 . 2 0 ; Sil.2 (b) V o l . 1 6 0 , N o . 2 , K 1 5 3 - K 1 5 8 G . F . ZHOU, X . K . SUN, S.Y. FU, Y.C. C H U A N G , R. G R O E S S I N G E R , and H.R. KIRCHMAYR R e l a t i o n s h i p b e t w e e n M i c r o s t r u c t u r e a n d C o e r c i v i t y in (Nd,Dy)-(Fe,Co)-B Based Sintered Magnets with Minor Nb and A1 75.50; 64.80; Sl.l (a) V o l . 1 2 0 , N o . 2 , 627-634 U . C . J O H R I , R . M . S I N G R U , a n d D. B A H A D U R M a g n e t i c a n d M o e s s b a u e r S t u d i e s of t h e S y s t e m (x=0.1,0.3,0.5) 76.80; 75.50; S10.15 (b) V o l . 1 6 1 , N o . 1 , 3 5 7 - 3 6 6 Y.

ENDO P h a s e T r a n s i t i o n s of H e i s e n b e r g F e r r o m a g n e t i c 75.30; 75.50; 75.70 (b) V o l . 1 6 1 , N o . 1 , 3 7 9 - 3 8 6

LaCo1-xZrxO

Superlattices

...

7 5 . 5 0 . S t u d i e s of s p e c i f i c m a g n e t i c

materials

237

D. V L A D I K O V A , L. I L K O V , a n d S. K A R B A N O V O p t i m a l P r e f i r i n g C o n d i t i o n s of S u b s t i t u t e d N i c k e l for Microwave Applications 6 4 . 7 5 a n d 7 5 . 5 0 ; S11.2 (a) V o l . 1 2 1 , N o . 1 , 2 4 9 - 2 5 6 S. U N N I K R I S H N A N a n d D . K . C H A K R A B A R T Y M a g n e t i c P r o p e r t i e s a n d D o m a i n S t a t e of t h e Ferrite-Magnesium Titanate Solid Solutions 7 5 . 5 0 ; 7 6 . 8 0 ; S11.2 (a) V o l . 1 2 1 , N o . 1 , 2 6 5 - 2 7 2

Ferrites

Magnesium

B. L I P P O L D , J . H E R R M A N N , W. R E I C H E L T , a n d H. O P P E R M A N N Preparation and Magnetic Investigations on M n 2 M o 3 O g Crystals 75.30; 75.50; SI.2; S10.15 (a) V o l . 1 2 1 , N o . 1 , K 9 1 - K 9 4

Single

L. SADfcOWSKI, J. K U R I A T A , B. B O J A N O W S K I , J. W A L C Z A K , M . K U R Z A W A , M.L. FALIN, and V.V. IZOTOV E P R S t u d y of A n t i f e r r o m a g n e t i c P h a s e T r a n s i t i o n in F e 4 V 2 M o 3 0 76.30; 75.50; Sll.l (a) V o l . 1 2 1 , N o . 1 , K 9 5 - K 9 8 B.X. GU, B . G . S H E N , a n d H.R. ZHAI C r y s t a l l i z a t i o n a n d M a g n e t i c P r o p e r t i e s of

Amorphous

Nd

o.i9Feo.8i A11°y 7 5 . 5 0 ; 6 1 . 4 0 ; S l . l ; SI.4 (a) V o l . 1 2 1 , N o . 1 , K 9 9 - K 1 0 4

A.G . POPOV, YE.V. BELOZEROV, A.G. KUCHIN, A.S. ERMOLENKO, G.M. MAKAROVA, V.S. GAVIKO, and V.I. KHRABROV M a g n e t i c P r o p e r t i e s of S m 2 ( F e , M ) 1 7 C X C o m p o u n d s , M = C o , A l , G a 7 5 . 5 0 ; SI (a) V o l . 1 2 1 , N o . 1 , K 1 1 1 - K 1 1 6 A . A . S O R O K I N , D.D. P E R L O V , R.Z. L E V I T I N , N . P . K O L M A K O V A , and A.P. DODOKIN D e t e r m i n a t i o n of G r o u n d Q u a s i d o u b l e t P a r a m e t e r s for H o 3 + in ( H o x Y 1 _ x ) 3 A l 5 0 12 f r o m L o w - T e m p e r a t u r e M a g n e t i c ... 7 1 . 7 0 a n d 7 5 . 5 0 ; S11.2 (b) V o l . 1 6 1 , N o . 2 , K 1 0 3 - K 1 0 6

Ion

Z H I - D O N G Z H A N G , X . K . SUN, Y.C. C H U A N G , a n d R . J . R A D W A N S K I A M o d e l B a s e d o n S i n g l e - I o n T h e o r y . I. T h e o r e t i c a l O u t l i n e 7 5 . 5 0 ; 7 5 . 3 0 ; S I . 2 ; SI.4 (a) V o l . 1 2 1 , N o . 2 , 611-616

238

Subject

ZHI-DONG ZHANG, X.K. SUN, Y.C. CHUANG, F.R. DE BOER, and R.J. RADWANSKI A Model Based on Single-Ion Theory. II. Preferential Substitution and Local-Environment Effects at Different 75.50; 75.30; Sl.l; SI.2 (a) Vol.121,No.2, 617-626

Index

...

L.I. VERSHININA, S.Z. SKLUEV, V.S. ZHIGALOV, A.G. STEPANOV, G.I. FROLOV, A.S. AVILOV, and S.V. OREKHOV The Structure of Amorphous Dy-Co Films with Magnetic Anisotropy 61.40 and 75.50; SI.2 (a) Vol.121,No.2, K145-K148 BAO-GEN SHEN and S. METHFESSEL Crystallization of the Amorphous F e 8 3 N d 7 B 1 0 Alloy and the Formation Process of N d 2 F e 2 3 B 3 Phase 75.50; Sl.l (a) Vol.121,No.2, K211-K214 Y. KHAN Phases Obtained by Continuous Heating of the Amorphous Permanent Magnet Alloy N d 4 4 F e 7 7 g B 1 7 8 61.55 and 75.50; Sl.l (a) Vol.122,No.1, K1-K6 X.K. SUN, ZHI-GANG ZHAO, LIU WEI, and Y.C. CHUANG Structure and Magnetic Properties of P r 2 F e 1 4 _ x C o x B 1 _ C, Compounds 75.50; Sl.l (a) Vol.122,No.1, K69-K72 A.G. LIPSON, V.A. KUZNETSOV, D.M. SAKOV, and YU.P. TOPOROV Electrical and Magnetic Properties of the Polymer-Ceramics Produced on the Basis of Lithium Fluoride 73.40 and 75.50; S9.ll; S12 (a) Vol.122,No.2, 563-568 W.A. KACZMAREK, R. BRAMLEY, and A. CALKA ESR Study of Amorphous Metallic Alloys below the Magnetic Multicritical Point 75.50 and 76.30; 75.40; Sl.l; SI.2 (a) Vol.122,No.2, 663-676 A. GRUSKOVA, J. LIPKA, J. SLAMA, I. TOTH, M. SEBERINI, and P. KABOS Moessbauer Effect and Its Application in the Investigation of the Substituted Li Ferrites Obtained from the Liquid Phase 75.30 and 75.50; 76.80; S11.2 (a) Vol.122,No.2, K171-K176

