T. Goto

activity

20012004

most citedMagnetization plateaux of S = 1/2 two-dimensional frustrated antiferromagnet Cs

_{2}

CuBr

_{4}

66 citations · 91 across the 3 of their papers we have counts for

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cond-mat.str-el2004★ 66 cited

Magnetization plateaux of S = 1/2 two-dimensional frustrated antiferromagnet Cs $_{2}$ CuBr $_{4}$

T. Ono, H. Tanaka, O. Kolomiyets +9

The field induced magnetic phase transitions of Cs $_{2}$ CuBr $_{4}$ were investigated by means of magnetization process and neutron scattering experiments. This system undergoes magneti…

cond-mat.str-el2002★ 2 cited

High-field magnetization of the 3d heavy-fermion system LiV $_{2}$ O $_{4 - d}$ (d = 0, 0.08)

N. Tsujii, K. Yoshimura, K. Kosuge +2

Metamagnetic behavior has been observed in LiV2O4 powder sample around 38 T at 4.2 K. On the other hand, magnetization for oxygen deficient LiV2O3.92 shows no indication of metamag…

cond-mat.str-el2001★ 23 cited

Field-Induced Two-Step Phase Transitions in the Singlet Ground State Triangular Antiferromagnet CsFeBr $_{3}$

Y. Tanaka, H. Tanaka, T. Ono +7

The ground state of the stacked triangular antiferromagnet CsFeBr $_{3}$ is a spin singlet due to the large single ion anisotropy $D (S^{z})^{2}$ . The field-induced magnetic ordering in th…

Magnetization plateaux of S = 1/2 two-dimensional frustrated antiferromagnet Cs2​CuBr4​

High-field magnetization of the 3d heavy-fermion system LiV2​O4−d​ (d = 0, 0.08)

Field-Induced Two-Step Phase Transitions in the Singlet Ground State Triangular Antiferromagnet CsFeBr3​

Magnetization plateaux of S = 1/2 two-dimensional frustrated antiferromagnet Cs $_{2}$ CuBr $_{4}$

High-field magnetization of the 3d heavy-fermion system LiV $_{2}$ O $_{4 - d}$ (d = 0, 0.08)

Field-Induced Two-Step Phase Transitions in the Singlet Ground State Triangular Antiferromagnet CsFeBr $_{3}$