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dc.contributor.authorZeybek, Z.
dc.contributor.authorUmucalilar, R. O.
dc.date.accessioned2025-01-09T20:14:35Z
dc.date.available2025-01-09T20:14:35Z
dc.date.issued2024
dc.identifier.issn0375-9601
dc.identifier.issn1873-2429
dc.identifier.urihttps://doi.org/10.1016/j.physleta.2024.129421
dc.identifier.urihttps://hdl.handle.net/20.500.14124/9157
dc.description.abstractWe study the nearly-degenerate quasihole manifold of the bosonic Hofstadter-Hubbard model on a torus, known to host the lattice analog of the Laughlin state at filling fraction ν = 1/2. Away from ν = 1/2 and in the presence of both localized and delocalized quasiholes, the ratio between the numerically calculated many-body Chern number for certain groups of states and the number of states in the relevant group turns out to be constant for this manifold, which is also manifested in the density profile as the depleted charge of localized quasiholes. Inspired by a zero-mode counting formula derivable from ageneralized Pauli principle, we employ a combinatorial scheme to account for the splittings in the manifold, allowing us to interpret some groups of states as the quasihole excitations corresponding to f illing fractions lower than ν = 1/2. In this scheme, the many-body Chern number of subgroups appears as a simple combinatorial factor.en_US
dc.language.isoengen_US
dc.publisherElsevieren_US
dc.relation.ispartofPhysics Letters Aen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.titleStructure of the nearly-degenerate manifold of lattice quasiholes on a torus (vol 445, 128259, 2022)en_US
dc.typecorrectionen_US
dc.departmentMimar Sinan Güzel Sanatlar Üniversitesien_US
dc.identifier.doi10.1016/j.physleta.2024.129421
dc.identifier.volume504en_US
dc.relation.publicationcategoryDiğeren_US
dc.identifier.wosqualityN/A
dc.identifier.wosWOS:001219179900001
dc.identifier.scopus2-s2.0-85188132222
dc.identifier.scopusqualityQ2
dc.indekslendigikaynakWeb of Scienceen_US
dc.indekslendigikaynakScopusen_US


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