Topological charge Fano effect in multi-Weyl semimetals

W. C. Silva, W. N. Mizobata, J. E. Sanches, L. S. Ricco, I. A. Shelykh, M. De Souza, M. S. Figueira, E. Vernek, A. C. Seridonio*

*Corresponding author for this work

Research output: Contribution to journalArticlepeer-review

Abstract

We theoretically analyze the Fano interference in a single impurity multi-Weyl semimetal hybrid system and show the emergence of the topological charge Fano effect in the bulk local density of states. In multi-Weyl semimetals, the number of Fermi arcs at the system boundaries is determined by the topological charge J, a direct consequence of the "bulk-boundary"correspondence principle. Analogously, we find that J also modulates the bulk Fano profile of the system with an embedded quantum impurity. Thus by increasing J, the Fano line shape evolves from resonant, typical for J=1 (single Weyl), towards antiresonant, extrapolating to the so-called hyper Weyl semimetals with J≫1. Specially for the maximum case protected by the rotational symmetry C2J=6, namely, the J=3 (triple Weyl), which acquires asymmetric Fano profile, the Fano parameter absolute value is predicted to be tan(C2J=6), where C2J(360∘/2J) defines the rotational angle. Hence, the Fano discretization in the J term introduces the topological charge Fano effect in multi-Weyl semimetals. We also suggest a transport device where we expect that the proposed Fano effect could be detected.

Original languageEnglish
Article number235135
JournalPhysical Review B
Volume105
Issue number23
DOIs
Publication statusPublished - 15 Jun 2022

Bibliographical note

Funding Information:
We thank the Brazilian funding agencies CNPq (Grants No. 302887/2020-2, No. 308410/2018-1, No. 311980/2021-0, No. 305738/2018-6, No. 311366/2021-0, No. 305668/2018-8, and No. 308695/2021-6), Coordenação de Aperfeiçoamento de Pessoal de Nível Superior–Brasil (CAPES) – Finance Code 001, the São Paulo Research Foundation (FAPESP; Grant No. 2018/09413-0) and FAPERJ Process No. 210 355/2018. L.S.R. and I.A.S. acknowledge support from the Icelandic Research Fund (project “Hybrid polaritonics”). I.A.S. also acknowledges support from the Program Priority 2030. L.S.R. thanks A.C.S. and Unesp for their hospitality.

Publisher Copyright:
© 2022 American Physical Society.

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