Susceptibility and 89Y nuclear magnetic resonance in Y1− x Ca x VO3
Temperature-dependent (10–300 K) field-cooled (FC) and zero-field-cooled (ZFC) susceptibilities, and 89Y NMR spectra and relaxation in Y1−xCaxVO3 with 0≤x≤0.9 are reported. In the paramagnetic phase (PA) of YVO3 and for T≥120 K the susceptibility χ is of antiferromagnetic (AF) type, with no field de...
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Veröffentlicht in: | Journal of applied physics 1996-04, Vol.79 (8), p.6624-6626 |
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creator | Cintolesi, F. Corti, M. Rigamonti, A. Rossetti, G. Ghigna, P. Lascialfari, A. |
description | Temperature-dependent (10–300 K) field-cooled (FC) and zero-field-cooled (ZFC) susceptibilities, and 89Y NMR spectra and relaxation in Y1−xCaxVO3 with 0≤x≤0.9 are reported. In the paramagnetic phase (PA) of YVO3 and for T≥120 K the susceptibility χ is of antiferromagnetic (AF) type, with no field dependence. Around the Neel temperature T(1)N=113±1 K a field-dependent ferromagnetic behavior is observed under FC condition. Below T(2)N≂77 K (AF phase with AF interplane coupling) strong difference is present between FC and ZFC χ’s. For T→T(1)+N the 89Y NMR line shows marked broadening and no measurable shift, consistent with a dominant dipolar contribution in the nucleus–electrons interaction. The 89Y relaxation rate T−11, related to the correlated spin dynamics of V3+ S(t), seems to indicate that the interplane ferromagnetic symmetry of the spin fluctuations is quenched in strong fields. The peculiar findings for χ and T1 could result from a field-dependent weak ferromagnetism of Dzyaloshinsky–Moriya character. In Y1−xCaxVO3, χ and T−11 decrease on increasing x, still preserving the qualitative behavior as for x=0. For x≂0.6 (Ca concentration which drives the transition to the metallic phase) the marks of the PA–AF transition are practically suppressed and behaviors characteristic of correlated metals are observed. |
doi_str_mv | 10.1063/1.361904 |
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In the paramagnetic phase (PA) of YVO3 and for T≥120 K the susceptibility χ is of antiferromagnetic (AF) type, with no field dependence. Around the Neel temperature T(1)N=113±1 K a field-dependent ferromagnetic behavior is observed under FC condition. Below T(2)N≂77 K (AF phase with AF interplane coupling) strong difference is present between FC and ZFC χ’s. For T→T(1)+N the 89Y NMR line shows marked broadening and no measurable shift, consistent with a dominant dipolar contribution in the nucleus–electrons interaction. The 89Y relaxation rate T−11, related to the correlated spin dynamics of V3+ S(t), seems to indicate that the interplane ferromagnetic symmetry of the spin fluctuations is quenched in strong fields. The peculiar findings for χ and T1 could result from a field-dependent weak ferromagnetism of Dzyaloshinsky–Moriya character. In Y1−xCaxVO3, χ and T−11 decrease on increasing x, still preserving the qualitative behavior as for x=0. For x≂0.6 (Ca concentration which drives the transition to the metallic phase) the marks of the PA–AF transition are practically suppressed and behaviors characteristic of correlated metals are observed.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.361904</identifier><language>eng</language><ispartof>Journal of applied physics, 1996-04, Vol.79 (8), p.6624-6626</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c724-e4c3384bcc787599bc594fdfe430dcb89dbf51f07964917e935be7d711c8753f3</citedby><cites>FETCH-LOGICAL-c724-e4c3384bcc787599bc594fdfe430dcb89dbf51f07964917e935be7d711c8753f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Cintolesi, F.</creatorcontrib><creatorcontrib>Corti, M.</creatorcontrib><creatorcontrib>Rigamonti, A.</creatorcontrib><creatorcontrib>Rossetti, G.</creatorcontrib><creatorcontrib>Ghigna, P.</creatorcontrib><creatorcontrib>Lascialfari, A.</creatorcontrib><title>Susceptibility and 89Y nuclear magnetic resonance in Y1− x Ca x VO3</title><title>Journal of applied physics</title><description>Temperature-dependent (10–300 K) field-cooled (FC) and zero-field-cooled (ZFC) susceptibilities, and 89Y NMR spectra and relaxation in Y1−xCaxVO3 with 0≤x≤0.9 are reported. In the paramagnetic phase (PA) of YVO3 and for T≥120 K the susceptibility χ is of antiferromagnetic (AF) type, with no field dependence. Around the Neel temperature T(1)N=113±1 K a field-dependent ferromagnetic behavior is observed under FC condition. Below T(2)N≂77 K (AF phase with AF interplane coupling) strong difference is present between FC and ZFC χ’s. For T→T(1)+N the 89Y NMR line shows marked broadening and no measurable shift, consistent with a dominant dipolar contribution in the nucleus–electrons interaction. The 89Y relaxation rate T−11, related to the correlated spin dynamics of V3+ S(t), seems to indicate that the interplane ferromagnetic symmetry of the spin fluctuations is quenched in strong fields. The peculiar findings for χ and T1 could result from a field-dependent weak ferromagnetism of Dzyaloshinsky–Moriya character. In Y1−xCaxVO3, χ and T−11 decrease on increasing x, still preserving the qualitative behavior as for x=0. 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In the paramagnetic phase (PA) of YVO3 and for T≥120 K the susceptibility χ is of antiferromagnetic (AF) type, with no field dependence. Around the Neel temperature T(1)N=113±1 K a field-dependent ferromagnetic behavior is observed under FC condition. Below T(2)N≂77 K (AF phase with AF interplane coupling) strong difference is present between FC and ZFC χ’s. For T→T(1)+N the 89Y NMR line shows marked broadening and no measurable shift, consistent with a dominant dipolar contribution in the nucleus–electrons interaction. The 89Y relaxation rate T−11, related to the correlated spin dynamics of V3+ S(t), seems to indicate that the interplane ferromagnetic symmetry of the spin fluctuations is quenched in strong fields. The peculiar findings for χ and T1 could result from a field-dependent weak ferromagnetism of Dzyaloshinsky–Moriya character. In Y1−xCaxVO3, χ and T−11 decrease on increasing x, still preserving the qualitative behavior as for x=0. For x≂0.6 (Ca concentration which drives the transition to the metallic phase) the marks of the PA–AF transition are practically suppressed and behaviors characteristic of correlated metals are observed.</abstract><doi>10.1063/1.361904</doi><tpages>3</tpages></addata></record> |
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title | Susceptibility and 89Y nuclear magnetic resonance in Y1− x Ca x VO3 |
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