FN ISI Export Format VR 1.0 PT J AU Andreeva, MA Irkaev, SM Semenov, VG Prokhorov, KA Salashchenko, NN Chumakov, AI Ruffer, R TI Mossbauer reflectometry of multilayer structure Zr(10 nm)/[Cr(1.7 nm)/Fe-57(1.6 nm)](26)/Cr(50 nm) - comparative measurements in energy and time domains SO HYPERFINE INTERACTIONS NR 5 AB It is shown that the nuclear resonance interaction strongly enhances the standing wave pattern formed in a multilayer structure at Bragg reflection. It is surprising that the amplitude of modulations increases with a depth and has a maximum in the middle part of multilayer for the time- dispersive method of investigation. The behavior of standing waves can be used for depth selective measurements. CR ANDREEVA MA, 1999, J ALLOY COMPD, V286, P322 ANDREEVA MA, 1999, JETP LETT+, V69, P863 BEDZYK MJ, 1988, NUCL INSTRUM METH A, V266, P679 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 NAGY DL, 1997, P 32 ZAK SCH PHYS CO TC 0 BP 343 EP 348 PG 6 JI Hyperfine Interact. PY 2000 VL 126 IS 1-4 GA 323TL J9 HYPERFINE INTERACTIONS UT ISI:000087581000051 ER PT J AU Nagy, DL Bottyan, L Deak, L Szilagyi, E Spiering, H Dekoster, J Langouche, G TI Synchrotron Mossbauer reflectometry SO HYPERFINE INTERACTIONS NR 34 AB Grazing incidence nuclear resonant scattering of synchrotron radiation can be applied to perform depth-selective phase analysis and to determine the isotopic and magnetic structure of thin films and multilayers. Principles and recent experiments of this new kind of reflectometry are briefly reviewed. Methodological aspects are discussed. Model calculations demonstrate how the orientations of the sublattice magnetisation in ferro- and antiferromagnetic multilayers affect time-integral and time-differential spectra. Experimental examples show the efficiency of the method in investigating finite-stacking, in-plane and out-of-plane anisotropy and spin-flop effects in magnetic multilayers. CR AFANASEV AM, 1965, ZH EKSP TEOR FIZ, V21, P215 ALP EE, 1993, PHYS REV LETT, V70, P3351 ANDREEVA MA, 1999, J ALLOY COMPD, V286, P322 BARON AQR, 1994, PHYS REV B, V50, P10354 BERNSTEIN S, 1963, PHYS REV, V132, P1625 BORN M, 1970, PRINCIPLES OPTICS, P51 BOTTYAN L, 1998, HYPERFINE INTERACT, V113, P295 BOTTYAN L, 1999, UNPUB CARBONE C, IN PRESS CHUMAKOV AI, 1999, HYPERFINE INTERACT, V123, P427 CHUMAKOV AI, 1993, PHYS REV LETT, V71, P2489 DEAK L, 1999, CONDENSED MATTER STU, P151 DEAK L, 1994, HYPERFINE INTERACT, V92, P1083 DEAK L, 1996, PHYS REV B, V53, P6158 FERMI E, 1946, PHYS REV, V70, P103 GROTE M, 1991, EUROPHYS LETT, V14, P707 HANNON JP, 1985, PHYS REV B, V32, P5068 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 KIESSIG H, 1931, ANNLN PHYS, V10, P715 KOHLHEPP J, 1997, PHYS REV B, V55, PR696 KULCSAR K, 1971, P INT C MOSSB SPECTR, P594 LAX M, 1951, REV MOD PHYS, V23, P287 MAJOR M, 1999, CONDENSED MATTER STU, P165 NAGY DL, 1997, CONDENSED MATTER STU, P17 NAGY DL, 1992, HYPERFINE INTERACT, V71, P1349 NAGY DL, 1999, MOSSBAUER SPECTROSCO, P323 NIESEN L, 1998, PHYS REV B, V58, P8590 NOTERMANN FC, 1992, PHYS REV B, V46, P10847 ROHLSBERGER R, 2000, HYPERFINE INTERACT, V125, P69 SMIRNOV GV, 1996, HYPERFINE INTERACT, V97-8, P551 SPIERING H, 2000, HYPERFINE INTERACT, V125, P197 SPIERING H, 1985, HYPERFINE INTERACT, V24, P737 TOELLNER TS, 1995, PHYS REV LETT, V74, P3475 WANG RW, 1994, PHYS REV LETT, V72, P920 TC 0 BP 353 EP 361 PG 9 JI Hyperfine