TY - JOUR
T1 - Spin fluctuations in the spin-1/2 kagome lattice antiferromagnet (Rb1-xCsx)2Cu3SnF12 around the quantum critical point detected by muon spin relaxation technique
AU - Suzuki, Takao
AU - Katayama, Kazuya
AU - Kawasaki, Ikuto
AU - Watanabe, Isao
AU - Tanaka, Hidekazu
N1 - Funding Information:
Acknowledgments This work was partially supported by Grant-in-Aid for Scientific Research (A) No. 26247058 from Japan Society for the Promotion of Science.
Publisher Copyright:
© 2018 The Physical Society of Japan.
PY - 2018
Y1 - 2018
N2 - Zero- and longitudinal-field muon spin relaxation (ZF-, LF-μSR) measurements were carried out on the spin-1/2 kagome lattice antiferromagnet (Rb1-xCsx)2Cu3SnF12 with x = 0.53 and 0.6, where xc = 0.53 is the quantum critical point between the antiferromagnetically ordered phase and the valence-bond-glass phase. In the case of xc = 0.53, the muon spin relaxation rate at LF 200 gauss increases monotonically with decreasing temperature and shows no evidence for a magnetic order. The LF dependence of the muon spin relaxation rate, which corresponds to the fluctuating frequency spectrum, shows "white" spectrum behavior down to 0.3 K. These results indicate that internal magnetic fields fluctuate and are consistent with reported results of magnetic susceptibility measurement for xc = 0.53. In the case of x = 0.60, which is adjacent to the quantum critical point, the partial missing asymmetry in ZF-μSR time spectra is observed from a higher temperature than the antiferromagnetic phase transition temperature. It is suggested that large spin fluctuations peculiar to the quantum critical region appear.
AB - Zero- and longitudinal-field muon spin relaxation (ZF-, LF-μSR) measurements were carried out on the spin-1/2 kagome lattice antiferromagnet (Rb1-xCsx)2Cu3SnF12 with x = 0.53 and 0.6, where xc = 0.53 is the quantum critical point between the antiferromagnetically ordered phase and the valence-bond-glass phase. In the case of xc = 0.53, the muon spin relaxation rate at LF 200 gauss increases monotonically with decreasing temperature and shows no evidence for a magnetic order. The LF dependence of the muon spin relaxation rate, which corresponds to the fluctuating frequency spectrum, shows "white" spectrum behavior down to 0.3 K. These results indicate that internal magnetic fields fluctuate and are consistent with reported results of magnetic susceptibility measurement for xc = 0.53. In the case of x = 0.60, which is adjacent to the quantum critical point, the partial missing asymmetry in ZF-μSR time spectra is observed from a higher temperature than the antiferromagnetic phase transition temperature. It is suggested that large spin fluctuations peculiar to the quantum critical region appear.
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U2 - 10.7566/JPSJ.87.074708
DO - 10.7566/JPSJ.87.074708
M3 - Article
AN - SCOPUS:85049659635
SN - 0031-9015
VL - 87
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 7
M1 - 074708
ER -