Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/10162
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dc.contributor.authorSaha, Madhumitaen_US
dc.contributor.authorAGARWALLA, BIJAY KUMARen_US
dc.contributor.authorKulkarni, Manasen_US
dc.contributor.authorPurkayastha, Archaken_US
dc.date.accessioned2025-06-12T06:04:23Z-
dc.date.available2025-06-12T06:04:23Z-
dc.date.issued2025-03en_US
dc.identifier.citationPhysical Review B, 111, (12).en_US
dc.identifier.issn2469-9969en_US
dc.identifier.issn2469-9950en_US
dc.identifier.urihttps://doi.org/10.1103/PhysRevB.111.125412en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/10162-
dc.description.abstractRecently, it has been shown that, in one-dimensional fermionic systems, close to band edges, the zero temperature conductance scales as 1/𝑁2, where 𝑁 is the system length. This universal subdiffusive scaling of conductance at band edges has been tied to an exceptional point (EP) of the transfer matrix of the system that occurs at every band edge. Further, in the presence of bulk dephasing probes, this EP has been shown to lead to a counterintuitive superballistic scaling of conductance, where the conductance increases with 𝑁 over a finite but large regime of system lengths. In this work, we explore how these behaviors are affected by the order of the transfer matrix EP at the band edge. We consider a one-dimensional fermionic lattice chain with a finite range of hopping. Depending on the range of hopping and the hopping parameters, this system can feature band edges which correspond to arbitrarily higher order EPs of the associated transfer matrix. Using this system we establish in generality that, in the absence of bulk dephasing, surprisingly, the universal 1/𝑁2 scaling of conductance is completely unaffected by the order of the EP. This is despite the fact that existence of transfer matrix EP is crucial for such behavior. In the presence of bulk dephasing, however, the phase coherence length, the extent of the superballisitic scaling regime, and the exponent of superballistic scaling all encode the order of the transfer matrix EP.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectExceptional pointsen_US
dc.subjectTight-binding modelen_US
dc.subjectTransfer matrix calculationsen_US
dc.subject2025en_US
dc.titleEffect of order of transfer matrix exceptional points on transport at band edgesen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Ben_US
dc.publication.originofpublisherForeignen_US
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