Abstract

We present data on the magnetic properties of two classes of layered spin S=1/2 antiferromagnetic quasi-triangular lattice materials: Cu2(1−x)Zn2x(OH)3NO3Cu_{2(1-x)}Zn_{2x}(OH)_3NO_3 (0<x<0.650 < x < 0.65) and its long chain organic derivatives Cu2(1−x)Zn2x(OH)3(C7H15COO)⋅mH2OCu_{2(1-x)}Zn_{2x}(OH)_3(C_7H_{15}COO)\cdot mH_2O (0<x<0.290 < x < 0.29), where non-magnetic Zn substitutes Cu isostructurally. It is found that the long-chain compounds, even in a clean system in the absence of dilution, x ⁣= ⁣0x\!=\!0, show spin-glass behavior, as evidenced by DC and AC susceptibility, and by time dependent magnetization measurements. A striking feature is the observation of a sharp crossover between two successive power law regimes in the DC susceptibility above the freezing temperature. Specific heat data are consistent with a conventional phase transition in the unintercalated compounds, and glassy behavior in the long chain compunds.

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