Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties
Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. The...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Raveau, B. [verfasserIn] Motin Seikh, M. D. [verfasserIn] Pralong, V. [verfasserIn] Caignaert, V. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2009 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Bulletin of materials science - Bangalore, 1979, 32(2009), 3 vom: Juni, Seite 305-312 |
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| Übergeordnetes Werk: |
volume:32 ; year:2009 ; number:3 ; month:06 ; pages:305-312 |
| Links: |
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| DOI / URN: |
10.1007/s12034-009-0044-6 |
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| Katalog-ID: |
SPR023922974 |
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| 245 | 1 | 0 | |a Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties |
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| 520 | |a Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. | ||
| 650 | 4 | |a Ordered oxygen deficient perovskites |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a ‘112’ cobaltites |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a ferromagnetic cobaltites |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a phase separation |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a magnetic transitions |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a magnetoresistive cobaltites |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Motin Seikh, M. D. |e verfasserin |4 aut | |
| 700 | 1 | |a Pralong, V. |e verfasserin |4 aut | |
| 700 | 1 | |a Caignaert, V. |e verfasserin |4 aut | |
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10.1007/s12034-009-0044-6 doi (DE-627)SPR023922974 (SPR)s12034-009-0044-6-e DE-627 ger DE-627 rakwb eng 600 ASE 51.00 bkl Raveau, B. verfasserin aut Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. Ordered oxygen deficient perovskites (dpeaa)DE-He213 ‘112’ cobaltites (dpeaa)DE-He213 ferromagnetic cobaltites (dpeaa)DE-He213 phase separation (dpeaa)DE-He213 magnetic transitions (dpeaa)DE-He213 magnetoresistive cobaltites (dpeaa)DE-He213 Motin Seikh, M. D. verfasserin aut Pralong, V. verfasserin aut Caignaert, V. verfasserin aut Enthalten in Bulletin of materials science Bangalore, 1979 32(2009), 3 vom: Juni, Seite 305-312 (DE-627)358454425 (DE-600)2096424-9 0973-7669 nnns volume:32 year:2009 number:3 month:06 pages:305-312 https://dx.doi.org/10.1007/s12034-009-0044-6 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 32 2009 3 06 305-312 |
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10.1007/s12034-009-0044-6 doi (DE-627)SPR023922974 (SPR)s12034-009-0044-6-e DE-627 ger DE-627 rakwb eng 600 ASE 51.00 bkl Raveau, B. verfasserin aut Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. Ordered oxygen deficient perovskites (dpeaa)DE-He213 ‘112’ cobaltites (dpeaa)DE-He213 ferromagnetic cobaltites (dpeaa)DE-He213 phase separation (dpeaa)DE-He213 magnetic transitions (dpeaa)DE-He213 magnetoresistive cobaltites (dpeaa)DE-He213 Motin Seikh, M. D. verfasserin aut Pralong, V. verfasserin aut Caignaert, V. verfasserin aut Enthalten in Bulletin of materials science Bangalore, 1979 32(2009), 3 vom: Juni, Seite 305-312 (DE-627)358454425 (DE-600)2096424-9 0973-7669 nnns volume:32 year:2009 number:3 month:06 pages:305-312 https://dx.doi.org/10.1007/s12034-009-0044-6 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 32 2009 3 06 305-312 |
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10.1007/s12034-009-0044-6 doi (DE-627)SPR023922974 (SPR)s12034-009-0044-6-e DE-627 ger DE-627 rakwb eng 600 ASE 51.00 bkl Raveau, B. verfasserin aut Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. Ordered oxygen deficient perovskites (dpeaa)DE-He213 ‘112’ cobaltites (dpeaa)DE-He213 ferromagnetic cobaltites (dpeaa)DE-He213 phase separation (dpeaa)DE-He213 magnetic transitions (dpeaa)DE-He213 magnetoresistive cobaltites (dpeaa)DE-He213 Motin Seikh, M. D. verfasserin aut Pralong, V. verfasserin aut Caignaert, V. verfasserin aut Enthalten in Bulletin of materials science Bangalore, 1979 32(2009), 3 vom: Juni, Seite 305-312 (DE-627)358454425 (DE-600)2096424-9 0973-7669 nnns volume:32 year:2009 number:3 month:06 pages:305-312 https://dx.doi.org/10.1007/s12034-009-0044-6 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 32 2009 3 06 305-312 |
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10.1007/s12034-009-0044-6 doi (DE-627)SPR023922974 (SPR)s12034-009-0044-6-e DE-627 ger DE-627 rakwb eng 600 ASE 51.00 bkl Raveau, B. verfasserin aut Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. Ordered oxygen deficient perovskites (dpeaa)DE-He213 ‘112’ cobaltites (dpeaa)DE-He213 ferromagnetic cobaltites (dpeaa)DE-He213 phase separation (dpeaa)DE-He213 magnetic transitions (dpeaa)DE-He213 magnetoresistive cobaltites (dpeaa)DE-He213 Motin Seikh, M. D. verfasserin aut Pralong, V. verfasserin aut Caignaert, V. verfasserin aut Enthalten in Bulletin of materials science Bangalore, 1979 32(2009), 3 vom: Juni, Seite 305-312 (DE-627)358454425 (DE-600)2096424-9 0973-7669 nnns volume:32 year:2009 number:3 month:06 pages:305-312 https://dx.doi.org/10.1007/s12034-009-0044-6 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 32 2009 3 06 305-312 |