Interact. PY 2000 VL 126 IS 1-4 GA 323TL J9 HYPERFINE INTERACTIONS UT ISI:000087581000053 ER PT J AU Spiering, H Deak, L Bottyan, L TI EFFINO SO HYPERFINE INTERACTIONS NR 20 AB The program EFFINO (Environment For FItting Nuclear Optics) evaluates Mossbauer absorption and time spectra both in nuclear forward scattering and in grazing incidence reflection geometry. Time-integral prompt and delayed angular scan spectra are also treated. The time spectra are calculated by Fourier transformation from frequency to time domain. The electric quadrupole and magnetic dipole fields at the nuclear sites are considered static at present. The specimen in both forward scattering and grazing incidence is assumed to be a multilayer, with individual thickness and interface roughness (the latter only for the grazing incidence case at present) and electronic index of refraction. Up to eight different layers plus eight repetition periods of those layers are treated. Each layer may contain zero to eight nuclear sites (zero in all layers being prompt X-ray reflectivity), with their own effective thickness or (for grazing incidence) their own complex nuclear index of refraction. From the forward scattering amplitude, a differential 4 x 4 propagation matrix is constructed for each layer. Several experimental spectra of the same or different type(s) can be fitted simultaneously. Correlations between parameters of the same or of different spectra can be introduced. CR *J GUT U, 1982, AN CHEM AN CHEM AFANASEV AM, 1965, ZH EKSP TEOR FIZ, V21, P215 ANDREEVA MA, 1994, SOV PHYS JETP, V78, P965 ANDREEVA MA, 1986, VESTN MOSK U FIZ AS+, V27, P57 BLUME M, 1968, PHYS REV, V171, P417 BORZDOV GN, 1976, ZH PRIKL SPEKTROSK, V25, P526 DEAK L, 1999, CONDENSED MATTER STU DEAK L, IN PRESS COMMON ANIS DEAK L, 1996, PHYS REV B, V53, P6158 FEDOROV FI, 1976, TEORIA GIROTROPII GRANT RW, 1968, PHYS REV, V171, P417 HANNON JP, 1969, PHYS REV, V186, P306 HANNON JP, 1968, PHYS REV, V169, P315 HANNON JP, 1984, PHYS REV B, V32, P5068 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 KULCSAR K, 1971, P INT C MOSSB SPECTR, P594 MULLER EW, 1982, MOSFUN LAB REPORT AN ROHLSBERGER R, 1994, THESIS U HAMBURG SPIERING H, 1978, HYP INTERACT, V120, P265 TC 1 BP 197 EP 204 PG 8 JI Hyperfine Interact. PY 2000 VL 125 IS 1-4 GA 288VZ J9 HYPERFINE INTERACTIONS UT ISI:000085586300011 ER PT J AU Semenov, VG Andreeva, MA Irkaev, SM Prokhorov, KA Salashchenko, NN Chumakov, AI Ruffer, R TI Anomalous decreasing of hyperfine magnetic field value in the top layers of multilayered structure revealed by mossbauer reflectometry method SO IZVESTIYA AKADEMII NAUK SERIYA FIZICHESKAYA NR 16 CR ALEXANDROV ML, 1992, HYPERFINE INTERACT, V71, P1461 ANDREEVA MA, 1996, HYPERFINE INTERACT, V97-8, P605 ANDREEVA MA, 1998, IZV AKAD NAUK FIZ+, V62, P406 ANDREEVA MA, 1999, J ALLOY COMPD, V286, P322 ANDREEVA MA, 1992, JETP LETT, V55, P62 ANDREEVA MA, 1991, PHYS STATUS SOLIDI A, V127, P455 ANDREEVA MA, 1999, POVERKHNOST, P59 ANDREEVA MA, 1994, ZH EKSP TEOR FIZ+, V105, P1767 BOTTYAN L, 1995, 10 INT C HFI LEUV BE HANNON JP, 1985, PHYS REV B, V32, P5068 IRKAEV SM, 1995, NUCL INSTRUM METH B, V103, P351 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 KLINKHAMMER F, 1996, J MAGN MAGN MATER, V161, P49 NAGY DL, 1997, P 32 ZAK SCH PHYS CO ZHETBAEV AK, 1995, FAZOVYE PREVRASHCHEN TC 0 BP 1422 EP 1429 PG 8 JI Izv. Akad. Nauk Ser. Fiz. PY 