2012
DOI: 10.1143/jpsj.81.023709
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Pressure-Induced Valence Transition in Antiferromagnet EuRh2Si2

Abstract: Considering the unique properties of EuRh 2 Si 2 from the viewpoint of the Eu valence, we have examined its physical properties under external pressure. At ambient pressure, EuRh 2 Si 2 is an antiferromagnet with a Néel temperature T N of 25 K, and the Eu ion is in the divalent state. The application of pressure up to 0.84 GPa slightly shifts T N toward higher values. Under pressures higher than 1.00 GPa, an abrupt first-order valence transition emerges simultaneously with the disappearance of antiferromagneti… Show more

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Cited by 83 publications
(45 citation statements)
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References 22 publications
(18 reference statements)
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“…Interestingly the valence of some Eu compounds is changed by temperature, magnetic field and pressure. For example, the Eu-divalent electronic state in EuRh 2 Si 2 is changed into a nearly trivalent one under pressure, where a critical pressure is P c 1 GPa [1]. In the case of EuNi 2 P 2 , a nearly Eu-divalent electronic state at room temperature is changed into a heavy fermion state at low temperatures via the Kondo effect, where an electronic specific heat coefficient is γ = 100 mJ/(K 2 ·mol) and the Kondo temperature is T K = 80 K [2].…”
Section: Introductionmentioning
confidence: 99%
“…Interestingly the valence of some Eu compounds is changed by temperature, magnetic field and pressure. For example, the Eu-divalent electronic state in EuRh 2 Si 2 is changed into a nearly trivalent one under pressure, where a critical pressure is P c 1 GPa [1]. In the case of EuNi 2 P 2 , a nearly Eu-divalent electronic state at room temperature is changed into a heavy fermion state at low temperatures via the Kondo effect, where an electronic specific heat coefficient is γ = 100 mJ/(K 2 ·mol) and the Kondo temperature is T K = 80 K [2].…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, valence instability often occurs in Eu compounds, from a divalent electronic state of Eu 2þ (4f 7 : S ¼ 7=2, L ¼ 0, and J ¼ 7=2) at high temperatures to a nearly trivalent electronic state (4f 6 in Eu 3þ : S ¼ L ¼ 3, and J ¼ 0) at low temperatures, depending on the magnetic field and pressure. [4][5][6] Here, S, L, and J are the spin, orbital, and total angular momenta, respectively. EuBi 3 is a divalent compound and orders antiferromagnetically below a Néel temperature T N ' 7:5 K, which was identified by electrical resistivity, magnetic susceptibility, and specific heat experiments.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, the trivalent Eu state is non-magnetic (J = 0, S = L = 3). For example, the recent experimental result of EuRh 2 Si 2 with the tetragonal structure is typical [1]. The electronic state of EuRh 2 Si 2 is divalent at ambient pressure, and orders antiferromagnetically below a Néel temperature T N = 23 K. The application of pressure up to 0.84 GPa slightly shifts T N toward higher values.…”
Section: Introductionmentioning
confidence: 96%