Nuclear magnetic resonance measurement station in SECUF using hybrid superconducting magnets*

Project supported by the Strategic Priority Research Program of the Chinese Academy of Sciences (Grant No. XDB07020200), the National Key Research and Development Program of China (Grant Nos. 2016YFA0300502 and 2015CB921304), and the National Natural Science Foundation of China (Grant No. 11634015).

Li Zheng1, 2, †, Zheng Guo-qing1, 2, ‡
       

(color online) (a) Top view of the Cu3Zn(OH)6FBr crystal structure, where F (brown) is in the center between two hexagons of two kagome Cu planes. (b) Magnetic field dependence of the spin gap. The black short-dash line is fitted by Δ(B) = Δ(0) − BSB with spin quantum number S = 1/2, where g-factor obtained from bulk magnetic susceptibility is g = 2.4 and μB is the Bohr magneton. For comparison, Δ(B) for S = 1 is shown by the blue dash line constrained by the value at 0.914 T, which hardly describes the data. Inset shows the Arrhenius plot of 19 KKchem with the vertical axis in logarithmic scale, which demonstrates visually that the gap decreases with increasing magnetic field. The solid curve is the fitting function A exp(−Δ/T) for 19 KKchem.[7]