1999 PD JUL VL 63 IS 7 GA 251FK J9 IZV AKAD NAUK FIZ UT ISI:000083433800028 ER PT J AU Andreeva, MA Irkaev, SM Semenov, VG Prokhorov, KA Salashchenko, NN Chumakov, AI Ruffer, R TI Moessbauer reflectometry of ultrathin multilayer Zr(10 nm)/[Fe- 57(1.6 nm)/Cr(1.7 nm)x26]/Cr(50 nm) film using synchrotron radiation SO JOURNAL OF ALLOYS AND COMPOUNDS NR 29 AB Time-resolved nuclear resonant reflectivity from ultrathin multilayer Zr(10 nm)/[Fe-57(1.6 nm)/Cr(1.7 nm)x26]/Cr(50 nm) film at grazing incidence angles of synchrotron radiation has been investigated at the Nuclear Resonance Beamline of the European Synchrotron Radiation Facility. For interpretation of the results, complementary measurements of X-ray reflectivity and grazing incidence Moessbauer spectra of reflectivity and secondary electron yield are invoked. Peculiarities and depth- selectivity of the Moessbauer reflectometry method in energy and rime domain are compared. It is shown that using this method the information about top layers of the multilayer structure can be obtained. Computer fitting of the energy and time spectra shows the decreasing of the hyperfine magnetic field in the upper layers of investigated multilayer structure. (C) 1999 Elsevier Science S.A. All rights reserved. CR ALEXANDROV ML, 1992, HYPERFINE INTERACT, V71, P1461 ANDREEVA MA, 1996, HYPERFINE INTERACT, V97-8, P605 ANDREEVA MA, 1995, HYPERFINE INTERACT, V96, P37 ANDREEVA MA, 1995, JETP LETT, V62, P905 ANDREEVA MA, 1998, NIZHNII NOVGOROD, P69 ANDREEVA MA, 1996, PHYS LETT A, V210, P359 ANDREEVA MA, 1991, PHYS STATUS SOLIDI A, V127, P455 ANDREEVA MA, 1999, POVERKHNOST, P59 ANDREEVA MA, 1997, POVERKHNOST, P62 ANDREEVA MA, 1994, ZH EKSP TEOR FIZ+, V105, P1767 BARON AQR, 1996, EUROPHYS LETT, V34, P331 CHECHIN AI, 1983, JETP LETT+, V37, P633 DEAK L, 1994, HYPERFINE INTERACT, V92, P1083 DIFONZO S, 1996, THIN SOLID FILMS, V287, P288 FROST JC, 1985, APPL PHYS LETT, V47, P581 GERDAU E, 1985, PHYS REV LETT, V54, P835 HANNON JP, 1985, PHYS REV B, V32, P5068 IRKAEV SM, 1995, NUCL INSTRUM METH B, V103, P351 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 KLINKHAMMER F, 1996, J MAGN MAGN MATER, V161, P49 NAGY DL, 1997, P 32 ZAK SCH PHYS ZA RUFFER R, 1996, HYPERFINE INTERACT, V97-8, P589 SMIRNOV GV, 1996, HYPERFINE INTERACT, V97-8, P551 SMIRNOV GV, 1997, PHYS REV B, V55, P5811 STURHAHN W, 1996, PHYS REV B, V53, P171 TOELLNER TS, 1995, PHYS REV LETT, V74, P3475 YONEDA Y, 1980, PHYS LETT A, V76, P152 ZHETBAEV AK, 1995, PHASE TRANSITIONS IM TC 3 BP 322 EP 332 PG 11 JI J. Alloy. Compd. PY 1999 PD MAY 5 VL 286 IS 1-2 GA 196DM J9 J ALLOYS COMPOUNDS UT ISI:000080293800057 ER PT J AU Stoev, KN Sakurai, K TI Review on grazing incidence x-ray spectrometry and reflectometry SO SPECTROCHIMICA ACTA PART B-ATOMIC SPECTROSCOPY NR 475 AB Grazing incidence X-ray techniques are now widely used for surface and thin film analysis. The present article overviews the recent advancement since 1993 of the grazing incidence X- ray spectrometry and reflectometry in both theoretical and experimental aspects. Every current topic related to the total reflection X-ray fluorescence spectrometry (TXRF) is described in detail through the introduction of numerous published works on the application in the various fields of the science and industrial technologies. Recent rapid growth in diffuse scattering at grazing incidence as well as in specular reflection is another important scope. The combined measurements of different grazing incidence X-ray techniques might be a future trend for realizing further advanced analysis of the surface and interfaces of materials. (C) 1999 Elsevier Science B.V. All rights reserved. 