Magnetic field and pressure effects on the spin frustrated systems NaV2O4 and Cu2OSeO3

碩士 === 國立中山大學 === 物理學系研究所 === 98 === In the geometrical spin frustrated systems, order-disorder phenomena are interesting, for their intrinsic fluctuation, complicated completing interactions, and lattice structure leading to many intrigue physical behavior. To clarify the mechanism of such systems,...

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Main Authors: Kuo-feng Tseng, 曾國峯
Other Authors: Hung-Duen Yang
Format: Others
Language:en_US
Published: 2010
Online Access:http://ndltd.ncl.edu.tw/handle/77310348245038349602
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spelling ndltd-TW-098NSYS51980162015-10-13T18:39:46Z http://ndltd.ncl.edu.tw/handle/77310348245038349602 Magnetic field and pressure effects on the spin frustrated systems NaV2O4 and Cu2OSeO3 自旋不穩態系統鈉釩氧及硒銅氧於磁場及壓力下的研究 Kuo-feng Tseng 曾國峯 碩士 國立中山大學 物理學系研究所 98 In the geometrical spin frustrated systems, order-disorder phenomena are interesting, for their intrinsic fluctuation, complicated completing interactions, and lattice structure leading to many intrigue physical behavior. To clarify the mechanism of such systems, experiments under extreme conditions (diverse magnetic fields and hydrostatic pressures) are powerful tools to meet the needs. In this dissertation, two kind of interesting materials are investigated. One is quasi-1D double chain antiferromagnet NaV2O4, the other is cubic like ferrimagnet Cu2OSeO3. In the polycrystalline compound NaV2O4, it exhibits an antiferromagnetic transition TN at 140 K, together with two field dependence subphases at 1 T≤H≤5 T. The two characteristic temperature TN1 and TN2 are associated to two subphases, which is determined by the peak position in the derivative of magnetization with respect to temperature. Under magnetic field, TN and TN1 remain almost unchanged (linear behavior), while TN2 acts in a nonlinear behavior with the application of magnetic field. Further, TN1 and TN2 are found to decrease roughly linear with applied pressure, while TN2 follows a nonlinear relation with applied pressure. On the other hand, the cubic single crystal Cu2OSeO3 exhibits a ferrimagnetic transition at 58 K, which is shifting to high temperature range with increasing magnetic fields. The peak values (from the mutual inductance measurements) associated with the ferrimagnetic transitions also increase with applied hydrostatic pressures. Moreover, the spin-flipped transitions are observed below transition temperature at ambient and applied pressure (12.67 kbar). The measurements above strongly suggested the ferrimagnetic spin configurations order earlier, i.e. transition temperatures increase with applied magnetic fields and pressures. In summary, the investigated frustrated spin systems (NaV2O4 and Cu2OSeO3) behave with the same trend with applied magnetic fields and hydrostatic pressures. It is possibly induced by the external DC magnetic field and the structure change and/or deformation under pressure. Hung-Duen Yang 楊弘敦 2010 學位論文 ; thesis 75 en_US
collection NDLTD
language en_US
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description 碩士 === 國立中山大學 === 物理學系研究所 === 98 === In the geometrical spin frustrated systems, order-disorder phenomena are interesting, for their intrinsic fluctuation, complicated completing interactions, and lattice structure leading to many intrigue physical behavior. To clarify the mechanism of such systems, experiments under extreme conditions (diverse magnetic fields and hydrostatic pressures) are powerful tools to meet the needs. In this dissertation, two kind of interesting materials are investigated. One is quasi-1D double chain antiferromagnet NaV2O4, the other is cubic like ferrimagnet Cu2OSeO3. In the polycrystalline compound NaV2O4, it exhibits an antiferromagnetic transition TN at 140 K, together with two field dependence subphases at 1 T≤H≤5 T. The two characteristic temperature TN1 and TN2 are associated to two subphases, which is determined by the peak position in the derivative of magnetization with respect to temperature. Under magnetic field, TN and TN1 remain almost unchanged (linear behavior), while TN2 acts in a nonlinear behavior with the application of magnetic field. Further, TN1 and TN2 are found to decrease roughly linear with applied pressure, while TN2 follows a nonlinear relation with applied pressure. On the other hand, the cubic single crystal Cu2OSeO3 exhibits a ferrimagnetic transition at 58 K, which is shifting to high temperature range with increasing magnetic fields. The peak values (from the mutual inductance measurements) associated with the ferrimagnetic transitions also increase with applied hydrostatic pressures. Moreover, the spin-flipped transitions are observed below transition temperature at ambient and applied pressure (12.67 kbar). The measurements above strongly suggested the ferrimagnetic spin configurations order earlier, i.e. transition temperatures increase with applied magnetic fields and pressures. In summary, the investigated frustrated spin systems (NaV2O4 and Cu2OSeO3) behave with the same trend with applied magnetic fields and hydrostatic pressures. It is possibly induced by the external DC magnetic field and the structure change and/or deformation under pressure.
author2 Hung-Duen Yang
author_facet Hung-Duen Yang
Kuo-feng Tseng
曾國峯
author Kuo-feng Tseng
曾國峯
spellingShingle Kuo-feng Tseng
曾國峯
Magnetic field and pressure effects on the spin frustrated systems NaV2O4 and Cu2OSeO3
author_sort Kuo-feng Tseng
title Magnetic field and pressure effects on the spin frustrated systems NaV2O4 and Cu2OSeO3
title_short Magnetic field and pressure effects on the spin frustrated systems NaV2O4 and Cu2OSeO3
title_full Magnetic field and pressure effects on the spin frustrated systems NaV2O4 and Cu2OSeO3
title_fullStr Magnetic field and pressure effects on the spin frustrated systems NaV2O4 and Cu2OSeO3
title_full_unstemmed Magnetic field and pressure effects on the spin frustrated systems NaV2O4 and Cu2OSeO3
title_sort magnetic field and pressure effects on the spin frustrated systems nav2o4 and cu2oseo3
publishDate 2010
url http://ndltd.ncl.edu.tw/handle/77310348245038349602
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