75.60. Domain effects, magnetization curves

2

75.60. Domain effects, magnetization curves, and hysteresis A.G. SHISHKOV, E.N. ILICHEVA, E.V. KOCHETKOVA, and YU.N. FEDYUNIN On the Choice of the Pulse Waveform for Reading without Distortion of the Vertical Bloch Line Information 75.70; 75.60; Sil.2 (a) Vol.117,No.1, K53-K56 A.H. WAFIK and A.A. SATTAR Dependence of the Irreversible Magnetization in Co 1 _ a Cd a Fe 2 0 on the Magnetizing Field 75.60; S10 (a) Vol.117,No.1, K61-K66 TIESONG ZHAO, ZHONGZHI FAN, and HANMIN JIN Magnetization Processes of the Rare-Earth and Fe Sublattices in R 2 F e 1 4 B (R=Tb,Dy,Ho,Er,and Tm) 75.30; 75.60; Sl.l; SI.4 (b) Vol.157,No.2, 677-684 A. TARI and J.S. HWANG Magnetisation and ESR Studies of G d ( N i 1 - x R h x ) 5 Compounds 75.60 and 76.30; SI.4 (b) Vol.157,No.2, 701-710 S.K. PAL and ANIL KUMAR Influence of s-d Interaction on the Curie Temperature 75.40 and 75.60 (b) Vol.157,No.2, K131-K136 D. PiUSA, R. PFRANGER, and B. WYStOCKI Magnetic Domain Structure of Sintered N d 1 5 F e 7 7 B g Magnet in Rotational Magnetic Field 75.60; Sl.l (a) Vol.117,No.2, 541-548

Permanent

K.G. NIKIFOROV, M. BARAN, V.K. BELYAEV, L.YA. PASENKO, S.I. RADAUTSAN, and A. WISNIEWSKI Magnetization and Chromium Ions with Minority Valence in CdCr 2 S 4 and HgCr 2 Se 4 Magnetic Semiconductors 75.30; 75.60; S11.2 (b) Vol.158,No.1, K63-K68 K. MAKI and H. KRONMUELLER Investigation of Demagnetization Processes in Fe 1 4 Nd 2 B-Type Sintered Magnets 75.60; Sl.l; SI.4 (a) Vol.118,No.1, 253-270

240

Subject

R. S C H A E F E R a n d A . H U B E R T A New M a g n e t o o p t i c Effect Related to Non-Uniform o n t h e S u r f a c e of a F e r r o m a g n e t 75.60; 78.20; Sl.l; SI.2; SI.4; Sil.2 (a) V o l . 1 1 8 , N o . 1 , 2 7 1 - 2 8 8 0. P O P O V a n d M . M I K H O V T e m p e r a t u r e a n d M a g n e t i c F i e l d D e p e n d e n c e of t h e Single Domain Size 75. 60 (a) V o l . 1 1 8 , N o . 1 , 289-294 H.

Index

Magnetization

Critical

PFEIFFER D e t e r m i n a t i o n of A n i s o t r o p y F i e l d D i s t r i b u t i o n i n P a r t i c l e A s s e m b l i e s T a k i n g into A c c o u n t T h e r m a l F l u c t u a t i o n s 75.60 (a) V o l . 1 1 8 , N o . 1 , 2 9 5 - 3 0 6

D. M A R T I N E Z , C. D E F R A N C I S C O , J. I N I G U E Z , J. R I V A S , a n d F. W A L Z I n f l u e n c e of B a S u b s t i t u t i o n s o n M a g n e t i c A f t e r - E f f e c t s in Magnetite Containing Vacancies 75.60; S11.2 (a) V o l . 1 1 8 , N o . 1 , K 3 1 - K 3 4 T. T Y M O S Z , K. S W I D E R C Z A K , a n d K. B R A N S K A L o r e n t z M i c r o s c o p e S t u d y of O b l i q u e l y E v a p o r a t e d C o C r Films 75.60 a n d 7 5 . 7 0 ; SI.2 (a) V o l . 1 1 8 , N o . 2 , 5 1 9 - 5 2 4 U.

HEIBER O n t h e D o m a i n C o n f i g u r a t i o n of F i n i t e U n i a x i a l 7 5 . 6 0 ; S10 (a) V o l . 1 1 8 , N o . 2 , 5 3 1 - 5 3 8

Thin

Crystals

V.P. GOGIN, V.A. MATVEEV, V.G. TASHIROV, YU.G. RAYZANOV, and A.A. ROMANYUKHA C o m p e n s a t i o n M e c h a n i s m of t h e T e m p e r a t u r e S t a b i l i z a t i o n of B u b b l e C o l l a p s e F i e l d in E u - T m G a r n e t 7 5 . 7 0 ; 7 5 . 6 0 ; S11.2 (a) V o l . 1 1 8 , N o . 2 , K 1 0 7 - K 1 1 0 H. P F E I F F E R a n d W . S C H U E P P E L I n v e s t i g a t i o n of M a g n e t i c P r o p e r t i e s of B a r i u m F e r r i t e by R e m a n e n c e C u r v e s 75.60; S11.2 (a) V o l . 1 1 9 , N o . 1 , 2 5 9 - 2 7 0

the

Powders

75.60. Domain effects, magnetization curves BAO-GEN SHEN, LIN-YUAN YANG, JUN-XIAN ZHANG, FENG WO, TAI-SHAN NING, JIAN-GAO ZHAO, HUI-QUN GUO, and WEN-SHAN ZHAN Hard Magnetic Properties of Heat Treated Fe 7 2 s C o 4 7Nc*4B Alloy 75.50; 75.60; Sl.l (a) Vol.119,No.1, K63-K66 K. ELK and V. CHRISTOPH Dipole-Dipole Interaction in Fine Particle Magnets 75. 60 (b) Vol.159,No.2, K111-K114 H.K. LACHOWICZ, E. PULIDO, A. SIEMKO, and A. HERNANDO Stress-Forced Magnetoresistance in Near-Zero Magnetostrictive Metallic Glasses 72.15 and 75.80; 75.60; Sl.l; SI.2 (a) Vol.119,No.2, 595-600 M. HRABCAK and E. KISDI-KOSZO Modification of Magnetic Properties of Amorphous Fe-Si-B Ribbons by Flash Annealing 75.50; 75.60; Sl.l (a) Vol.119,No.2, 601-606 A.V. KOROLEV, V.S. GAVIKO, and N.V. MUSHNIKOV The Magnetic Annealing Effect in Hydrogen Containing Intermetallic Sm(Fe,Co)2 Compounds 75.60 and 75.80; SI.2 (a) Vol.119,No.2, K163-K166 H. PFEIFFER Relaxation Behaviour of Magnetic Particle Assemblies Due to Thermal Fluctuations 75.60 (a) Vol.120,No.1, 233-246 H. PFEIFFER, W. SCHUEPPEL, and TH. KLUPSCH On the Magnetic Properties of Planar Hexaferrite Powders 75.60; S11.2 (a) Vol.120,No.1, K89-K92 A.H. WAFIK and A.Z. MOHAMED Barkhausen Jumps and Microstructure in Molybdenum Eutectoid Steel 75.60; 64.80; Sl.l (a) Vol.120,No.2, 601-608 R.L. SOMMER and F.P. LIVI Barkhausen Noise Measurements in Small Samples of (110)[001] Silicon-Iron 75.60; SI.61 (a) Vol.120,No.2, 609-616 16 p h y s i c a , Reg.-Bd. 23