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PY 1999 PD JAN 4 VL 54 IS 1 GA 180EV J9 SPECTROCHIM ACTA PT B-AT SPEC UT ISI:000079373400005 ER PT J AU Andreeva, MA Gittsovich, VN Irkaev, SM Semenov, VG TI Coherent Mossbauer reflectometry of surfaces SO IZVESTIYA AKADEMII NAUK SERIYA FIZICHESKAYA NR 36 CR ALEXANDROV ML, 1992, HYPERFINE INTERACT, V71, P1461 ALP EE, 1993, PHYS REV LETT, V70, P3351 ANDREEVA MA, 1996, HYPERFINE INTERACT, V97-8, P605 ANDREEVA MA, 1992, JETP LETT, V55, P62 ANDREEVA MA, 1996, MESSBAUEROVSKAYA REN ANDREEVA MA, 1996, PHYS LETT A, V210, P359 ANDREEVA MA, 1991, PHYS STATUS SOLIDI A, V127, P455 ANDREEVA MA, 1995, PISMA ESKP TEOR FIZ, V62, P905 ANDREEVA MA, 1985, POVERKHNOST, P5 ANDREEVA MA, 1986, POVERKHNOST FIZIKA K, P145 ANDREEVA MA, 1994, SOV PHYS JETP, V78, P956 ANDREEVA MA, 1986, VESTN MOSK U FIZ AS+, V27, P57 ANDREEVA MA, 1987, ZH TEKH FIZ+, V57, P2009 BARON AQR, 1994, PHYS REV B, V50, P10354 BERNSTEIN S, 1963, PHYS REV, V132, P1625 BORN M, 1973, OSNOVY OPTIKI BOTTYAN L, 1995, 10 INT C HYP INT LEU, PR89 CHUMAKOV AI, 1996, NUCL INSTRUM METH A, V383, P642 FAIGEL G, 1990, HYPERFINE INTERACT, V58, P242 FROST JC, 1985, APPL PHYS LETT, V47, P581 HANNON JP, 1979, PHYS REV LETT, V43, P636 IRKAEV SM, 1995, NUCL INSTRUM METH B, V103, P351 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 KAGAN Y, 1979, J PHYS C SOLID STATE, V12, P615 PALKIN AB, 1995, ZH TEKH FIZ+, V65, P159 PARRATT LG, 1954, PHYS REV, V95, P359 PONOMAREV YV, 1995, J XRAY SCI TECHNOLOG, V5, P379 ROHLSBERGER R, 1993, Z PHYS B CON MAT, V92, P489 RUFFER R, 1996, HYPERFINE INTERACT, V97-8, P589 RUFFER R, 1991, NUCL INSTRUM METH A, V303, P495 SENTENOV VG, 1997, ICAME 97 RIO DE JAN, V14 SMIRNOV GV, 1996, HYPERFINE INTERACT, V97-8, P551 STURHAHN W, 1994, PHYS REV B, V49, P9285 TOELLNER TS, 1995, PHYS REV LETT, V74, P3475 TRAMMELL GT, 1978, PHYS REV B, V18, P165 TC 1 BP 406 EP 417 PG 12 JI Izv. Akad. Nauk Ser. Fiz. PY 1998 PD FEB VL 62 IS 2 GA ZB563 J9 IZV AKAD NAUK FIZ UT ISI:000072485100028 ER PT J AU Andreeva, MA Irkaev, SM Semenov, VG TI Secondary radiation emission at Mossbauer total external reflection SO HYPERFINE INTERACTIONS NR 42 AB The effects of energy dependence of secondary radiation emission (SRE) followed by nuclear resonant and nonresonant photo-absorption at Mossbauer total external reflection (MTER) have been considered theoretically and checked experimentally. Numerical interpretation of a set of MTER and CEM spectra at different grazing angles has given the depth profiles of electronic density, photoabsorption coefficient and hyperfine interaction variations in 50 nm slightly oxidized Fe-57 film. Empirical functions of photo- and conversion electron yield are also determined. They appeared to be nonsimilar and nonmonotone. The energy dependencies of SRE are recalculated for time domain Mossbauer spectroscopy of synchrotron radiation (SR). 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Radioanal. Nucl. Chem.