Large Magnetoresistance and Volume Expansion Associated with Valence Transition in Eu(Rh sub( 1-x)Ir sub( x)) sub( 2)Si sub( 2)

We report lattice parameters as a function of temperature, magnetization curves, and magnetoresistance of polycrystalline samples of ... The lattice parameters a and c for x = 0.3, 0.4, and 0.5 jump at around the valence transition temperature Tv. For these samples, the high-temperature (larger a, c...

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Veröffentlicht in:Journal of the Physical Society of Japan 2016-12, Vol.85 (12), p.1-1
Hauptverfasser: Mitsuda, Akihiro, Fujimoto, Takumi, Kishaba, Eigo, Hamano, Suguru, Kondo, Akihiro, Kindo, Koichi, Wada, Hirofumi
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container_issue 12
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container_title Journal of the Physical Society of Japan
container_volume 85
creator Mitsuda, Akihiro
Fujimoto, Takumi
Kishaba, Eigo
Hamano, Suguru
Kondo, Akihiro
Kindo, Koichi
Wada, Hirofumi
description We report lattice parameters as a function of temperature, magnetization curves, and magnetoresistance of polycrystalline samples of ... The lattice parameters a and c for x = 0.3, 0.4, and 0.5 jump at around the valence transition temperature Tv. For these samples, the high-temperature (larger a, c) and low-temperature (smaller a, c) phases, the volume fraction of which changes with temperature, coexist at around Tv, which means that the valence transition is of the first order. The magnetization curves of x = 0.3, 0.4, and 0.5 at T = 4.2 K exhibit a metamagnetic transition with a large hysteresis, implying a first-order field-induced valence transition. The transition field Bv is proportional to Tv, Bv = aTv with a = 0.36 T/K. For x = 0.3, a large negative magnetoresistance associated with the field-induced valence transition is observed. The origin of the negative magnetoresistance is discussed. (ProQuest: ... denotes formulae/symbols omitted.)
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The lattice parameters a and c for x = 0.3, 0.4, and 0.5 jump at around the valence transition temperature Tv. For these samples, the high-temperature (larger a, c) and low-temperature (smaller a, c) phases, the volume fraction of which changes with temperature, coexist at around Tv, which means that the valence transition is of the first order. The magnetization curves of x = 0.3, 0.4, and 0.5 at T = 4.2 K exhibit a metamagnetic transition with a large hysteresis, implying a first-order field-induced valence transition. The transition field Bv is proportional to Tv, Bv = aTv with a = 0.36 T/K. For x = 0.3, a large negative magnetoresistance associated with the field-induced valence transition is observed. The origin of the negative magnetoresistance is discussed. 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subjects Hysteresis
Lattice parameters
Magnetization curves
Magnetoresistance
Magnetoresistivity
Origins
Phases
Transition temperature
title Large Magnetoresistance and Volume Expansion Associated with Valence Transition in Eu(Rh sub( 1-x)Ir sub( x)) sub( 2)Si sub( 2)
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