2

242

Subject

J. C H E N a n d H . K R O N M U E L L E R P r o p e r t i e s of N d - F e - B M a g n e t s P r o c e s s e d by t h e Decrepitation Technique 75.60; Sl.l (a) V o l . 1 2 0 , N o . 2 , 6 1 7 - 6 2 6

Index

Hydrogen

K. E L K a n d V . C H R I S T O P H O n t h e W o h l f a r t h R e m a n e n c e R e l a t i o n s in M a g n e t i c Ensembles 75.60 (b) V o l . 1 6 1 , N o . 1 , K 4 1 - K 4 4 Y . D . Y A O , Y . Y . C H E N , S.J. T Z E N G , a n d T . H . C H U A N G Electrical Resistivity, Magnetization, and Grain P r e c i p i t a t e s in N i - S n A l l o y s 7 2 . 1 5 ; 7 5 . 6 0 ; SI.2 (a) V o l . 1 2 1 , N o . 1 , 2 1 3 - 2 1 8

Particle

Boundary

Z H I - D O N G Z H A N G , X.K. SUN, Z H U O N G - W U ZHANG, Y . C . C H U A N G , a n d F.R. D E B O E R E f f e c t s of P a r t i a l C o S u b s t i t u t i o n o n M a g n e t i c P r o p e r t i e s (Nd,Gd)2Fe14B 75.30; 75.60; Sl.l (a) V o l . 1 2 1 , N o . 1 , 2 4 1 - 2 4 8 G . F . ZHOU, S.Y. FU, X.K. SUN, a n d Y.C. C H U A N G I n f l u e n c e of A n n e a l i n g o n t h e M a g n e t i c P r o p e r t i e s M i c r o s t r u c t u r e of N d - F e - B B a s e d M a g n e t s 75.60; Sl.l (a) V o l . 1 2 1 , N o . 1 , 2 5 7 - 2 6 4

of

and

BAO-GEN SHEN, HUI-QUN GUO, LIN-YUAN YANG, JUN-XIAN ZHANG, and JIAN-GAO ZHAO C r y s t a l l i z a t i o n of A m o r p h o u s C o 8 4 _ x B x Z r 1 6 A l l o y s a n d Its Influence on Hard Magnetic Properties 7 5 . 3 0 ; 6 1 . 4 0 ; 7 5 . 6 0 ; SI.2 (a) V o l . 1 2 1 , N o . 1 , K 1 0 5 - K 1 1 0 H. P F E I F F E R , W . S C H U E P P E L , a n d A. S A E C K L O n t h e D e t e r m i n a t i o n of t h e V o l u m e a n d t h e A n i s o t r o p y F i e l d of S m a l l M a g n e t i c P a r t i c l e s by C o e r c i v i t y M e a s u r e m e n t s 75. 60 (a) V o l . 1 2 1 , N o . 1 , K 1 1 7 - K 1 2 0 L.

KRAUS B l o c h W a l l s in M a g n e t o s t r i c t i v e M e t a l l i c 7 5 . 6 0 ; 75.80 (b) V o l . 1 6 1 , N o . 2 , 8 5 3 - 8 6 0

Glasses

75.60. Domain effects, magnetization curves P. NOVOTNY and R. GEMPERLE Wall Hysteresis Loops Exhibiting Asymmetry 75.60; Sil.2 (a) Vol.121,No.2, K215-K218 H. PFEIFFER Influence of Thermal Fluctuations on the Magnetic Properties of Particle Assemblies 75.60 (a) Vol.122,No.1, 377-390 JUN-XIAN ZHANG, BAO-GEN SHEN, and WEN-SHAN ZHAN Magnetic Properties of Amorphous Nd 4 Fe g 6 _ x B x Alloys and Influences of Heat Treatment on Its Hard Magnetic Properties 75.30; 75.60; Sl.l (a) Vol.122,No.2, 651-656 A.H. WAFIK Dependence of the Irreversible Magnetization in Co^_ a Cu a Fe 2 0 on the Magnetizing Field 75.60; S10 (a) Vol.122,NO.2, 657-662

75.70. Magnetic films and plates

A.G. SHISHKOV, E.N. ILICHEVA, E.V. KOCHETKOVA, and YU.N. FEDYUNIN On the Choice of the Pulse Waveform for Reading without Distortion of the Vertical Bloch Line Information 75.70; 75.60; Sil.2 (a) Vol.117,No.1, K53-K56 A. URBANIAK-KUCHARCZYK and H. ZEYADA The Hyperfine Field Distribution in Diluted Ising Ferromagnet 75.30; 75.70 (b) Vol.158,No.1, K59-K62 /

/

s

H. RATAJCZAK, I. GOSCIANSKA, and T. LUCINSKI Influence of Annealing on Saturation Magnetization and Hall Resistivity in Amorphous Nd 1 2 C o 82 B 6 Films 61.40 and 68.55; 73.60; 75.70; SI.2; SI. 4 (a) Vol.118,No.1, 189-196 / / T. TYMOSZ, K. SWIDERCZAK, and K. BRANSKA Lorentz Microscope Study of Obliquely Evaporated CoCr Thin Films 75.60 and 75.70; SI.2 (a) Vol.118,No.2, 519-524