-Artic. PY 1996 PD JAN VL 202 IS 1-2 GA TY485 J9 J RADIOANAL NUCL CHEM ART UT ISI:A1996TY48500003 ER PT J AU Deak, L Bottyan, L Nagy, DL Spiering, H TI Coherent forward-scattering amplitude in transmission and grazing incidence Mossbauer spectroscopy SO PHYSICAL REVIEW B-CONDENSED MATTER NR 19 AB The theory of both transmission and grazing incidence Mossbauer spectroscopy is reanalyzed. Starting with the nuclear susceptibility tensor a common concise first-order perturbation formulation is given by introducing the forward-scattering amplitude into an anisotropic optical scheme. Formulas of Blume and Kistner as well as those of Andreeva are rederived for the forward-scattering and grazing incidence geometries, respectively. Limitations of several previously intuitively introduced approximations are pointed out. The grazing incidence integral propagation matrices are written in a form built up from 2 x 2 matrix exponentials which is particularly suitable for numerical calculations and practical fitting of both energy domain (conventional source experiment) and time domain (synchrotron radiation experiment) Mossbauer spectra. CR AFANASEV AM, 1965, ZH EKSP TEOR FIZ, V21, P215 ANDREEVA MA, 1982, MESSBAUEROVSKAYA GAM ANDREEVA MA, 1986, POVERKHNOST, V9, P145 ANDREEVA MA, 1994, SOV PHYS JETP, V78, P965 ANDREEVA MA, 1986, VESTN MOSK U FIZ AS+, V27, P57 BLUME M, 1968, PHYS REV, V171, P417 BORZDOV GN, 1976, ZH PRIKL SPEKTROSK, V25, P526 FEDOROV FI, 1976, TEORIYA GIROTROPII FORST JC, 1985, APPL PHYS LETT, V47, P581 HANNON JP, 1969, PHYS REV, V186, P306 HANNON JP, 1968, PHYS REV, V169, P315 HANNON JP, 1985, PHYS REV B, V32, P5068 HANNON JP, 1985, PHYS REV B, V32, P6363 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 LAX M, 1951, REV MOD PHYS, V23, P287 NAGY DL, 1992, HYPERFINE INTERACT, V71, P1349 ROHLSBERGER R, 1994, THESIS U HAMBURG SPIERING H, 1985, HYPERFINE INTERACT, V24, P737 TC 11 BP 6158 EP 6164 PG 7 JI Phys. Rev. B-Condens Matter PY 1996 PD MAR 1 VL 53 IS 10 GA TZ773 J9 PHYS REV B-CONDENSED MATTER UT ISI:A1996TZ77300030 ER PT J AU Andreeva, MA TI Time-differential Mossbauer total external reflection of synchrotron radiation SO PHYSICS LETTERS A NR 14 AB The effect of interference of nuclear resonant and electronic Rayleigh scattering is theoretically treated in time domain Mossbauer total external reflection. The ''interference peak'' recently observed experimentally on the total delayed reflectivity angular curve is explained by the abrupt increasing of the ''initial excitation'' of the resonant sample at the electronic critical angle. The effect of the time dependence of secondary radiation emission followed by nonresonant photoabsorption is predicted. It is shown that it can be used for depth selective structure investigations. CR ANDREEVA MA, 1992, JETP LETT+, V55, P63 ANDREEVA MA, 1994, SOV PHYS JETP, V78, P956 ANDREEVA MA, 1987, ZH TEKH FIZ+, V57, P2009 BARON AQR, 1994, PHYS REV B, V50, P10354 BEDZYK MJ, 1989, PHYS REV LETT, V62, P1376 BERNSTEIN S, 1963, PHYS REV, V132, P1625 CHUMAKOV AI, 1985, ZH EKSP TEOR FIZ+, V89, P1810 DEAK L, 1994, HYPERFINE INTERACT, V92, P1083 HENKE BL, 1972, PHYS REV A-GEN PHYS, V6, P94 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 ISAENKO SA, 1994, PHYS LETT A, V186, P274 KOVALCHUK MV, 1986, USP FIZ NAUK+, V149, P69 TOELLNER TS, 1995, PHYS REV LETT, V74, P3475 WAGNER FE, 1968, Z PHYS, V210, P361 TC 3 BP 359 EP 363 PG 5 JI Phys. Lett. A PY 1996 PD JAN 15 VL 210 IS 4-5 GA TQ229 J9 PHYS LETT A UT ISI:A1996TQ22900022 ER PT J AU