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10.1007/s12034-009-0044-6 doi (DE-627)SPR023922974 (SPR)s12034-009-0044-6-e DE-627 ger DE-627 rakwb eng 600 ASE 51.00 bkl Raveau, B. verfasserin aut Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. Ordered oxygen deficient perovskites (dpeaa)DE-He213 ‘112’ cobaltites (dpeaa)DE-He213 ferromagnetic cobaltites (dpeaa)DE-He213 phase separation (dpeaa)DE-He213 magnetic transitions (dpeaa)DE-He213 magnetoresistive cobaltites (dpeaa)DE-He213 Motin Seikh, M. D. verfasserin aut Pralong, V. verfasserin aut Caignaert, V. verfasserin aut Enthalten in Bulletin of materials science Bangalore, 1979 32(2009), 3 vom: Juni, Seite 305-312 (DE-627)358454425 (DE-600)2096424-9 0973-7669 nnns volume:32 year:2009 number:3 month:06 pages:305-312 https://dx.doi.org/10.1007/s12034-009-0044-6 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_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 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_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 51.00 ASE AR 32 2009 3 06 305-312 |
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Enthalten in Bulletin of materials science 32(2009), 3 vom: Juni, Seite 305-312 volume:32 year:2009 number:3 month:06 pages:305-312 |
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Raveau, B. @@aut@@ Motin Seikh, M. D. @@aut@@ Pralong, V. @@aut@@ Caignaert, V. @@aut@@ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR023922974</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111110404.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2009 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s12034-009-0044-6</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR023922974</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s12034-009-0044-6-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">600</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">51.00</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Raveau, B.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2009</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Ordered oxygen deficient perovskites</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">‘112’ cobaltites</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">ferromagnetic cobaltites</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">phase separation</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">magnetic transitions</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">magnetoresistive cobaltites</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Motin Seikh, M. 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Raveau, B. |
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Raveau, B. ddc 600 bkl 51.00 misc Ordered oxygen deficient perovskites misc ‘112’ cobaltites misc ferromagnetic cobaltites misc phase separation misc magnetic transitions misc magnetoresistive cobaltites Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties |
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600 ASE 51.00 bkl Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties Ordered oxygen deficient perovskites (dpeaa)DE-He213 ‘112’ cobaltites (dpeaa)DE-He213 ferromagnetic cobaltites (dpeaa)DE-He213 phase separation (dpeaa)DE-He213 magnetic transitions (dpeaa)DE-He213 magnetoresistive cobaltites (dpeaa)DE-He213 |
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ddc 600 bkl 51.00 misc Ordered oxygen deficient perovskites misc ‘112’ cobaltites misc ferromagnetic cobaltites misc phase separation misc magnetic transitions misc magnetoresistive cobaltites |
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ddc 600 bkl 51.00 misc Ordered oxygen deficient perovskites misc ‘112’ cobaltites misc ferromagnetic cobaltites misc phase separation misc magnetic transitions misc magnetoresistive cobaltites |
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Raveau, B. Motin Seikh, M. D. Pralong, V. Caignaert, V. |
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ordered oxygen deficient ‘112’ perovskites, $ lnbaco_{2} %$ o_{5·50+δ} $: complex magnetism and transport properties |
| title_auth |
Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties |
| abstract |
Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. |
| abstractGer |
Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. |
| abstract_unstemmed |
Abstract The ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $ (Ln = lanthanide or Y), exhibit a very flexible structure which can either uptake (δ > 0) or release oxygen (δ < 0) depending on the experimental conditions of synthesis and on the size of the lanthanide. These compounds exhibit remarkably complex magnetic transitions, metal-insulator transition and exceptionally high magnetoresistance. We show herein that their physics is mainly dominated by three different ferromagnetic states, depending on the cobalt valency: FM1 for δ = 0 ($ Co^{3+} $), FM2 for δ < 0 ($ Co^{2+} $/$ Co^{3+} $) and FM3 for δ > 0 ($ Co^{3+} $/$ Co^{4+} $). The competition between ferromagnetism and antiferromagnetism in these phases and the various transitions are discussed taking into consideration the spin state of cobalt, the issue of phase separation and the effect of cobalt coordination and disproportionation. |
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| title_short |
Ordered oxygen deficient ‘112’ perovskites, $ LnBaCo_{2} %$ O_{5·50+δ} $: complex magnetism and transport properties |
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https://dx.doi.org/10.1007/s12034-009-0044-6 |
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Motin Seikh, M. D. Pralong, V. Caignaert, V. |
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10.1007/s12034-009-0044-6 |
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2024-07-03T22:20:56.352Z |
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| score |
7.398299 |