-16*

243

244

Subject

Index

L. V A T S K I C H E V , J. M U C H A , ZH. G E O R G I E V , a n d M . V A T S K I C H E V A M e a s u r e m e n t s of t h e R o t a t i o n a l H y s t e r e s i s L o s s e s in M a g n e t i c Films by the Planar Hall Effect 72.15 and 75.70 (a) V o l . 1 1 8 , N o . 2 , K 9 5 - K 9 8 V.P. GOGIN, V.A. MATVEEV, V.G. TASHIROV, YU.G. RAYZANOV, and A.A. ROMANYUKHA C o m p e n s a t i o n M e c h a n i s m of t h e T e m p e r a t u r e S t a b i l i z a t i o n of t h e B u b b l e C o l l a p s e F i e l d in E u - T m G a r n e t 75.70; 75.60; S11.2 (a) V o l . 1 1 8 , N o . 2 , K 1 0 7 - K 1 1 0 M . M A N Z E L , E. S T E I N B E I S S , a n d W . S C H U E P P E L M a g n e t i c P r o p e r t i e s of S p u t t e r - S y n t h e s i z e d C o N - F i l m s 7 5 . 7 0 ; SI.62 (a) V o l . 1 1 9 , N o . 1 , 279-284 S H A O P I N G LI a n d L . E . C R O S S A n a l y s i s of M a g n e t o s t a t i c M o d e s M o d i f i e d b y E x c h a n g e Anisotropy Energies 68.30 a n d 7 5 . 1 0 ; 75.70 (b) V o l . 1 5 9 , N o . 2 , 8 6 1 - 8 7 2 B.X. GU, H. H O M B U R G , S. M E T H F E S S E L , a n d H . R . ZHAI C r y s t a l l i z a t i o n B e h a v i o r a n d M a g n e t i c P r o p e r t i e s of Nd-Fe-B Thin Films 68.55 a n d 7 5 . 7 0 ; 7 6 . 8 0 ; S l . l (a) V o l . 1 2 0 , N o . 1 , 1 5 9 - 1 6 8

and

Amorphous

K.P. GHATAK and M. M O N D A L O n a S i m p l i f i e d A n a l y s i s of t h e M a g n e t i c S u s c e p t i b i l i t i e s E l e c t r o n s in U l t r a t h i n F i l m s of N o n - P a r a b o l i c ... 75.20 a n d 7 5 . 7 0 ; 7 1 . 2 5 ; S 7 . 1 6 (b) V o l . 1 6 0 , N o . 2 , 6 7 3 - 6 8 2

of

N.V. EDNERAL, V.G. KUTILIN, YU.A. LISOVSKII, M.L. SOKOLOVA, A.M. UMPELEV, A.O. TITOV, and L.K. FIONOVA T h i n F i l m S t r u c t u r e s for M a g n e t o - O p t i c a l I n f o r m a t i o n R e c o r d i n g 68.55; 75.70; 78.20; Sl.l (a) V o l . 1 2 0 , N o . 2 , 4 5 7 - 4 6 6 Y.

ENDO P h a s e T r a n s i t i o n s of H e i s e n b e r g F e r r o m a g n e t i c 75.30; 75.50; 75.70 (b) V o l . 1 6 1 , N o . 1 , 3 7 9 - 3 8 6

Superlattices

75.80. Magnetomechanical and magnetoelectric effects

75.80. Magnetomechanical and magnetoelectric magnetostriction

245

effects,

For galvanomagnetic effects, see 72.15 and 72.20 For magneto-optical effects, see 78.20

P. PAWLICKI Magnetoelastic Effects in the Exactly Solvable Vaks-Larkin-Ovchinnikov Model of Ising Spins 75.10 and 75.80 (b) Vol.157,No.1, K51-K54 M. FAEHNLE and J. FURTHMUELLER On the Change of Magnetostriction by Field Annealing of Amorphous Ferromagnetic Alloys 75.80; SI.2 (a) Vol.117,No.1, K71-K76 H.K. LACHOWICZ, E. PULIDO, A. SIEMKO, and A. HERNANDO Stress-Forced Magnetoresistance in Near-Zero Magnetostrictive Metallic Glasses 72.15 and 75.80; 75.60; S1.1; SI.2 (a) Vol.119,No.2, 595-600 A.V. KOROLEV, V.S. GAVIKO, and N.V. MUSHNIKOV The Magnetic Annealing Effect in Hydrogen Containing Intermetallic Sm(Fe,Co)2 Compounds 75.60 and 75.80; SI.2 (a) Vol.119,No.2, K163-K166 L. KRAUS Bloch Walls in Magnetostrictive Metallic Glasses 75.60; 75.80 (b) Vol.161,No.2, 853-860

246

Subject Index

76. Magnetic Resonances and Relaxation in Condensed Hatter; Moessbauer Effect 76.20. General theory of resonances and relaxation E.I. NEIMARK, I.N. NURUTDINOVA, and A.B. ROITSIN A Method for Calculating the Inhomogeneously Broadened Resonance Line Shape 76.20 (b) Vol.158,No.1, K55-K58 A.YA. FISHMAN, M.A. IVANOV, V.YA. MITROFANOV, and A.A. SHEMYAKOV Hyperfine Interactions of Jahn-Teller Ion Mn 3+ in Cubic Magnets with Spinel and Garnet Structures 75.50; 76.20; Sil.2 (b) Vol.160,No.2, K153-K158 M.I. KAGANOV and T.I. SHALAEVA Resonance Polaritons 71.36; 76.20 (b) Vol.162,No.2, 469-476

76.30. Electron paramagnetic resonance and relaxation C. YU, C. LAI, S.A. MARSHALL, D.R. YODER-SHORT, and Y.N. ZHANG Electron Paramagnetic Resonance Spectra Observed in Single Crystals of YBa 2 Cu 3 0 7 _ i 74.60; 76.30; S10.15 (b) Vol.157,No.1, 379-388 WEN-CHEN ZHENG Spin-Lattice Coupling Coefficients F^^ for SrTi0 3 :Cr 3 + Crystal 71.70; 76.30; Sll.l (b) Vol.157,No.1, K33-K38 KH.B. GEZALOV, A.M. GASANOV, A.A. GARIBOV, M.M. ALIEV, and N.I. MUSAEV The Nature of Paramagnetic Centers in gamma-Irradiated Boron Oxides 61.80 and 76.30; S10.1 (a) Vol.117,No.1, K57-K60 D. SKRZYPEK Critical Behaviour of the Magnetic Resonance in K N i x M n 1 - x F 75.30 and 76.30; S9 (b) Vol.157,No.2, 695-700

76.30. Electron paramagnetic resonance and relaxation A. TARI and J.S. HWANG M a g n e t i s a t i o n a n d E S R S t u d i e s of G d ( N ^ ^ R l ^ ) 7 5 . 6 0 a n d 7 6 . 3 0 ; SI.4 (b) V o l . 1 5 7 , N o . 2 , 7 0 1 - 7 1 0 S. W A P L A K a n d N . N . K O L P A K O V A Phase Transitions in C d 2 N b 2 0 7 64.70; 76.30; S10.15 (a) V o l . 1 1 7 , N o . 2 , 4 6 1 - 4 6 6

5

2

Compounds

S t u d i e d b y E P R of C r 3 +

Ion

W.A. KACZMAREK, R. BRAMLEY, and A. CALKA I t i n e r a n t E l e c t r o n C o n t r i b u t i o n t o t h e M a g n e t i s m of N i - T M Glassy Metallic Magnets 7 5 . 5 0 a n d 7 6 . 3 0 ; S l . l ; SI.2 (a) V o l . 1 1 7 , N o . 2 , K 1 4 1 - K 1 4 6 E.A. E I V A Z O V , A . F . S A F A R O V , S.M. A T A K I S H I E V , a n d Y A . M . T h e E P R S p e c t r u m of C o Q 7 C u Q 3 C r 2 S 4 _ x S e x S y s t e m 76.30; S8.16 (a) V o l . 1 1 7 , N o . 2 , K 1 4 7 - K 1 5 0

