Local spin dynamics in geometrically frustrated Mo pyrochlore antiferromagnet Lu$_2$Mo$_2$O$_{5-y}$N$_2$

S. K. Dey; K. Ishida; H. Okabe; M. Hiraishi; A. Koda; T. Honda; J. Yamaura; H. Kageyama; R. Kadono

doi:10.1103/PhysRevB.107.024407

paper

Local spin dynamics in geometrically frustrated Mo pyrochlore antiferromagnet Lu $_{2}$ Mo $_{2}$ O $_{5 - y}$ N $_{2}$

arXiv:2206.13049 · doi:10.1103/PhysRevB.107.024407

Abstract

The magnetic ground state of oxynitride pyrochlore Lu $_{2}$ Mo $_{2}$ O $_{5 - y}$ N $_{2}$ , a candidate compound for the quantum spin liquid ( $S = 1/2$ , Mo $^{5 +}$ ), was studied by muon spin rotation/relaxation experiment. In contrast to Lu $_{2}$ Mo $_{2}$ O $_{7}$ ( $S = 1$ , Mo $^{4 +}$ ) which exhibits the spin-glass behavior with a freezing temperature $T_{g} ≃ 16$ K, no such spin freezing or long range magnetic order was observed down to 0.3 K. Moreover, two separate magnetic domains were detected below $\sim$ 13 K, which were characterized by differences in spin dynamics. The first is the "sporadic" spin fluctuation seen in frustrated antiferromagnets, where the amplitude of the hyperfine fields suggests that the excitation comprises a local cluster of unpaired spins. The other is rapid paramagnetic fluctuation, which is only weakly suppressed at low temperatures. In place of the paramagnetic fluctuation, the volume fraction for the sporadic fluctuation steadily increases with decreasing temperature, indicating the formation of an excitation gap with a broad distribution of the gap energy involving null gap.

11 pages, 10 figures

Local spin dynamics in geometrically frustrated Mo pyrochlore antiferromagnet Lu2​Mo2​O5−y​N2​

Abstract

Local spin dynamics in geometrically frustrated Mo pyrochlore antiferromagnet Lu $_{2}$ Mo $_{2}$ O $_{5 - y}$ N $_{2}$