Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1

Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An...
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Autor*in:	Akselrod, Z. Z. [verfasserIn] Budzynski, M. [verfasserIn] Kharzatov, T. [verfasserIn] Komissarova, B. A. [verfasserIn] Kryukova, L. N. [verfasserIn] Reiman, S. I. [verfasserIn] Ryasny, G. K. [verfasserIn] Sorokin, A. A. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	1983

Schlagwörter:	Field Component Hyperfine Field Bulk Magnetization Inequivalent Site Lave Compound

Übergeordnetes Werk:	Enthalten in: Hyperfine interactions - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975, 14(1983), 1 vom: Apr., Seite 7-19
Übergeordnetes Werk:	volume:14 ; year:1983 ; number:1 ; month:04 ; pages:7-19

Links:	Volltext

DOI / URN:	10.1007/BF02098292

Katalog-ID:	SPR012985686

Internformat


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245	1	0	\|a Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1
264		1	\|c 1983
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520			\|a Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe).
650		4	\|a Field Component \|7 (dpeaa)DE-He213
650		4	\|a Hyperfine Field \|7 (dpeaa)DE-He213
650		4	\|a Bulk Magnetization \|7 (dpeaa)DE-He213
650		4	\|a Inequivalent Site \|7 (dpeaa)DE-He213
650		4	\|a Lave Compound \|7 (dpeaa)DE-He213
700	1		\|a Budzynski, M. \|e verfasserin \|4 aut
700	1		\|a Kharzatov, T. \|e verfasserin \|4 aut
700	1		\|a Komissarova, B. A. \|e verfasserin \|4 aut
700	1		\|a Kryukova, L. N. \|e verfasserin \|4 aut
700	1		\|a Reiman, S. I. \|e verfasserin \|4 aut
700	1		\|a Ryasny, G. K. \|e verfasserin \|4 aut
700	1		\|a Sorokin, A. A. \|e verfasserin \|4 aut
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936	b	k	\|a 33.00 \|q ASE
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952			\|d 14 \|j 1983 \|e 1 \|c 04 \|h 7-19