ABASOV

V.K. VORONKOVA, L.V. MOSINA, A.E. USACHEV, and YU.V. YABLOKOV W e a k P a i r E x c h a n g e I n t e r a c t i o n s b e t w e e n C o b a l t I o n s in t h e Quasi-One-Dimensional Antiferromagnet CsCoCl3 76.30; 71.70; S9.15 (b) V o l . 1 5 8 , N o . 1 , 3 3 7 - 3 4 6 WAN-LUN YU C r y s t a l F i e l d E f f e c t o n t h e g - F a c t o r s of 71.70; 76.30; S8.ll; S10.1; Sll.l (b) V o l . 1 5 8 , N o . 1 , K 1 3 - K 1 6

6

S-State

Ions

M . W A T T E N B A C H , C. K I S I E L O W S K I - K E M M E R I C H , H. A L E X A N D E R , V . V . K V E D E R T.R. MCHEDLIDZE, and YU.A. OSIPYAN E l e c t r i c - D i p o l e S p i n R e s o n a n c e of D i s l o c a t i o n s in P l a s t i c a l l y Deformed p-Type Silicon 71.55 and 76.30; S5.ll (b) V o l . 1 5 8 , N o . 1 , K 4 9 - K 5 4 S. F U J I T A a n d S. W A T A N A B E O n t h e O r i e n t a t i o n D e p e n d e n c e of t h e C y c l o t r o n R e s o n a n c e f o r H o l e s in G e a n d Si 7 1 . 2 5 a n d 7 6 . 3 0 ; S 5 . l l ; S5.12 (b) V o l . 1 5 8 , N o . 1 , K 6 9 - K 7 4 DEYAN HE, FANGQING ZHANG, and GUANGHUA CHEN A D i r e c t M e a s u r e m e n t of T h e r m a l E q u i l i b r i u m D e f e c t s in Hydrogenated Amorphous Silicon-Nitrogen Alloy Films 61.70 and 76.30; S5.ll (a) V o l . 1 1 8 , N o . 1 , K 3 9 - K 4 2

Peaks

248

Subject

L.K. A M I N O V a n d Y U . Y U . K O S T E T S K I I T e m p e r a t u r e D e p e n d e n c e of E P R L i n e w i d t h of I m p u r i t i e s Van-Vleck Paramagnets 71.70 a n d 7 6 . 3 0 ; S 9 . 1 6 (b) V o l . 1 5 8 , N o . 2 , 5 9 5 - 6 0 2

Index

in

K. ZINK, A . K R O S T , H . N E L K O W S K I , J. S A H M , a n d H. S T U T E N B E C K E R E n e r g y T r a n s f e r M e c h a n i s m s in Z n ^ ^ n ^ e (0. 0 0 5 < x < 0 . 017) Detected by ODMR 71.70; 76.30; 78.55; S8.15 (b) V o l . 1 5 8 , N o . 2 , 6 0 3 - 6 0 8 WEN-CHEN ZHENG A n E s t i m a t e of t h e S p i n - L a t t i c e C o u p l i n g C o e f f i c i e n t s Trigonal C d S : M n 2 + Crystals 71.70; 76.30; S8.ll (b) V o l . 1 5 8 , N o . 2 , K 1 3 7 - K 1 4 2 G U O Y I N S H E N , C H A N G Q I N G XU, a n d G U I R U B A I C u 2 + - C u 2 + P a i r E f f e c t o n E P R P a r a m e t e r s in C 2 v Crystals 71.70 a n d 7 6 . 3 0 ; Sll (b) V o l . 1 5 8 , N o . 2 , K 1 8 5 - K 1 9 0

Symmetry

D . L . D Z H A P A R I D Z E , S.V. A L C H A N G Y A N , D.M. D A R A S E L I A , a n d T.I. S A N A D Z E E P R a n d R F D S S t u d y of G d 3 + in a l p h a - L i I 0 3 S i n g l e 76.30; Sll.l (b) V o l . 1 5 8 , N o . 2 , K 1 9 5 - K 1 9 6 W.

for

ZAPART P o s s i b i l i t y of S i m u l t a n e o u s l y I n c o m m e n s u r a t e a n d P h a s e i n R b I n ( M o 0 4 ) 2 b y E P R of C r 3 + I o n 64.70 a n d 7 6 . 3 0 ; § 1 1 . 1 (a) V o l . 1 1 8 , N o . 2 , 4 4 7 - 4 5 4

Crystals

Ferroelastic

M . ZABKOWSKA-WACIiAWEK a n d W . W O J C I E C H O W S K I E l e c t r i c a l a n d M a g n e t i c P r o p e r t i e s of C o p p e r Phthalocyanine-Carbon Black Mixtures 7 2 . 8 0 ; 7 6 . 3 0 ; S12 (a) V o l . 1 1 8 , N o . 2 , K 8 7 - K 9 0 P. S I V A P R A S A D , K. R A M E S H , a n d Y.P. R E D D Y O p t i c a l a n d E P R S t u d i e s of C u 2 + in M g N H 4 P 0 4 76.30 a n d 7 8 . 5 0 ; 7 1 . 5 5 ; S l l . l (a) V o l . 1 1 8 , N o . 2 , K 1 0 3 - K 1 0 6

* 6 H,0

GUANGHUA CHEN, WEI JIA, and FANGQING ZHANG E S R S t u d y o n A n n e a l i n g B e h a v i o r of R e a c t i v e l y a-GeNx:H Films 68.60 a n d 7 6 . 3 0 ; S6 (a) V o l . 1 1 8 , N o . 2 , K 1 1 5 - K 1 1 8

