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arxiv: 1808.02614 · v2 · pith:X2IJIMZBnew · submitted 2018-08-08 · ❄️ cond-mat.str-el · cond-mat.mtrl-sci

Valence-Bond-Glass State with Singlet Gap in the Spin-1/2 Square-Lattice Random J₁-J₂ Heisenberg Antiferromagnet Sr₂CuTe_(1-x)W_xO₆

classification ❄️ cond-mat.str-el cond-mat.mtrl-sci
keywords cutelow-temperaturemagneticsingletstatecomponentfieldheat
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The double-perovskite compounds Sr$_2$CuTeO$_6$ and Sr$_2$CuWO$_6$ are magnetically described as quasi-two-dimensional spin-1/2 square-lattice $J_1{-}J_2$ Heisenberg antiferromagnets with predominant $J_1$ and $J_2$ exchange interactions, respectively. We report the low-temperature magnetic properties of Sr$_2$CuTe$_{1-x}$W$_x$O$_6$ with randomness in the magnitudes of $J_1$ and $J_2$. It was found that the low-temperature specific heat for $0.1\leq x \leq 0.5$ has a large component proportional to the temperature $T$ above 1.2 K, although the low-temperature specific heat for the two parent systems is approximately proportional to $T^3$. With decreasing temperature below 1.2 K, the $T$-linear component decreases rapidly toward zero, which is insensitive to the magnetic field up to 9 T. This is suggestive of the singlet excitation decoupled from the magnetic field. The NMR spectrum for $x=0.2$ exhibits no long-range order down to 1.8 K. These results indicates that the ground state of Sr$_2$CuTe$_{1-x}$W$_x$O$_6$ is a valence-bond-glass state with singlet gaps.

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