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Peer-reviewedCC BY 4.0SciPost Physics

Phonon thermal Hall effect in quartz and its absence in silica

Abstract

The observation of a misalignment between the applied heat flux and the measured temperature gradient in insulating solids induced by magnetic field has become a subject of experimental investigation, theoretical speculation, and unsettled controversy. To identify the origin of this phonon thermal Hall effect, we performed a comparative study of longitudinal and transverse heat transport in crystalline (quartz) and vitreous (silica) SiO 2 using identical experimental set-ups and thermometers. A finite signal was detected in the crystalline samples and none in the amorphous sample, within our resolution. The cleaner crystal exhibited a larger thermal Hall conductivity than the dirtier one, ruling out disorder as the driver of the effect. On the other hand, the amplitude of the transverse thermal resistivity is almost identical in the two crystalline samples (W ⊥ /B≈ 10 -6 m.K.W -1 .T -1 ). We show that in a phonon gas, as in a molecular gas displaying the Senftleben-Beenakker effect, heat is conducted through two channels, and argue that a thermal Hall response is unavoidable whenever these channels differ both in entropy production and in their coupling to the magnetic field. Under such conditions, the conserved energy current and the non-conserved entropy current cease to be parallel. Finally, the magnitude of the transverse thermal resistivity can be accounted for by a surprisingly simple picture. The heat flux induces a tiny drift velocity of the lattice nuclei, the magnetic field exerts a transverse Berry force on this drift, and this force is balanced by an entropic restoring force.

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BibTeX
@article{ling2026phonon,
  title = {{Phonon thermal Hall effect in quartz and its absence in silica}},
  author = {Yu Ling and Benoît Fauqué and Kamran Behnia},
  journal = {SciPost Physics},
  year = {2026},
  month = aug,
  doi = {10.21468/scipostphys.21.2.036},
  url = {https://hal.science/hal-05794350v1},
  note = {CC BY 4.0},
}
RIS
TY  - JOUR
TI  - Phonon thermal Hall effect in quartz and its absence in silica
AU  - Yu Ling
AU  - Benoît Fauqué
AU  - Kamran Behnia
PY  - 2026
DA  - 2026/08/10
JO  - SciPost Physics
DO  - 10.21468/scipostphys.21.2.036
UR  - https://hal.science/hal-05794350v1
AB  - The observation of a misalignment between the applied heat flux and the measured temperature gradient in insulating solids induced by magnetic field has become a subject of experimental investigation, theoretical speculation, and unsettled controversy. To identify the origin of this phonon thermal Hall effect, we performed a comparative study of longitudinal and transverse heat transport in crystalline (quartz) and vitreous (silica) SiO 2 using identical experimental set-ups and thermometers. A finite signal was detected in the crystalline samples and none in the amorphous sample, within our resolution. The cleaner crystal exhibited a larger thermal Hall conductivity than the dirtier one, ruling out disorder as the driver of the effect. On the other hand, the amplitude of the transverse thermal resistivity is almost identical in the two crystalline samples (W ⊥ /B≈ 10 -6 m.K.W -1 .T -1 ). We show that in a phonon gas, as in a molecular gas displaying the Senftleben-Beenakker effect, heat is conducted through two channels, and argue that a thermal Hall response is unavoidable whenever these channels differ both in entropy production and in their coupling to the magnetic field. Under such conditions, the conserved energy current and the non-conserved entropy current cease to be parallel. Finally, the magnitude of the transverse thermal resistivity can be accounted for by a surprisingly simple picture. The heat flux induces a tiny drift velocity of the lattice nuclei, the magnetic field exerts a transverse Berry force on this drift, and this force is balanced by an entropic restoring force.
SN  - 2542-4653
ER  -