Sputtered

76.30. Electron paramagnetic resonance and relaxation H. HIKITA, K. TAKEDA, and Y. KIMURA EPR of New Cr 3 + Centers in Sn02 Crystals 76.30; S10.1 (a) Vol.119,No.1, 251-258 V.K. JAIN and G. LEHMANN Electron Paramagnetic Resonance of Mn 2 + in Orthorhombic and Higher Symmetry Crystals (Review Article) 76.30; 64.60; Sll (b) Vol.159,No.2, 495-544 T. KAMIKAWA A New Hole Centre in Neutron Irradiated LiF Crystals 61.70; 76.30; S9.ll (b) Vol.159,No.2, 571-576 WEN-CHEN ZHENG Spin-Lattice Coupling Coefficients F^^ for d 8 Ions in Cubic Symmetry 71.70; 76.30; S10.1 (b) Vol.159,No.2, K67-K72 W. A. KACZMAREK Magnetic Structure Rearrangement during Crystallization in Ni 7 3 Mn 5 Si 1 0 B 1 2 Ribbons 75.50 and 76.30; SI.2 (a) Vol.119,NO.2, K159-K162 H.A. BUCKMASTER and K. KUMAR The Cjjj Symmetry EPR Spectral Parameters for (0.005Gd,0.995La)(C2H5S04)3 * 9 H,0 and 9 D 2 0 76.30; 71.70; Sll (b) Vol.160,No.1, 349-356 WEN-CHEN ZHENG Spin-Lattice Coupling Coefficients for CaO:Ni2+ Crystals 71.70; 76.30; S10.1 (b) Vol.160,No.1, K43-K48 A.A. ALYBAKOV, O.M. ARBOTOEV, V.A. GUBANOVA, and I.K. TURDALIEV Paramagnetic Centers in X-Irradiated LiH2P04 Single Crystals 76.30; Sll.l (a) Vol.120,No.1, K85-K88 S.A. MARSHALL, D.R. YODER-SHORT, C. YU, Y.N. ZHANG, and J.K. FURDYNA Super Hyperfine Structure in the EPR Spectrum of Divalent Manganese in Single Crystal Zinc Selenide 71.70 and 76.30; S8.12 (b) Vol.160,No.2, 591-600

249

Subject

250 A . G O L T Z E N E a n d C. S C H W A B Q u a l i t a t i v e a n d Q u a n t i t a t i v e D i f f e r e n t i a t i o n of A n i o n - A n t i s i t e - R e l a t e d S p e c t r a in G a A s 71.70 a n d 76.30; S7.12 (b) V o l . 1 6 0 , N O . 2 , 6 4 9 - 6 6 0 S.M. A K H M I N , V . P . M E I K L Y A R , A . E . U S A C H E V , a n d Y U . V . 5 9 C o 2 + E N D O r in t h e T e t r a g o n a l P h a s e of C s C a C l 3 76.30 a n d 7 6 . 7 0 ; 6 4 . 6 0 ; S 9 . 1 6 (b) V o l . 1 6 0 , N o . 2 , K 1 4 9 - K 1 5 2 C.

Index

Paramagnetic

YABLOKOV

KISIELOWSKI-KEMMERICH V a c a n c i e s a n d T h e i r C o m p l e x e s in t h e C o r e of S c r e w D i s l o c a t i o n s . M o d e l s w h i c h A c c o u n t f o r E S R - I n v e s t i g a t i o n ... (Review A r t i c l e ) 61.70; 76.30; S5.ll (b) V o l . 1 6 1 , N o . 1 , 11-42

S. S O E D E R H O L M , J. H E L L B E R G , J. K R Z Y S T E K , G. O L O V S S O N , I. O L O V S S O N , and J.U. V O N SCHUETZ E l e c t r o n i c P r o p e r t i e s a n d C r y s t a l S t r u c t u r e of a M e t h y l t h i o Substituted Naphthalene Cation Radical Salt: ( D M b T N ) 3 ( C 1 0 4 ) 2 61.65 and 72.20; 71.55; 75.30; 76.30; S12.1 (b) V o l . 1 6 1 , N o . 1 , 2 4 5 - 2 5 6 F. M A E S , F. C A L L E N S , P. M A T T H Y S , a n d E. E P R of Sj in N a B r 61.70 a n d 7 6 . 3 0 ; S 9 . l l (b) V o l . 1 6 1 , N o . 1 , K 1 - K 4

BOESMAN

F U - Z H E N L I a n d Z H A O - M I N LI T h e E i g h t - O r d e r P e r t u r b a t i o n F o r m u l a of Z e r o - F i e l d S p l i t t i n g for 3 d 5 I o n s i n D 3 d S i t e a n d Its A p p l i c a t i o n t o C a C 0 3 : M n 2 + 71.70; 76.30; Sll.l (b) V o l . 1 6 1 , N o . 1 , K 2 9 - K 3 4 E. P O S S E N R I E D E , O . F . S C H I R M E R , a n d G. E S R of N d 3 + in B a T i 0 3 76.30; Sll.l (b) V o l . 1 6 1 , N o . 1 , K 5 5 - K 5 8

GODEFROY

D . P . E R C H A K , R . B . G E L F A N D , N.M. P E N I N A , V . F . S T E L M A K H , V.P. TOLSTYKH, A.G. ULYASHIN, V.S. VARICHENKO, and A.M. ZAITSEV P o i n t P a r a m a g n e t i c D e f e c t s in D i a m o n d I r r a d i a t e d by High-Energy Ions 6 1 . 7 0 ; 7 6 . 3 0 ; 7 8 . 6 0 ; S5 (a) V o l . 1 2 1 , N o . 1 , 63-72 A . P O E P P L a n d G. V O E L K E L E S R a n d P h o t o - E S R I n v e s t i g a t i o n s of t h e v j C e n t r e in ZnO R a w M a t e r i a l a n d L i - D o p e d ZnO C e r a m i c P o w d e r 71.55; 76.30; S10.1 (a) V o l . 1 2 1 , N o . 1 , 195-204

76.30. Electron paramagnetic resonance and W . ZAP A R T a n d M . B . Z A P A R T I n c o m m e n s u r a t e P h a s e in K S c ( M o 0 4 ) 2 64.70 a n d 7 6 . 3 0 ; S l l . l (a) V o l . 1 2 1 , N o . 1 , K 4 3 - K 4 6

relaxation

b y E P R of

251

Cr3+

A . P O E P P L a n d G. V O E L K E L E S R a n d P h o t o - E S R I n v e s t i g a t i o n s of t h e P b 3 + C e n t r e in U n d o p e d ZnO C e r a m i c s 71.55; 76.30; S10.1 (a) V o l . 1 2 1 , N o . 1 , K 6 9 - K 7 2 L. S A D Ü O W S K I , J . K U R I A T A , B. B O J A N O W S K I , J. W A L C Z A K , M . K U R Z A W A , M.L. FALIN, and V.V. IZOTOV E P R S t u d y of A n t i f e r r o m a g n e t i c P h a s e T r a n s i t i o n i n F e 4 V 2 M o 3 0 76.30; 75.50; Sll.l (a) V o l . 1 2 1 , N o . 1 , K 9 5 - K 9 8 A.CH. LUSHCHIK and A.G. FRORIP T h e r m a l i z e d a n d H o t I n t e r s t i t i a l H a l o g e n Ions in A l k a l i 61.70 a n d 7 8 . 5 5 ; 6 1 . 8 0 ; 7 6 . 3 0 ; S 9 . l l (b) V o l . 1 6 1 , N o . 2 , 5 2 5 - 5 3 6 WEN-CHEN ZHENG S p i n - L a t t i c e C o u p l i n g C o e f f i c i e n t s G ^ j for T r i g o n a l and ZnSiFg * 6 H 2 0 : N i 2 + Crystals 7 1 . 7 0 ; 7 6 . 3 0 ; S 9 . 1 6 ; S10 (b) V o l . 1 6 1 , N o . 2 , 7 1 1 - 7 1 6 A.P. PECHONII, T.V. ANTIMIROVA, M.D. GLINCHUK, a n d I.M. S M O L Y A N I N O V A n E S R S t u d y of L i + I m p u r i t y I o n D e f o r m a t i o n a l 76.30; 61.70; Sil (b) V o l . 1 6 1 , N o . 2 , 8 4 3 - 8 5 2