Indexfelder

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allfields	10.1007/BF02098292 doi (DE-627)SPR012985686 (SPR)BF02098292-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Akselrod, Z. Z. verfasserin aut Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1 1983 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe). Field Component (dpeaa)DE-He213 Hyperfine Field (dpeaa)DE-He213 Bulk Magnetization (dpeaa)DE-He213 Inequivalent Site (dpeaa)DE-He213 Lave Compound (dpeaa)DE-He213 Budzynski, M. verfasserin aut Kharzatov, T. verfasserin aut Komissarova, B. A. verfasserin aut Kryukova, L. N. verfasserin aut Reiman, S. I. verfasserin aut Ryasny, G. K. verfasserin aut Sorokin, A. A. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 14(1983), 1 vom: Apr., Seite 7-19 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:14 year:1983 number:1 month:04 pages:7-19 https://dx.doi.org/10.1007/BF02098292 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_224 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2018 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2152 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_2808 GBV_ILN_4246 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4326 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4700 GBV_ILN_4753 33.00 ASE AR 14 1983 1 04 7-19
spelling	10.1007/BF02098292 doi (DE-627)SPR012985686 (SPR)BF02098292-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Akselrod, Z. Z. verfasserin aut Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1 1983 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe). Field Component (dpeaa)DE-He213 Hyperfine Field (dpeaa)DE-He213 Bulk Magnetization (dpeaa)DE-He213 Inequivalent Site (dpeaa)DE-He213 Lave Compound (dpeaa)DE-He213 Budzynski, M. verfasserin aut Kharzatov, T. verfasserin aut Komissarova, B. A. verfasserin aut Kryukova, L. N. verfasserin aut Reiman, S. I. verfasserin aut Ryasny, G. K. verfasserin aut Sorokin, A. A. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 14(1983), 1 vom: Apr., Seite 7-19 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:14 year:1983 number:1 month:04 pages:7-19 https://dx.doi.org/10.1007/BF02098292 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_224 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2018 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2152 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_2808 GBV_ILN_4246 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4326 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4700 GBV_ILN_4753 33.00 ASE AR 14 1983 1 04 7-19
allfields_unstemmed	10.1007/BF02098292 doi (DE-627)SPR012985686 (SPR)BF02098292-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Akselrod, Z. Z. verfasserin aut Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1 1983 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe). Field Component (dpeaa)DE-He213 Hyperfine Field (dpeaa)DE-He213 Bulk Magnetization (dpeaa)DE-He213 Inequivalent Site (dpeaa)DE-He213 Lave Compound (dpeaa)DE-He213 Budzynski, M. verfasserin aut Kharzatov, T. verfasserin aut Komissarova, B. A. verfasserin aut Kryukova, L. N. verfasserin aut Reiman, S. I. verfasserin aut Ryasny, G. K. verfasserin aut Sorokin, A. A. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 14(1983), 1 vom: Apr., Seite 7-19 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:14 year:1983 number:1 month:04 pages:7-19 https://dx.doi.org/10.1007/BF02098292 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_224 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2018 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2152 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_2808 GBV_ILN_4246 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4326 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4700 GBV_ILN_4753 33.00 ASE AR 14 1983 1 04 7-19
allfieldsGer	10.1007/BF02098292 doi (DE-627)SPR012985686 (SPR)BF02098292-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Akselrod, Z. Z. verfasserin aut Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1 1983 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe). Field Component (dpeaa)DE-He213 Hyperfine Field (dpeaa)DE-He213 Bulk Magnetization (dpeaa)DE-He213 Inequivalent Site (dpeaa)DE-He213 Lave Compound (dpeaa)DE-He213 Budzynski, M. verfasserin aut Kharzatov, T. verfasserin aut Komissarova, B. A. verfasserin aut Kryukova, L. N. verfasserin aut Reiman, S. I. verfasserin aut Ryasny, G. K. verfasserin aut Sorokin, A. A. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 14(1983), 1 vom: Apr., Seite 7-19 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:14 year:1983 number:1 month:04 pages:7-19 https://dx.doi.org/10.1007/BF02098292 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_224 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2018 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2152 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_2808 GBV_ILN_4246 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4326 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4700 GBV_ILN_4753 33.00 ASE AR 14 1983 1 04 7-19
