Laboratoire de Physique des Solides, Université Paris-Sud 11, UMR CNRS 8502, 91405 Orsay, France.
Phys Rev Lett. 2011 Dec 2;107(23):237201. doi: 10.1103/PhysRevLett.107.237201. Epub 2011 Nov 28.
We report (17)O NMR measurements in the S=1/2 (Cu(2+)) kagome antiferromagnet Herbertsmithite ZnCu(3)(OH)(6)Cl(2) down to 45 mK in magnetic fields ranging from 2 to 12 T. While Herbertsmithite displays a gapless spin-liquid behavior in zero field, we uncover an instability toward a spin-solid phase at sub-Kelvin temperature induced by an applied magnetic field. The latter phase shows largely suppressed moments ≲0.1 μ(B) and gapped excitations. The H-T phase diagram suggests the existence of a quantum critical point at the small but finite magnetic field μ(0)H(c)=1.55(25) T. We discuss this finding in light of the perturbative Dzyaloshinskii-Moriya interaction which was theoretically proposed to sustain a quantum critical regime for the quantum kagome Heisenberg antiferromagnet model.
我们报告了在磁场范围为 2 到 12 T 下,对 S=1/2(Cu(2+))) kagome 反铁磁体 Herbertsmithite ZnCu(3)(OH)(6)Cl(2) 在 45 mK 以下的 (17)O NMR 测量。虽然 Herbertsmithite 在零场下显示出无能隙自旋液体行为,但我们发现,在施加磁场的情况下,在亚开尔文温度下会出现向自旋固体相的不稳定性。后一相表现出大大抑制的磁矩≲0.1 μ(B) 和能隙激发。H-T 相图表明,在微小但有限的磁场 μ(0)H(c)=1.55(25) T 下存在量子临界点。我们根据理论上提出的微扰 Dzyaloshinskii-Moriya 相互作用来讨论这一发现,该相互作用被认为可以维持量子 kagome Heisenberg 反铁磁体模型的量子临界点。