IRKAEV, SM ANDREEVA, MA SEMENOV, VG BELOZERSKII, GN GRISHIN, OV TI GRAZING-INCIDENCE MOSSBAUER-SPECTROSCOPY - A NEW METHOD FOR SURFACE-LAYER ANALYSIS .3. INTERPRETATION OF EXPERIMENTAL-DATA SO NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B- BEAM INTERACTIONS WITH MATERIALS AND ATOMS NR 11 AB Quantitative analysis of two sets of experimental GIMS data is presented. A computation procedure, which allows us to determine the distribution versus depth separately for each kind of hyperfine interaction in Fe-57 film for different states of oxidation is described. The result of our analysis shouts that grazing incidence Mossbauer spectroscopy is really a new technique for surface investigation. CR ANDREEVA MA, 1992, JETP LETT, V55, P62 ANDREEVA MA, 1994, ZH EKSP TEOR FIZ+, V105, P1767 AYYUB P, 1988, J PHYS C SOLID STATE, V21, P2229 BOWEN LH, 1979, MOSSBAUER EFFECT REF, V2, P76 DUNHAM WR, 1977, NUCL INSTRUM METHODS, V145, P537 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 ISAENKO SA, 1994, PHYS LETT A, V186, P274 LILJEQUIST D, 1978, NUCL INSTRUM METHODS, V155, P529 MEISEL T, 1977, KEMIA KOZLEMENYEK, V48, P41 STRATMANN M, 1989, CORROS SCI, V29, P1329 TC 4 BP 351 EP 358 PG 8 JI Nucl. Instrum. Methods Phys. Res. Sect. B-Beam Interact. Mater. Atoms PY 1995 PD NOV VL 103 IS 3 GA TF850 J9 NUCL INSTRUM METH PHYS RES B UT ISI:A1995TF85000014 ER PT J AU GITTSOVICH, VN SEMENOV, VG UZDIN, VM TI BULK AND SURFACE MAGNETIC-PROPERTIES OF DILUTE FECR ALLOYS SO JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS NR 34 AB The electronic and magnetic structures of dilute FeCr alloys have been investigated in the framework of the periodic Anderson model. The theory involves only a few phenomenological parameters, which can be determined via magnetic properties of pure Fe and Cr samples. Some examples are considered: the perturbation of magnetic moments of Fe atoms due to Cr impurities both in the bulk and near the surface; the electronic structure of the Cr protective monolayer covering the Fe surface; and the properties of Fe/Cr superlattices. CR ANDERSON PW, 1961, PHYS REV, V124, P41 BAIBICH MN, 1988, PHYS REV LETT, V61, P2472 BARNAS J, 1991, PHYS REV B, V42, P8110 DRITTLER B, 1989, PHYS REV B, V40, P8203 FREEMAN AJ, 1967, HYPERFINE INTERACTIO FREEMAN AJ, 1987, J APPL PHYS, V61, P6741 FREEMAN AJ, 1991, J MAGN MAGN MATER, V100, P497 HASEGAWA H, 1991, PHYS REV B, V43, P10803 HERMAN F, 1991, J APPL PHYS, V69, P4783 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 JUNGBLUT R, 1991, J APPL PHYS, V70, P5923 KAZANSKI AK, 1988, SOV PHYS JETP, V67, P372 KAZANSKII AK, 1990, FIZ TVERD TELA+, V32, P3384 KLEBANOFF LE, 1984, PHYS REV B, V30, P1048 KONDRATEV AS, 1991, FIZ MET METALL NM, V3, P74 KORECKI J, 1985, PHYS REV LETT, V55, P2491 LANG P, 1993, PHYS REV LETT, V71, P1927 OHNISHI S, 1983, PHYS REV B, V28, P6741 PARKIN SSP, 1993, PHYS REV LETT, V71, P1641 PARKIN SSP, 1991, PHYS REV LETT, V67, P3598 SHINJO T, 1991, SURF SCI REP, V12, P49 STOEFFLER D, 1992, J MAGN MAGN MATER, V104, P1819 STOEFFLER D, 1991, J MAGN MAGN MATER, V93, P386 TERAOKA Y, 1977, PHYSICA B & C, V91, P199 TERAOKA Y, 1990, PROG THEOR PHYS, V101, P181 TURTUR C, 1994, PHYS REV LETT, V72, P1557 UNGURIS J, 1991, PHYS REV LETT, V67, P140 VANSCHILFGAARDE M, 1993, PHYS REV LETT, V71, P1923 VANSCHILFGAARDE M, 1993, PHYS REV LETT, V71, P3870 VEGA A, 1992, J MAGN MAGN MATER, V104, P1687 VEGA