Magnetic Phase Diagrams of YVO^sub 3^ and TbVO^sub 3^ under High Pressure
Magnetic states in R VO ... ( R = Y, Tb) were investigated using low-temperature and high-pressure neutron-diffraction techniques, and the pressure-temperature magnetic phase diagrams were clarified up to 6.2 GPa. We elucidated that, on application of pressure, the magnetic ground state changes from...
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Veröffentlicht in: | Journal of the Physical Society of Japan 2012-02, Vol.81 (2), p.1 |
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creator | Bizen, Daisuke Nakao, Hironori Iwasa, Kazuaki Murakami, Youichi Osakabe, Toyotaka Fujioka, Jun Yasue, Toshio Miyasaka, Shigeki Tokura, Yoshinori |
description | Magnetic states in R VO ... ( R = Y, Tb) were investigated using low-temperature and high-pressure neutron-diffraction techniques, and the pressure-temperature magnetic phase diagrams were clarified up to 6.2 GPa. We elucidated that, on application of pressure, the magnetic ground state changes from C -type spin ordering ( C -SO) to G -type spin ordering ( G -SO); this corresponds to the orbital ground-state switching from G -type orbital ordering ( G -OO) to C -type orbital ordering ( C -OO). It is also interesting that the G -SO transition occurs simultaneously with the C -OO transition, but not with the G -OO one. When the transition temperature of C -OO exceeds that of G -OO under high pressure, the G -OO phase vanishes completely, and a simultaneous spin and orbital order-disorder phase transition occurs. Such a transition is the first case in perovskite-type transition-metal oxides. (ProQuest: ... denotes formulae/symbols omitted.) |
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( R = Y, Tb) were investigated using low-temperature and high-pressure neutron-diffraction techniques, and the pressure-temperature magnetic phase diagrams were clarified up to 6.2 GPa. We elucidated that, on application of pressure, the magnetic ground state changes from C -type spin ordering ( C -SO) to G -type spin ordering ( G -SO); this corresponds to the orbital ground-state switching from G -type orbital ordering ( G -OO) to C -type orbital ordering ( C -OO). It is also interesting that the G -SO transition occurs simultaneously with the C -OO transition, but not with the G -OO one. When the transition temperature of C -OO exceeds that of G -OO under high pressure, the G -OO phase vanishes completely, and a simultaneous spin and orbital order-disorder phase transition occurs. Such a transition is the first case in perovskite-type transition-metal oxides. 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( R = Y, Tb) were investigated using low-temperature and high-pressure neutron-diffraction techniques, and the pressure-temperature magnetic phase diagrams were clarified up to 6.2 GPa. We elucidated that, on application of pressure, the magnetic ground state changes from C -type spin ordering ( C -SO) to G -type spin ordering ( G -SO); this corresponds to the orbital ground-state switching from G -type orbital ordering ( G -OO) to C -type orbital ordering ( C -OO). It is also interesting that the G -SO transition occurs simultaneously with the C -OO transition, but not with the G -OO one. When the transition temperature of C -OO exceeds that of G -OO under high pressure, the G -OO phase vanishes completely, and a simultaneous spin and orbital order-disorder phase transition occurs. Such a transition is the first case in perovskite-type transition-metal oxides. 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( R = Y, Tb) were investigated using low-temperature and high-pressure neutron-diffraction techniques, and the pressure-temperature magnetic phase diagrams were clarified up to 6.2 GPa. We elucidated that, on application of pressure, the magnetic ground state changes from C -type spin ordering ( C -SO) to G -type spin ordering ( G -SO); this corresponds to the orbital ground-state switching from G -type orbital ordering ( G -OO) to C -type orbital ordering ( C -OO). It is also interesting that the G -SO transition occurs simultaneously with the C -OO transition, but not with the G -OO one. When the transition temperature of C -OO exceeds that of G -OO under high pressure, the G -OO phase vanishes completely, and a simultaneous spin and orbital order-disorder phase transition occurs. Such a transition is the first case in perovskite-type transition-metal oxides. (ProQuest: ... denotes formulae/symbols omitted.)</abstract><cop>Tokyo</cop><pub>The Physical Society of Japan</pub></addata></record> |
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subjects | Diffraction Low temperature physics Magnetic fields Neutrons Perovskite Phase transitions Pressure |
title | Magnetic Phase Diagrams of YVO^sub 3^ and TbVO^sub 3^ under High Pressure |
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