TY - JOUR
T1 - Unique pressure versus temperature phase diagram for antiferromagnets Eu2Ni3Ge5 and EuRhSi3
AU - Nakashima, Miho
AU - Amako, Yasushi
AU - Matsubayashi, Kazuyuki
AU - Uwatoko, Yoshiya
AU - Nada, Masato
AU - Sugiyama, Kiyohiro
AU - Hagiwara, Masayuki
AU - Haga, Yoshinori
AU - Takeuchi, Tetsuya
AU - Nakamura, Ai
AU - Akamine, Hiromu
AU - Tomori, Keisuke
AU - Yara, Tomoyuki
AU - Ashitomi, Yosuke
AU - Hedo, Masato
AU - Nakama, Takao
AU - Ōnuki, Yoshichika
N1 - Funding Information:
We are very grateful to helpful discussions with Professors H. Shiba, T. Hotta, and K. Miyake. This work was supported by JSPS KAKENHI Grant Numbers JP16H01078 and JP16H04006.
Publisher Copyright:
©2017 The Physical Society of Japan.
PY - 2017
Y1 - 2017
N2 - We studied the magnetic properties of the antiferromagnets Eu2Ni3Ge5 and EuRhSi3 by measuring their electrical resistivity, specific heat, magnetic susceptibility, magnetization, and thermoelectric power, together with the electrical resistivities at high pressures of up to 15 GPa. These compounds have almost divalent Eu ions at ambient pressure and order antiferromagnetically with a successive change in the antiferromagnetic structure at TN = 19 K and TN′ = 17 K in Eu2Ni3Ge5, and at TN = 49 K and TN = 45 K in EuRhSi3. Magnetic field versus temperature (H-T) phase diagrams were constructed for both compounds from the magnetization measurements. The Néel temperature in Eu2Ni3Ge5 was found to increase up to 7 GPa but to decrease continuously with further increasing pressure, without the so-called valence transition. Under a high pressure of 15 GPa, Kondo-like behavior of the electrical resistivity was observed, suggesting the existence of the heavy-fermion state at low temperatures. A similar trend is likely to occur in EuRhSi3. The present P-T phase diagrams for both compounds are the first cases that are reminiscent of the phase diagram of EuCu2(SixGe1-x)2.
AB - We studied the magnetic properties of the antiferromagnets Eu2Ni3Ge5 and EuRhSi3 by measuring their electrical resistivity, specific heat, magnetic susceptibility, magnetization, and thermoelectric power, together with the electrical resistivities at high pressures of up to 15 GPa. These compounds have almost divalent Eu ions at ambient pressure and order antiferromagnetically with a successive change in the antiferromagnetic structure at TN = 19 K and TN′ = 17 K in Eu2Ni3Ge5, and at TN = 49 K and TN = 45 K in EuRhSi3. Magnetic field versus temperature (H-T) phase diagrams were constructed for both compounds from the magnetization measurements. The Néel temperature in Eu2Ni3Ge5 was found to increase up to 7 GPa but to decrease continuously with further increasing pressure, without the so-called valence transition. Under a high pressure of 15 GPa, Kondo-like behavior of the electrical resistivity was observed, suggesting the existence of the heavy-fermion state at low temperatures. A similar trend is likely to occur in EuRhSi3. The present P-T phase diagrams for both compounds are the first cases that are reminiscent of the phase diagram of EuCu2(SixGe1-x)2.
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U2 - 10.7566/JPSJ.86.034708
DO - 10.7566/JPSJ.86.034708
M3 - Article
AN - SCOPUS:85014661488
SN - 0031-9015
VL - 86
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 3
M1 - 034708
ER -