Skip to content
DraconiticResearch
Search Sources API
190,839 studies31 sourcesUpdated 54 min ago
PreprintarXiv licencearXiv

Time-Reversal Symmetry in Artificial Topological Graphene Rings

Abstract

We study an artificial graphene ring described by the low-energy two-valley Dirac Hamiltonian with a uniform mass term. When the ring is threaded by an Aharonov-Bohm flux, the problem reduces to a second-order radial equation solved by Bessel functions. We give the exact secular equation and, for narrow rings, closed expressions for the spectrum and the persistent current. We then add a uniform magnetic field perpendicular to the plane. The radial problem is solved with confluent hypergeometric functions, and the persistent current and magnetization are written as derivatives of a secular determinant from which the spurious roots have been removed. Besides the usual orbital coupling, the field enters through a valley-dependent term that comes from the Dirac structure and lifts the valley degeneracy. A weak-field expansion, accurate up to corrections of order B^4, gives this valley splitting explicitly and separates the diamagnetic and paramagnetic contributions to the susceptibility. Finally, we work out what time reversal implies for the spectrum. Physical time reversal, which exchanges the valleys, leads to an exact relation between levels at opposite fields. The effective single-valley time reversal, on the other hand, is broken by the mass term and by the boundary conditions, yet leaves no trace in the zero-field spectrum. Numerical results for the spectrum, the persistent current, and the magnetization illustrate the analysis.

Related

  1. Phase-sensitive signatures of time-reversal-symmetry-breaking superconductivity in magic-angle twisted trilayer graphene
    Taehyeok Jin, Cheong-Eung Ahn, Seok Lee +6
    Nature CommunicationsPeer-reviewedCC BY-NC-ND 4.0Full textCondensed matterCrossref
  2. Time-reversal symmetry breaking and inherent Josephson diodes in a multi-component order parameter superconductor
    Remko Fermin, Matthijs Rog, Guido Stam +6
    Communications PhysicsPeer-reviewedCC BY-NC-ND 4.0Full textCondensed matterNatureCrossref
  3. Type-II quantum spin Hall insulator without time-reversal symmetry
    Panjun Feng, Chaoyang Tan, Xun-Wang Yan +5
    Science China Physics Mechanics and AstronomyPeer-reviewedLicence not statedFull text8 citedAtomic, molecular & optical physicsCondensed matterOpenAlex
  4. Valley-Helical Superconductivity Driven by Repulsion and Quantum Geometry: Applications to Time-Reversal Symmetric Rhombohedral Graphene
    Julian May-Mann, Trithep Devakul, Gal Shavit
    arXivPreprintCC BY 4.0Full textCondensed matterarXiv
  5. Fractionalization-Induced Time-Reversal Symmetry Breaking at Continuous Superconducting Transitions in Low-Symmetry Kondo Lattices
    Wonjune Choi, Shi-Zeng Lin
    arXivPreprintarXiv licenceFull textCondensed matterarXiv
BibTeX
@misc{neto2026timereversal,
  title = {{Time-Reversal Symmetry in Artificial Topological Graphene Rings}},
  author = {J. A. da Silva Neto and G. Q. Garcia and A. M. de M. Carvalho and C. Furtado},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.28055},
  eprint = {2610.28055},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.28055},
}
RIS
TY  - UNPB
TI  - Time-Reversal Symmetry in Artificial Topological Graphene Rings
AU  - J. A. da Silva Neto
AU  - G. Q. Garcia
AU  - A. M. de M. Carvalho
AU  - C. Furtado
PY  - 2026
DA  - 2026/10/20
PB  - arXiv
DO  - 10.48550/arxiv.2610.28055
UR  - https://arxiv.org/abs/2610.28055
AB  - We study an artificial graphene ring described by the low-energy two-valley Dirac Hamiltonian with a uniform mass term. When the ring is threaded by an Aharonov-Bohm flux, the problem reduces to a second-order radial equation solved by Bessel functions. We give the exact secular equation and, for narrow rings, closed expressions for the spectrum and the persistent current. We then add a uniform magnetic field perpendicular to the plane. The radial problem is solved with confluent hypergeometric functions, and the persistent current and magnetization are written as derivatives of a secular determinant from which the spurious roots have been removed. Besides the usual orbital coupling, the field enters through a valley-dependent term that comes from the Dirac structure and lifts the valley degeneracy. A weak-field expansion, accurate up to corrections of order B^4, gives this valley splitting explicitly and separates the diamagnetic and paramagnetic contributions to the susceptibility. Finally, we work out what time reversal implies for the spectrum. Physical time reversal, which exchanges the valleys, leads to an exact relation between levels at opposite fields. The effective single-valley time reversal, on the other hand, is broken by the mass term and by the boundary conditions, yet leaves no trace in the zero-field spectrum. Numerical results for the spectrum, the persistent current, and the magnetization illustrate the analysis.
ER  -