TY - JOUR
T1 - Yb 2(Pd 1-xNi x) 2Sn
T2 - Interplay of geometrical frustration and Kondo effect in quantum spin system
AU - Kikuchi, Fumitake
AU - Hara, Katsuya
AU - Matsuoka, Eiichi
AU - Onodera, Hideya
AU - Nakamura, Shintaro
AU - Nojima, Tsutomu
AU - Katoh, Kenichi
AU - Ochiai, Akira
N1 - Copyright:
Copyright 2012 Elsevier B.V., All rights reserved.
PY - 2009/8
Y1 - 2009/8
N2 - Single crystals of Yb 2(Pd 1-xNi x)2Sn with × = 0, 0.1, and 0.2 were prepared to clarify the effects of pressure on Yb 2Pd 2Sn which is considered to reside near the quantum critical point. The magnetization and specific heat measurements revealed that their ground states are regarded as an S = 1/2 XY-like spin system. Although nondoped Yb 2Pd 2Sn shows no magnetic transition down to 0.5 K owing to the Kondo effect, Ni-doped Yb 2Pd 2Sn exhibits a distinct magnetic transition. Furthermore, the magnetic susceptibility of Ni-doped Yb 2Pd 2Sn exhibits a broad peak in the temperature range higher than the magnetic transition temperature, which is not explained by the S = 1/2 Coqblin-Schrieffer model, suggesting the effect of geometrical frustration arising from the characteristic structure of these compounds, i.e., the Shastry-Sutherland lattice.
AB - Single crystals of Yb 2(Pd 1-xNi x)2Sn with × = 0, 0.1, and 0.2 were prepared to clarify the effects of pressure on Yb 2Pd 2Sn which is considered to reside near the quantum critical point. The magnetization and specific heat measurements revealed that their ground states are regarded as an S = 1/2 XY-like spin system. Although nondoped Yb 2Pd 2Sn shows no magnetic transition down to 0.5 K owing to the Kondo effect, Ni-doped Yb 2Pd 2Sn exhibits a distinct magnetic transition. Furthermore, the magnetic susceptibility of Ni-doped Yb 2Pd 2Sn exhibits a broad peak in the temperature range higher than the magnetic transition temperature, which is not explained by the S = 1/2 Coqblin-Schrieffer model, suggesting the effect of geometrical frustration arising from the characteristic structure of these compounds, i.e., the Shastry-Sutherland lattice.
KW - Quantum critical point
KW - Quantum spin system
KW - Shastry-Sutherland lattice
KW - Xy-type Spin
KW - Yb (Pd Ni ) Sn
KW - Yb Pd Sn
UR - http://www.scopus.com/inward/record.url?scp=69149105285&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=69149105285&partnerID=8YFLogxK
U2 - 10.1143/JPSJ.78.083708
DO - 10.1143/JPSJ.78.083708
M3 - Article
AN - SCOPUS:69149105285
SN - 0031-9015
VL - 78
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 8
M1 - 083708
ER -