Microscopic mechanism of the zero in-plane-field resistance peak

Determine the microscopic mechanism by which an in-plane magnetic field near zero produces excess longitudinal resistance across existing magnetic domain walls in the valley-polarized quarter-metal state of twisted double bilayer graphene.

Background

The paper establishes that the anomalous zero-in-plane-field resistance peak is associated with metastable magnetic domains in the valley-polarized quarter-metal state of twisted double bilayer graphene. Because spin and valley polarization are coupled by spin-orbit interaction, the authors argue that adjacent domains may also possess oppositely oriented spin polarizations.

The authors discuss current-driven precession of spin textures at domain walls as a speculative explanation. At zero in-plane field, weakly pinned in-plane domain-wall moments could precess under spin-transfer torque, whereas a finite in-plane field could pin those moments and suppress the resulting excess resistance. However, the available data do not identify this microscopic transport mechanism unambiguously.

References

These observations raise two distinct questions. For a given domain configuration, what is the mechanism by which $B_\parallel$ near zero produces excess resistance?

Metastable magnetic domains and the anomalous $B_\parallel=0$ resistance peak in twisted double bilayer graphene  (2608.25263 - Gao et al., 26 Aug 2026) in Section Discussion, subsection “Mechanism of the $B_\parallel$ peak”

A complete microscopic theory connecting these observations remains an open challenge.

Metastable magnetic domains and the anomalous $B_\parallel=0$ resistance peak in twisted double bilayer graphene  (2608.25263 - Gao et al., 26 Aug 2026) in Section Discussion, final paragraph