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Magic Fermions: Carroll and Flat Bands

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dc.contributor.author Banerjee, Aritra
dc.date.accessioned 2024-08-20T10:12:37Z
dc.date.available 2024-08-20T10:12:37Z
dc.date.issued 2023-03
dc.identifier.uri https://link.springer.com/article/10.1007/JHEP03(2023)227
dc.identifier.uri http://dspace.bits-pilani.ac.in:8080/jspui/xmlui/handle/123456789/15300
dc.description.abstract The Carroll algebra is constructed as the c → 0 limit of the Poincare algebra and is associated to symmetries on generic null surfaces. In this paper, we begin investigations of Carrollian fermions or fermions defined on generic null surfaces. Due to the availability of two different (degenerate) metrics on Carroll spacetimes, there is the possibility of two different versions of Carroll Clifford algebras. We consider both possibilities and construct explicit representations of Carrollian gamma matrices and show how to build higher spacetime dimensional representations out of lower ones. Actions for Carroll fermions are constructed with these gamma matrices and the properties of these actions are investigated. We show that in condensed matter systems where the dispersion relation becomes trivial i.e. the energy is not dependent on momentum and bands flatten out, Carroll symmetry generically appears. We give explicit examples of this including that of twisted bi-layer graphene, where superconductivity appears at so called magic angles and connect this to Carroll fermions. en_US
dc.language.iso en en_US
dc.publisher Springer en_US
dc.subject Physics en_US
dc.subject Poincare algebra en_US
dc.title Magic Fermions: Carroll and Flat Bands en_US
dc.type Article en_US


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