Random singlet physics in the $S = \frac{1}{2}$ pyrochlore antiferromagnet NaCdCu$_2$F$_7$

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Hauptverfasser: Kancko, Andrej, Sakai, Hironori, Corrêa, Cinthia Antunes, Proschek, Petr, Prokleška, Jan, Haidamak, Tetiana, Uhlarz, Marc, Berlie, Adam, Tokunaga, Yo, Colman, Ross Harvey
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Veröffentlicht: 2025
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author Kancko, Andrej
Sakai, Hironori
Corrêa, Cinthia Antunes
Proschek, Petr
Prokleška, Jan
Haidamak, Tetiana
Uhlarz, Marc
Berlie, Adam
Tokunaga, Yo
Colman, Ross Harvey
author_facet Kancko, Andrej
Sakai, Hironori
Corrêa, Cinthia Antunes
Proschek, Petr
Prokleška, Jan
Haidamak, Tetiana
Uhlarz, Marc
Berlie, Adam
Tokunaga, Yo
Colman, Ross Harvey
contents We report a random singlet ground state in the $S=\frac{1}{2}$ Heisenberg pyrochlore antiferromagnet NaCdCu$_2$F$_7$. Cationic Na$^+$/Cd$^{2+}$ disorder on the pyrochlore $A$ site generates a broad distribution of Cu$^{2+}$--F$^-$--Cu$^{2+}$ exchange couplings, introducing intrinsic magnetic bond disorder. Despite strong antiferromagnetic interactions ($θ_{\mathrm{CW}}=-72$~K), no magnetic order or global spin freezing is observed in DC and AC susceptibility, specific heat or $^{23}$Na nuclear magnetic resonance to 120 mK, with muon spin relaxation experiments confirming persistent spin dynamics to 58 mK. $T$-linear specific heat, a Curie-like susceptibility tail, and power-law scaling with data collapse in $χ(T)$, $M(H)$, $C_{\mathrm{mag}}/T$, $^{23}$Na $(1/T_1T)$ and the muon spin polarization $P(t)$ reveal a disorder-driven network of random singlets and orphan spins. Scaling across multiple bulk and local probes is consistent with a broad distribution of exchange energies, $P[\mathcal{J}] \sim \mathcal{J}^{-α}$. This behavior contrasts with previously-studied Na$A''B_2$F$_7$ pyrochlore fluorides, where magnetic bond disorder precipitates spin-glass freezing, underscoring the crucial role of strong $S=\frac{1}{2}$ quantum fluctuations in NaCdCu$_2$F$_7$.
format Preprint
id arxiv_https___arxiv_org_abs_2509_20199
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Random singlet physics in the $S = \frac{1}{2}$ pyrochlore antiferromagnet NaCdCu$_2$F$_7$
Kancko, Andrej
Sakai, Hironori
Corrêa, Cinthia Antunes
Proschek, Petr
Prokleška, Jan
Haidamak, Tetiana
Uhlarz, Marc
Berlie, Adam
Tokunaga, Yo
Colman, Ross Harvey
Strongly Correlated Electrons
We report a random singlet ground state in the $S=\frac{1}{2}$ Heisenberg pyrochlore antiferromagnet NaCdCu$_2$F$_7$. Cationic Na$^+$/Cd$^{2+}$ disorder on the pyrochlore $A$ site generates a broad distribution of Cu$^{2+}$--F$^-$--Cu$^{2+}$ exchange couplings, introducing intrinsic magnetic bond disorder. Despite strong antiferromagnetic interactions ($θ_{\mathrm{CW}}=-72$~K), no magnetic order or global spin freezing is observed in DC and AC susceptibility, specific heat or $^{23}$Na nuclear magnetic resonance to 120 mK, with muon spin relaxation experiments confirming persistent spin dynamics to 58 mK. $T$-linear specific heat, a Curie-like susceptibility tail, and power-law scaling with data collapse in $χ(T)$, $M(H)$, $C_{\mathrm{mag}}/T$, $^{23}$Na $(1/T_1T)$ and the muon spin polarization $P(t)$ reveal a disorder-driven network of random singlets and orphan spins. Scaling across multiple bulk and local probes is consistent with a broad distribution of exchange energies, $P[\mathcal{J}] \sim \mathcal{J}^{-α}$. This behavior contrasts with previously-studied Na$A''B_2$F$_7$ pyrochlore fluorides, where magnetic bond disorder precipitates spin-glass freezing, underscoring the crucial role of strong $S=\frac{1}{2}$ quantum fluctuations in NaCdCu$_2$F$_7$.
title Random singlet physics in the $S = \frac{1}{2}$ pyrochlore antiferromagnet NaCdCu$_2$F$_7$
topic Strongly Correlated Electrons
url https://arxiv.org/abs/2509.20199