Halides

Al203:Fe3+

F i e l d s in K T a 0 3

T . L . CHOY a n d Y . Y . Y E U N G L o c a l D i s t o r t i o n a n d C r y s t a l F i e l d P a r a m e t e r s for C r 3 + O r t h o r h o m b i c S i t e s in M g O 76.30; S10.1 (b) V o l . 1 6 1 , N o . 2 , K 1 0 7 - K 1 1 0

at

G U A N G H U A C H E N , J I N Z H A N G XU, a n d F A N G Q I N G Z H A N G T h e E S R S t u d i e s of B - D o p e d a - S i : H T h i n F i l m s P r e p a r e d by Reactive-Sputtering 61.40 a n d 7 6 . 3 0 ; 6 8 . 5 5 ; S5.ll (a) V o l . 1 2 1 , N o . 2 , 5 0 1 - 5 0 6 K A N G - W E I Z H O U , S A N G - B O ZHAO, P I N G - F E N G W U , a n d J U N - K A I X I E E P R P a r a m e t e r s a n d S p e c t r a l F i n e S t r u c t u r e of N i 2 + in L i N b O 7 1 . 7 0 a n d 7 6 . 3 0 ; 7 8 . 5 0 ; Sll.l (b) V o l . 1 6 2 , N o . 1 , 1 9 3 - 1 9 8

Subject

252

Index

N. GUSKOS', G . P . T R I B E R I S , M . C A L A M I O T O U , C H . T R I K A L I N O S , A . K O U F O U D A K I S , C. M I T R O S , H. G A M A R I - S E A L E , a n d D. N I A R C H O S T e m p e r a t u r e D e p e n d e n c e of t h e E P R S p e c t r a o f G d B a 2 C u 3 0 7 _ ( j Compounds in Orthorombic and Tetragonal Phase 72.20 and 74.70; 76.30; S10.15 (b) V o l . 1 6 2 , N o . 1 , 2 4 3 - 2 5 0 S.K. MISRA a n d J I A N S H E N G SUN E P R of a G d 3 + - D o p e d N H 4 P r ( S 0 4 ) 2 * 4 H 2 0 S i n g l e C r y s t a l . S t u d y of P h a s e T r a n s i t i o n a n d S u p e r p o s i t i o n - M o d e l C a l c u l a t i o n of .. 76.30; Sll (b) V o l . 1 6 2 , N O . 1 , 2 6 5 - 2 7 4 R. H R A B A N S K I a n d J. L E C H O p t i m i z a t i o n of Spin Hamiltonian Parameters by the M e t h o d Non-Linear Least Squares Fitting 76.30; Sll (b) V o l . 1 6 2 , N o . 1 , 2 7 5 - 2 8 0

of

M.D. GLINCHUK, I.P. BYKOV, V.M. KURLIAND, M. BOUDYS, a n d K. N E J E Z C H L E B V a l e n c y S t a t e s a n d D i s t r i b u t i o n o f M a n g a n e s e I o n s in P Z T Ceramics Simultaneously Doped with Mn and Nb 71.55; 76.30; S10.15 (a) V o l . 1 2 2 , N o . 1 , 3 4 1 - 3 4 6 H. M E T Z , G. V O E L K E L , a n d W . W I N D S C H A S i m p l e M e t h o d f o r F i t t i n g of I n h o m o g e n o u s E S R Curves 76.30 (a) V o l . 1 2 2 , N o . 1 , K7 3 - K 7 6

Saturation

S. S W A M I , V . K . A G A R W A L , S.S. S H A R M A , a n d J. V A R M A M o e s s b a u e r a n d E S R S t u d i e s of P o l y m e t a l l i c N o d u l e s 76.30 a n d 76.80; SI.2 (a) V o l . 1 2 2 , N o . 1 , K 7 7 - K 8 2 F.J.

OWENS N o n - R e s o n a n t M i c r o w a v e A b s o r p t i o n in N = 3 P h a s e of Bi-Pb-Sr-Ca-Cu-0 High-Temperature Superconductor 74.30; 76.30; S10.15 (b) V o l . 1 6 2 , N o . 2 , 5 6 5 - 5 7 4

S . K . M I S R A , J I A N S H E N G S U N , a n d U. O R H U N EPR of a V 0 2 + - D o p e d F e ( N H 4 ) 2 ( S 0 4 ) 2 * 6 H 2 ° Single Crystal: V O z + - F e 2 + Exchange Interaction and Spin-Lattice Relaxation 76.30; Sll (b) V o l . 1 6 2 , N o . 2 , 5 8 5 - 5 9 6

...

76.30. Electron paramagnetic resonance and relaxation

253

N. GUSKOS, M. CALAMIOTOU, S.M. PARASKEVAS, A. KOUFOUDAKIS, C. MITROS, H. GAMARI-SEALE, J. KURIATA, L. SADLOWSKI, and M. WABIA On the Influence of Oxygen Deficiency on EPR Spectra of NdBajCUjOy.^ 76.30; 74.70; S10.15 (b) Vol.162,No.2, K101-K106 W.A. KACZMAREK, R. BRAMLEY, and A. CALKA ESR Study of Amorphous Metallic Alloys below the Magnetic Multicritical Point 75.50 and 76.30; 75.40; Sl.l; SI.2 (a) Vol.122,No.2, 663-676

76.50. Ferromagnetic, antiferromagnetic, and ferrimagnetic resonances; spin-wave resonance (see also

75.30.

Spin

waves)

A.M. MANSANARES, F.C.G. GANDRA, E.C. DA SILVA, H. VARGAS, M. DO CARMO, R.S. VARELLA, and F. GALEMBECK Photoacoustic Detection of Magnetite-Crystal Formation from Iron(III) Hydroxide Acetate 75.50 and 76.50; S12 (a) Vol.117,No.2, K155-K160 G. SERFOZO, E. KISDI-KOSZO, A. SLAWSKA-WANIEWSKA, L. POTOCKY, S. JONELIUNAS, and M. BARAN Study of Metallic Glasses Rapidly Quenched in Magnetic Field 75.50; 76.50; Sl.l (a) Vol.118,No.1, 307-310

