X. Rao

activity

20172021

most citedSurvival of itinerant excitations and quantum spin state transitions in YbMgGaO

_{4}

with chemical disorder

58 citations · 89 across the 6 of their papers we have counts for

collaborators

Showing 2019Show all

3 papers · 1 filter

cond-mat.mtrl-sci2019★ 4 cited

Quantum oscillation of thermal conductivity and violation of Weidemann-Franz law in TaAs $_{2}$ and NbAs $_{2}$

X. Rao, X. Zhao, X. -Y. Wang +5

We report a study of thermal conductivity and resistivity at ultra-low temperatures and in high magnetic fields for semi-metal materials TaAs $_{2}$ and NbAs $_{2}$ by using single cryst…

cond-mat.str-el2019★ 6 cited

Low-temperature thermal conductivity and magnetic transitions of the kagomé-staircase compound Ni $_{3}$ V $_{2}$ O $_{8}$

Z. Y. Zhao, Q. J. Li, X. G. Liu +6

Kagomé-staircase compound Ni $_{3}$ V $_{2}$ O $_{8}$ is an attractive multiferroic material exhibiting rich phase diagrams. However, the magnetic properties and magnetic transitions have bee…

cond-mat.mtrl-sci2019★ 6 cited

Magnetism study on a frustration-free spatially anisotropic $S$ = 1 square lattice antiferromagnet Ni[SC(NH $_{2}$ ) $_{2}$ ] $_{6}$ Br $_{2}$

X. Zhao, Z. Y. Zhao, L. M. Chen +7

Magnetism of the $S$ = 1 Heisenberg antiferromagnets on the spatially anisotropic square lattice has been scarcely explored. Here we report a study of the magnetism, specific heat,…

Quantum oscillation of thermal conductivity and violation of Weidemann-Franz law in TaAs2​ and NbAs2​

Low-temperature thermal conductivity and magnetic transitions of the kagomé-staircase compound Ni3​V2​O8​

Magnetism study on a frustration-free spatially anisotropic S = 1 square lattice antiferromagnet Ni[SC(NH2​)2​]6​Br2​

Quantum oscillation of thermal conductivity and violation of Weidemann-Franz law in TaAs $_{2}$ and NbAs $_{2}$

Low-temperature thermal conductivity and magnetic transitions of the kagomé-staircase compound Ni $_{3}$ V $_{2}$ O $_{8}$

Magnetism study on a frustration-free spatially anisotropic $S$ = 1 square lattice antiferromagnet Ni[SC(NH $_{2}$ ) $_{2}$ ] $_{6}$ Br $_{2}$