allfieldsSound	10.1007/BF02098292 doi (DE-627)SPR012985686 (SPR)BF02098292-e DE-627 ger DE-627 rakwb eng 530 ASE 33.00 bkl Akselrod, Z. Z. verfasserin aut Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1 1983 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe). Field Component (dpeaa)DE-He213 Hyperfine Field (dpeaa)DE-He213 Bulk Magnetization (dpeaa)DE-He213 Inequivalent Site (dpeaa)DE-He213 Lave Compound (dpeaa)DE-He213 Budzynski, M. verfasserin aut Kharzatov, T. verfasserin aut Komissarova, B. A. verfasserin aut Kryukova, L. N. verfasserin aut Reiman, S. I. verfasserin aut Ryasny, G. K. verfasserin aut Sorokin, A. A. verfasserin aut Enthalten in Hyperfine interactions Dordrecht [u.a.] : Springer Science + Business Media B.V, 1975 14(1983), 1 vom: Apr., Seite 7-19 (DE-627)320612953 (DE-600)2021614-2 1572-9540 nnns volume:14 year:1983 number:1 month:04 pages:7-19 https://dx.doi.org/10.1007/BF02098292 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_224 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2018 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2152 GBV_ILN_2158 GBV_ILN_2188 GBV_ILN_2193 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_2808 GBV_ILN_4246 GBV_ILN_4251 GBV_ILN_4277 GBV_ILN_4326 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4700 GBV_ILN_4753 33.00 ASE AR 14 1983 1 04 7-19
language	English
source	Enthalten in Hyperfine interactions 14(1983), 1 vom: Apr., Seite 7-19 volume:14 year:1983 number:1 month:04 pages:7-19
sourceStr	Enthalten in Hyperfine interactions 14(1983), 1 vom: Apr., Seite 7-19 volume:14 year:1983 number:1 month:04 pages:7-19
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Field Component Hyperfine Field Bulk Magnetization Inequivalent Site Lave Compound
dewey-raw	530
isfreeaccess_bool	false
container_title	Hyperfine interactions
authorswithroles_txt_mv	Akselrod, Z. Z. @@aut@@ Budzynski, M. @@aut@@ Kharzatov, T. @@aut@@ Komissarova, B. A. @@aut@@ Kryukova, L. N. @@aut@@ Reiman, S. I. @@aut@@ Ryasny, G. K. @@aut@@ Sorokin, A. A. @@aut@@
publishDateDaySort_date	1983-04-01T00:00:00Z
hierarchy_top_id	320612953
dewey-sort	3530
id	SPR012985686
language_de	englisch
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author	Akselrod, Z. Z.
spellingShingle	Akselrod, Z. Z. ddc 530 bkl 33.00 misc Field Component misc Hyperfine Field misc Bulk Magnetization misc Inequivalent Site misc Lave Compound Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1
authorStr	Akselrod, Z. Z.
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topic_title	530 ASE 33.00 bkl Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1 Field Component (dpeaa)DE-He213 Hyperfine Field (dpeaa)DE-He213 Bulk Magnetization (dpeaa)DE-He213 Inequivalent Site (dpeaa)DE-He213 Lave Compound (dpeaa)DE-He213
topic	ddc 530 bkl 33.00 misc Field Component misc Hyperfine Field misc Bulk Magnetization misc Inequivalent Site misc Lave Compound
topic_unstemmed	ddc 530 bkl 33.00 misc Field Component misc Hyperfine Field misc Bulk Magnetization misc Inequivalent Site misc Lave Compound
topic_browse	ddc 530 bkl 33.00 misc Field Component misc Hyperfine Field misc Bulk Magnetization misc Inequivalent Site misc Lave Compound
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
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title	Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1
ctrlnum	(DE-627)SPR012985686 (SPR)BF02098292-e
title_full	Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1
author_sort	Akselrod, Z. Z.
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author_browse	Akselrod, Z. Z. Budzynski, M. Kharzatov, T. Komissarova, B. A. Kryukova, L. N. Reiman, S. I. Ryasny, G. K. Sorokin, A. A.
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author-letter	Akselrod, Z. Z.
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title_sort	measurements of the hyperfine magnetic fields at ta and fe in the laves compounds ($ zr_{x} $ $ hf_{1−x} $)$ fe_{2} $ for 0≤x≤1
title_auth	Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1
abstract	Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe).
abstractGer	Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe).
abstract_unstemmed	Abstract The hyperfine magnetic fields $ at^{181} $Ta $ and^{57} $Fe in the ferromagnetic Laves intermetallic compounds ($ Zr_{x} %$ Hf_{1−x} $)$ Fe_{2} $ (0≤x≤1) have been measured by the methods of TDPAC and Mössbauer effect, respectively, and shown to be practically independent of x at x≥0.4. An average value $ B_{hf} $ (Ta)=−6.52 T at 300 K was obtained for samples with x≥0.4, and −14.2 T for pure $ HfFe_{2} $ in the hexagonal C14 modification. For 0<x<0.4, a superposition of both field components was observed. A deviation of the temperature dependence of $ B_{hf} $(Ta) in ($ Zr_{0.9} $ $ Hf_{0.1} $)$ Fe_{2} $ from that for $ B_{hf} $ (Fe) and the bulk magnetization was confirmed, studied in detail, and shown to exist for all x≥0.4. The temperature dependence of $ B_{hf} $(Ta) in $ HfFe_{2} $ was close to that of $ B_{hf} $ (Fe).
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title_short	Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1
url	https://dx.doi.org/10.1007/BF02098292
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author2	Budzynski, M. Kharzatov, T. Komissarova, B. A. Kryukova, L. N. Reiman, S. I. Ryasny, G. K. Sorokin, A. A.
author2Str	Budzynski, M. Kharzatov, T. Komissarova, B. A. Kryukova, L. N. Reiman, S. I. Ryasny, G. K. Sorokin, A. A.
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up_date	2024-07-03T16:40:43.642Z
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Measurements of the hyperfine magnetic fields at Ta and Fe in the Laves compounds ($ Zr_{x} $ $ Hf_{1−x} $)$ Fe_{2} $ for 0≤x≤1

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