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Solitons induced by an in-plane magnetic field in rhombohedral multilayer graphene

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Solitons induced by an in-plane magnetic field in rhombohedral multilayer graphene. / Tymczyszyn, Max; Cross, Peter; McCann, Edward.
In: Physical Review B: Condensed Matter and Materials Physics, Vol. 108, No. 11, 115425, 15.09.2023.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Tymczyszyn, M, Cross, P & McCann, E 2023, 'Solitons induced by an in-plane magnetic field in rhombohedral multilayer graphene', Physical Review B: Condensed Matter and Materials Physics, vol. 108, no. 11, 115425. https://doi.org/10.1103/PhysRevB.108.115425

APA

Tymczyszyn, M., Cross, P., & McCann, E. (2023). Solitons induced by an in-plane magnetic field in rhombohedral multilayer graphene. Physical Review B: Condensed Matter and Materials Physics, 108(11), Article 115425. https://doi.org/10.1103/PhysRevB.108.115425

Vancouver

Tymczyszyn M, Cross P, McCann E. Solitons induced by an in-plane magnetic field in rhombohedral multilayer graphene. Physical Review B: Condensed Matter and Materials Physics. 2023 Sept 15;108(11):115425. doi: 10.1103/PhysRevB.108.115425

Author

Tymczyszyn, Max ; Cross, Peter ; McCann, Edward. / Solitons induced by an in-plane magnetic field in rhombohedral multilayer graphene. In: Physical Review B: Condensed Matter and Materials Physics. 2023 ; Vol. 108, No. 11.

Bibtex

@article{3a85aea8b9ae4db0b553d0fcbb5dc25b,
title = "Solitons induced by an in-plane magnetic field in rhombohedral multilayer graphene",
abstract = "We model the influence of an in-plane magnetic field on the orbital motion of electrons in rhombohedral graphene multilayers. For zero field, the low-energy band structure includes a pair of flat bands near zero energy, which are localized on the surface layers of a finite thin film. For finite field, we find that the zero-energy bands persist and that level bifurcations occur at energies determined by the component of the in-plane wave vector q that is parallel to the external field. The occurrence of level bifurcations is explained by invoking semiclassical quantization of the zero-field Fermi surface of rhombohedral graphite. We find parameter regions with a single isoenergetic contour of Berry phase zero corresponding to a conventional Landau level spectrum and regions with two isoenergetic contours, each of Berry phase π, corresponding to a Dirac-like spectrum of levels. We write down an analogous one-dimensional tight-binding model and relate the persistence of the zero-energy bands in large magnetic fields to a soliton texture supporting zero-energy states in the Su-Schrieffer-Heeger model. We show that different states contributing to the zero-energy flat bands in rhombohedral graphene multilayers in a large field, as determined by the wave vector q, are localized on different bulk layers of the system, not just the surfaces.",
author = "Max Tymczyszyn and Peter Cross and Edward McCann",
year = "2023",
month = sep,
day = "15",
doi = "10.1103/PhysRevB.108.115425",
language = "English",
volume = "108",
journal = "Physical Review B: Condensed Matter and Materials Physics",
issn = "1098-0121",
publisher = "AMER PHYSICAL SOC",
number = "11",

}

RIS

TY - JOUR

T1 - Solitons induced by an in-plane magnetic field in rhombohedral multilayer graphene

AU - Tymczyszyn, Max

AU - Cross, Peter

AU - McCann, Edward

PY - 2023/9/15

Y1 - 2023/9/15

N2 - We model the influence of an in-plane magnetic field on the orbital motion of electrons in rhombohedral graphene multilayers. For zero field, the low-energy band structure includes a pair of flat bands near zero energy, which are localized on the surface layers of a finite thin film. For finite field, we find that the zero-energy bands persist and that level bifurcations occur at energies determined by the component of the in-plane wave vector q that is parallel to the external field. The occurrence of level bifurcations is explained by invoking semiclassical quantization of the zero-field Fermi surface of rhombohedral graphite. We find parameter regions with a single isoenergetic contour of Berry phase zero corresponding to a conventional Landau level spectrum and regions with two isoenergetic contours, each of Berry phase π, corresponding to a Dirac-like spectrum of levels. We write down an analogous one-dimensional tight-binding model and relate the persistence of the zero-energy bands in large magnetic fields to a soliton texture supporting zero-energy states in the Su-Schrieffer-Heeger model. We show that different states contributing to the zero-energy flat bands in rhombohedral graphene multilayers in a large field, as determined by the wave vector q, are localized on different bulk layers of the system, not just the surfaces.

AB - We model the influence of an in-plane magnetic field on the orbital motion of electrons in rhombohedral graphene multilayers. For zero field, the low-energy band structure includes a pair of flat bands near zero energy, which are localized on the surface layers of a finite thin film. For finite field, we find that the zero-energy bands persist and that level bifurcations occur at energies determined by the component of the in-plane wave vector q that is parallel to the external field. The occurrence of level bifurcations is explained by invoking semiclassical quantization of the zero-field Fermi surface of rhombohedral graphite. We find parameter regions with a single isoenergetic contour of Berry phase zero corresponding to a conventional Landau level spectrum and regions with two isoenergetic contours, each of Berry phase π, corresponding to a Dirac-like spectrum of levels. We write down an analogous one-dimensional tight-binding model and relate the persistence of the zero-energy bands in large magnetic fields to a soliton texture supporting zero-energy states in the Su-Schrieffer-Heeger model. We show that different states contributing to the zero-energy flat bands in rhombohedral graphene multilayers in a large field, as determined by the wave vector q, are localized on different bulk layers of the system, not just the surfaces.

U2 - 10.1103/PhysRevB.108.115425

DO - 10.1103/PhysRevB.108.115425

M3 - Journal article

VL - 108

JO - Physical Review B: Condensed Matter and Materials Physics

JF - Physical Review B: Condensed Matter and Materials Physics

SN - 1098-0121

IS - 11

M1 - 115425

ER -