A, 1994, PHYS REV B, V49, P12797 VICTORA RH, 1985, PHYS REV B, V31, P7335 WALKER TG, 1991, PHYS REV LETT, V69, P1121 TC 8 BP 165 EP 174 PG 10 JI J. Magn. Magn. Mater. PY 1995 PD APR VL 146 IS 1-2 GA QX849 J9 J MAGN MAGN MATER UT ISI:A1995QX84900025 ER PT J AU ANDREEVA, MA BELOZERSKI, GN GRISHIN, OV IRKAEV, SM SEMENOV, VG TI MOSSBAUER TOTAL EXTERNAL REFLECTION - COMPOSITION OF SURFACE- LAYERS SO HYPERFINE INTERACTIONS NR 10 AB An ambiguity of Mossbauer spectra measured under total external reflection conditions due to the increase of the number of parameters which should be determined can be compensated by measuring a series of experimental spectra. The interpretation of all experimental data must be done by means of numerical modeling (or fitting). The method enables us to study phase transformations within a layer of about 10 nm thickness. CR ALEKSANDROV ML, 1992, HYPERFINE INTERACT, V71, P1461 ANDREEVA MA, 1992, JETP LETT, V55, P62 ANDREEVA MA, 1991, PHYS STATUS SOLIDI A, V127, P455 BELOZERSKI GN, 1988, 4 VSES SOV KOG VZAIM, P236 BERNSTEIN S, 1965, J PHYS CHEM SOLIDS, V26, P883 BERNSTEIN S, 1963, PHYS REV, V132, P1625 FROST JC, 1985, APPL PHYS LETT, V47, P581 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 WAGNER FE, 1968, Z PHYS, V210, P361 TC 1 BP 37 EP 49 PG 13 JI Hyperfine Interact. PY 1995 VL 96 IS 1-2 GA QY512 J9 HYPERFINE INTERACTIONS UT ISI:A1995QY51200003 ER PT J AU ANDREEVA, MA IRKAEV, SM SEMENOV, VG TI DETERMINATION OF WORK FUNCTION OF CONVERSION ELECTRONS AND PHOTOELECTRONS BY THE SLIDING MOSSBAUER-SPECTROSCOPY TECHNIQUE SO ZHURNAL EKSPERIMENTALNOI I TEORETICHESKOI FIZIKI NR 28 CR ALEXANDROV ML, 1992, HYPERFINE INTERACT, V71, P1461 ANDREEVA MA, 1991, PHYS STATUS SOLIDI A, V127, P455 ANDREEVA MA, 1992, PISAM ZHETF, V55, P62 ANDREEVA MA, 1986, POVERKHNOST ANDREEVA MA, 1986, VESTN MOSK U FIZ AS+, V27, P57 ANDREEVA MA, 1987, ZH TEKH FIZ, V57, P9 AYYUB P, 1988, J PHYS C SOLID STATE, V21, P2229 BEDZYK MJ, 1989, PHYS REV LETT, V62, P1376 BORZDOV GN, 1976, ZH PRIKL SPEKTROSK, V25, P526 BRETT ME, 1986, J MAGN MAGN MATER, V60, P175 BRONSHTEIN IM, 1969, VTORICHNAYA ELEKTRON BUSHUEV VA, 1990, VTORICHNYE PROTSESSY CHUMAKOV AI, 1985, ZH EKSP TEOR FIZ+, V89, P1810 COWAN PL, 1986, PHYS REV LETT, V57, P2399 HENKE BL, 1972, PHYS REV A-GEN PHYS, V6, P94 IRKAEV SM, 1994, IN PRESS NUCL INCL 3 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 JONES RG, 1982, SURF SCI, V114, P38 KOVALCHUK MV, 1986, FIZ TVERD TELA+, V28, P3409 KOVALCHUK MV, 1986, USP FIZ NAUK+, V149, P69 KRUGLOV MV, 1986, FIZ TVERD TELA+, V28, P322 LILJEQUIST D, 1978, NUCL INSTRUM METHODS, V155, P529 MUKHAMEDZHANOV EK, 1984, POVERKHNOST, P54 NOVAKOVA AA, 1989, MESSBAEROVSKAYA KONV SOLOMIN IK, 1984, FIZ TVERD TELA+, V26, P519 STRATMANN M, 1989, CORROS SCI, V29, P1329 ZABINSKI JS, 1989, NUCL INSTRUM METH B, V42, P379 TC 6 BP 1767 EP 1784 PG 18 JI Zhurnal Eksperimentalnoi Teor. Fiz. PY 1994 PD JUN VL 105 IS 6 GA NX082 J9 ZH EKSP TEOR FIZ UT ISI:A1994NX08200023 ER PT J AU ISAENKO, SA CHUMAKOV, AI SHINKAREV, SI TI STUDIES OF GRAZING-INCIDENCE REFLECTION OF NUCLEAR GAMMA- RADIATION FROM FE-57 FILM SO PHYSICS LETTERS A NR 13 AB Grazing incidence reflection of nuclear gamma-radiation from a 240 angstrom film of Fe-57 has been studied. Mossbauer spectra of scattering were measured in the interval of grazing angles between 3.2 and 6.8 mrad. Almost pure nuclear reflection of