76.60. Nuclear magnetic resonance and relaxation K.D. TOVSTYUK, I.O. POLYAKOV, E.I. SLINKO, N.K. TOVSTYUK, and A.G. KHANDOZHKO Lithium Impurity States in PbTe 64.60; 61.70; 76.60; S8 (b) Vol.157,No.1, 151-158 N.T. MAMEDOV and A.M. PANICH Phase Transition in TIGaTe 64.70 and 76.60; S8.16 (a) Vol.117,No.1, K15-K18 XIQI FENG, DONGSHENG WANG, and JIZHOU ZHANG NMR Spectra of Mg Nuclei in Mg-Doped LiNb0 3 Crystals 76.60; Sll.l (b) Vol.157,No.2, K127-K130

Subject

254 J. C Z A P L I C K I , N . W E I D E N , a n d A . W E I S S D y n a m i c s of P r o t o n s in C d ( N H 3 ) g X 2 T y p e 76.60; S9.16 (a) V o l . 1 1 7 , N o . 2 , 5 5 5 - 5 6 2

Index

Compounds

S.G. K O Z L O V A , Y U . G . K R I G E R , a n d S . P . G A B U D A A n i s o t r o p i c R e o r i e n t a t i o n of O c t a h e d r a l I o n s A c c o r d i n g t o N M R Relaxation in Solid State 76.60; 71.70; Sll (b) V o l . 1 5 8 , N o . 1 , 3 2 9 - 3 3 6 E.K. SADYKOV and A.I. SKVORTSOV T h e o r y of R . F . M o e s s b a u e r S p e c t r a of t h e M a g n e t i c s Magnetic Anisotropy 76.60 a n d 7 6 . 8 0 ; S l l . l (b) V o l . 1 5 8 , N o . 2 , 685-694

with

S. G R A N D E , B. L I P P O L D , G. M A Y E R , a n d H. S C H M I E D E L N Q R M e a s u r e m e n t s of 6 3 C u in Y B a 2 C u 3 0 7 _ x 74.70 and 76.60; S10.15 (b) V o l . 1 5 8 , N o . 2 , 707-714 R. P I R L O T , M . C Y A M U K U N G U , L. G R E N A C S , J. L E H M A N N , a n d K. T O M P A R e l a x a t i o n T i m e M e a s u r e m e n t s a n d H y p e r f i n e F i e l d s a t 1 2 B in Transition Metals 76.60; SI (b) V o l . 1 5 8 , N o . 2 , K 1 9 7 - K 2 0 0 M . M A C K O W I A K , N. W E I D E N , a n d A. W E I S S Phase Transitions and Molecular Dynamics in Tris(Methylammonium) Nonabromodiantimonate(III) 63.20 a n d 6 4 . 7 0 ; 7 6 . 6 0 ; S12 (a) V o l . 1 1 9 , N o . 1 , 7 7 - 8 6 P.K.

J.

and Its

KAHOL E v a l u a t i o n of M o m e n t s f r o m t h e N M R S o l i d E c h o e s in D i p o l a r Solids 76.60 (b) V o l . 1 5 9 , N o . 2 , 8 7 3 - 8 8 2

KASPRZAK T h e I n f l u e n c e of E l e c t r o n H o p p i n g o n t h e Q u a d r u p o l e in C u 2 0 76.60; 72.20; S10.1 (b) V o l . 1 6 0 , N o . 1 , K 5 3 - K 5 6

J.E.

...

GARBARCZYK S t u d y of P r o t o n i c D i f f u s i o n in H 4 Using PFG NMR Method 66.30; 76.60; Sll (a) V o l . 1 2 0 , N o . 2 , 3 8 7 - 3 9 0

5U02(I06)1

3

* m

Relaxation

H20

76.60. N u c l e a r m a g n e t i c r e s o n a n c e a n d r e l a x a t i o n

255

A.A. B O G U S L A V S K I I , YU.N. IVANOV, A.I. KRIEGER, A . K . M O S K A L E V , V.l. P A K H O M O V , a n d R.SH. L O T F U L L I N N M R I n v e s t i g a t i o n of Q u a d r u p o l e I n t e r a c t i o n a n d C h e m i c a l Shift 133 C s in C s 2 H g B r 4 C r y s t a l 76.60 a n d 7 7 . 8 0 ; S9.16 (b) V o l . 1 6 1 , N o . 1 , K49-K54 T.SH. A B E S A D Z E a n d R.A. E L EGAIMI S u b h a r m o n i c E x c i t a t i o n of M u l t i p l e Spin Echo S i g n a l s Systems with Quadrupole Interaction 76.60 (b) V o l . 1 6 1 , N o . 2 , K111-K112

in

76.70. M a g n e t i c d o u b l e r e s o n a n c e s a n d cross e f f e t s S.M. A K H M I N , V . P . M E I K L Y A R , A.E. U S A C H E V , a n d YU.V. Y A B L O K O V 59 C o 2 + E N D O R in t h e T e t r a g o n a l P h a s e of C s C a C l 3 76.30 a n d 7 6 . 7 0 ; 64.60; S9.16 (b) V o l . 1 6 0 , N o . 2 , K149-K152 S.M. A K H M I N , V . P . M E I K L Y A R , A.E. USACHEV, YU.V. Y A B L O K O V , a n d S.V. Y U R T A E V A E l e c t r o n - N u c l e a r I n t e r a c t i o n s of t h e C e 3 + Ion in C S j N a l n C I 76.70; S9.16 (b) V o l . 1 6 2 , N o . 2 , K107-K112

76.80. M o e s s b a u e r e f f e c t ; o t h e r g a m m a - r a y

spectroscopy

A.K. ZHETBAEV, K . M . DONBAEV, a n d M . B . A B L A N O V Spin R e o r i e n t a t i o n in I r r a d i a t e d H e m a t i t e at 7 to 60 K 61.70 a n d 7 6 . 8 0 ; S10.1 (b) V o l . 1 5 7 , N o . 1 , K55-K60 E.A. V A S I L E V a n d T.M. T K A C H E N K O T h e 1 1 9 S n A t o m D y n a m i c s in N i s b - N i 1 76.80; SI.2 (b) V o l . 1 5 7 , N o . 1 , K61-K64

5

Solid

Solutions

E.P. ELSUKOV, YU.N. V O R O B E V , A.V. T R U B A C H E V , and V.A. B A R I N O V S t r u c t u r e a n d M a g n e t i c P r o p e r t i e s of Fe-P E l e c t r o d e p o s i t e d Alloys 61.55 a n d 7 5 . 5 0 ; 76.80; Sl.l (a) V o l . 1 1 7 , N o . 1 , 291-298 J.J. BARA, B.F. BOGACZ, A. POLACZEK, M. PEKALA, a n d A. G R O D Z I N S K I T h e T e m p e r a t u r e I n d u c e d T r a n s i t i o n in the t h e t a - T y p e V a n a d i u m Oxide Bronzes 61.60; 6 4 . 7 0 ; 7 6 . 8 0 ; S10 (a) V o l . 1 1 8 , N o . 1 , 41-52

256

Subject

K. MELZER, J. SUWALSKI, and M. i U K A S I A K Moessbauer Study on the Spin Arrangement BaCo

Ti

in B a F e 1 2 ° i 9

an