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Effect of disorder on the quantum spin liquid candidate Na$_4$Ir$_3$O$_8$ (1807.03940v1)

Published 11 Jul 2018 in cond-mat.str-el and cond-mat.mtrl-sci

Abstract: We report on the effects of introducing magnetic and non-magnetic disorder in the hyperkagome iridate quantum spin liquid (QSL) candidate Na$4$Ir$_3$O$_8$ by partially replacing Ir${4+}$ ($S = 1/2$) with Ru${4+}$ ($S = 1$) or Ti${4+}$ ($S = 0$). Specifically, we synthesized Na$_4$(Ir${1-x}$Ru$x$)$_3$O$_8 (x = 0.05, 0.10, 0.2, 0.3)$ and Na$_4$Ir${2.7}$Ti${0.3}$O$_8$ samples and measured electrical transport, AC and DC magnetization, and heat capacity down to $T = 1.8$ K. Na$_4$Ir$_3$O$_8$ is associated with a large Weiss temperature $\theta = -650$ K, a broad anomaly in magnetic heat capacity C${mag}$ at T $\approx25$ K, low temperature power-law heat capacity, and spin glass freezing below $T_f \approx 6$ K. We track the change in these characteristic features as Ir is partially substituted by Ru or Ti. We find that for Ru substitution, $\theta$ increases and stays negative, the anomaly in C${mag}$ is suppressed in magnitude and pushed to lower temperatures, low temperature $C \sim T\alpha$ with $\alpha$ between $2$ and $3$ and decreasing towards $2$ with increasing $x$, and $T_f$ increases with increase in Ru concentration $x$. For Ti substitution we find that $\theta$ and T$_f$ become smaller and the anomaly in $C{mag}$ is completely suppressed. In addition, introducing non-magnetic Ti leads to the creation of orphan spins which show up in the low temperature magnetic susceptibility.

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