resonant radiation at high grazing angle was observed. A theoretical simulation of experimental results made it possible to fit all measured Mossbauer spectra with a single set of sample parameters. An extremely thin layer of Fe2O3 of not more than 4 angstrom thickness was distinguished on the sample surface. CR BARON AQR, COMMUNICATION BARON AQR, 1992, INT C ANOMALOUS SCAT BERNSTEIN S, 1963, PHYS REV, V132, P1625 FROST JC, 1985, APPL PHYS LETT, V47, P581 GROTE M, 1991, EUROPHYS LETT, V17, P707 HANNON JP, 1985, PHYS REV B, V32, P5068 HANNON JP, 1985, PHYS REV B, V32, P6363 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P554 KIKUTA S, 1992, INT C ANOMALOUS SCAT ROHLSBERGER R, 1993, Z PHYS B CON MAT, V92, P489 RUFFER R, 1992, SYNCHR RAD NEWS, V25 WAGNER FE, 1968, Z PHYS, V210, P361 TC 5 BP 274 EP 278 PG 5 JI Phys. Lett. A PY 1994 PD MAR 14 VL 186 IS 3 GA NB668 J9 PHYS LETT A UT ISI:A1994NB66800016 ER PT J AU IRKAEV, SM ANDREEVA, MA SEMENOV, VG BELOZERSKII, GN GRISHIN, OV TI GRAZING-INCIDENCE MOSSBAUER-SPECTROSCOPY - NEW METHOD FOR SURFACE-LAYERS ANALYSIS .2. THEORY OF GRAZING-INCIDENCE MOSSBAUER-SPECTRA SO NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B- BEAM INTERACTIONS WITH MATERIALS AND ATOMS NR 27 AB A general theory of grazing incidence Mossbauer spectroscopy (GIMS) spectra for an inhomogeneous layered medium is presented. The computer simulation based on this theory shows that the shape of the resonant spectrum of the reflected wave intensity, in the case of a resonant film, differs considerably from the case of a semiinfinite resonant mirror. This shape strongly depends on the thickness and the properties of the film and of the nonresonant substrate. The proposed theory of the lineshape of Mossbauer secondary radiation spectra from resonant films takes into account the influence of different types of photo- and conversion electrons on the resulting spectrum. It is shown that the fitting of grazing incidence Mossbauer spectra can be done only by means of numerical simulations. CR ALEKSANDROV PA, 1980, FIZ TVERD TELA+, V22, P2797 ANDREEVA MA, 1992, JETP LETT, V55, P62 ANDREEVA MA, 1982, MOSSBAUEROVSKAYA GAM ANDREEVA MA, 1984, OPT SPEKTROSK+, V56, P546 ANDREEVA MA, 1991, PHYS STATUS SOLIDI A, V127, P455 ANDREEVA MA, 1984, PHYS STATUS SOLIDI B, V125, P461 ANDREEVA MA, 1981, PHYS STATUS SOLIDI B, V103, P193 ANDREEVA MA, 1986, POVERKHNOST, V9, P145 ANDREEVA MA, 1986, VESTN MOSK U FIZ AS+, V27, P57 ANDREEVA MA, 1987, ZH TEKH FIZ+, V57, P2009 ANDREEVA MA, 1983, ZH TEKH FIZ+, V53, P1395 AZZAM RMA, 1977, ELLIPSOMETRY POLARIZ BEDZYK MJ, 1988, NUCL INSTRUM METH A, V266, P679 BERNSTEIN S, 1963, PHYS REV, V132, P1625 BLUME M, 1968, PHYS REV, V171, P417 BORN M, 1968, PRINCIPLES OPTICS BORZDOV GN, 1976, ZH PRIKL SPECTR, V25, P527 FROST JC, 1985, APPL PHYS LETT, V47, P581 HANNON JP, 1985, PHYS REV B, V32, P5068 HANNON JP, 1985, PHYS REV B, V32, P5081 HANNON JP, 1985, PHYS REV B, V32, P6363 HANNON JP, 1985, PHYS REV B, V32, P6374 HANNON JP, 1979, PHYS REV LETT, V43, P636 IRKAEV SM, 1993, NUCL INSTRUM METH B, V74, P545 LILJEQUIST D, 1978, NUCL INSTRUM METHODS, V155, P529 PARRATT LG, 1954, PHYS REV, V95, P359 WAGNER FE, 1968, Z PHYS, V210, P361 TC 14 BP 554 EP 564 PG 11 JI Nucl. Instrum. Methods Phys. Res. Sect. B-Beam Interact. Mater. Atoms PY 1993 PD JUN VL 74 IS 4 GA LG426 J9 NUCL INSTRUM METH PHYS RES B UT ISI:A1993LG42600012 ER