RQMP (CPM) Seminar

Heat conduction in herbertsmithite: field dependence at the onset of the quantum spin liquid regime

Quentin Barthélémy

Université de Sherbrooke

Herbertsmithite ZnCu₃(OH)₆Cl₂ is an emblematic quantum spin liquid candidate because it is the closest realization of the nearest-neighbor S = 1/2 kagome Heisenberg antiferromagnet with a dynamical ground state. After recalling some selected developments of our 17O NMR and high-field specific studies [1, 2], I will present our recent thermal transport study [3], where we report thermal conductivity measurements on high quality single crystals over a wide range of temperatures (0.05-120 K) in magnetic fields up to 15 T. We also report measurements of the thermal Hall effect, found to be vanishingly small. At high temperatures, in the paramagnetic regime, the thermal conductivity has a negligible field dependence. Upon cooling and the development of correlations, the onset of a clear monotonic field dependence below about 20 K signals a new characteristic temperature scale that may reflect the subtle crossover towards the quantum spin liquid regime. Deconfined spinons, if present, are not detected and phonons, as the main carriers of heat, are strongly scattered by the intrinsic spin excitations and the magnetic defects. In view of the colossal fields required to affect the intrinsic spins, most of the field-induced evolution is attributed to the progressive polarization of some magnetic defects. By elaborating a phenomenological model, we extract the magnetization of these main scattering centers which does not resemble the Brillouin function for free spins 1/2, requiring to go beyond the paradigm of isolated paramagnetic spins. Besides, the onset of a nonmonotonic field dependence below about 2 K underlines the existence of another characteristic temperature scale, previously highlighted with other measurements, and sheds new light on the phase diagram of herbertsmithite down to the lowest temperatures.

[1] P. Khuntia et al., Nature Physics 16, 469 (2020)
[2] Q. Barthélemy et al., Physical Review X 12, 011014 (2022)
[3] Q. Barthélemy et al., arXiv:2211.08546 (2022)