New expressions for the Aharonov-Bohm phase and consequences for the fundamentals of quantum mechanics

dc.authorscopusid7004016669
dc.authorscopusid6602787345
dc.authorscopusid55893162300
dc.contributor.authorYarman, Nuh Tolga
dc.contributor.authorYarman, Tolga
dc.contributor.authorMissevitch, Oleg
dc.contributor.otherEnerji Sistemleri Mühendisliği / Energy Systems Engineering
dc.date.accessioned2024-05-25T11:27:55Z
dc.date.available2024-05-25T11:27:55Z
dc.date.issued2024
dc.departmentOkan Universityen_US
dc.department-temp[Kholmetskii, Alexander] Belarusian State Univ, Dept Phys, Minsk, BELARUS; [Yarman, Tolga] Istanbul Okan Univ, Istanbul, Turkiye; [Missevitch, Oleg] Belarusian State Univ, Inst Nucl Problems, Minsk, BELARUSen_US
dc.description.abstractWe focus on new expressions for the Aharonov-Bohm (AB) phase proposed recently by C. Marletto and V. Vedral (Phys. Rev. Lett. 125, 040401 (2020)) and by our team (A. L. Kholmetskii et al., Ann. Phys., 434, 168627 (2021)). We emphasize the mismatch between the standard expression for the electric component of the AB phase and the expression by Marletto and Vedral for this component, which, as we show, has fundamental roots and indicates the need to use different expressions for the Hamiltonian of the radiative component and bound component of the electromagnetic (EM) field. We further show that the corrected expression for the AB phase of Marletto and Vedral and our expression for the AB phase do not coincide with its standard representation through the potentials of EM field (Y. Aharonov, D. Bohm, Phys. Rev. 115 (1959) 485) and contain additional terms, which straightforwardly allow to re-express the AB phase via electric and magnetic fields instead of scalar and vector potentials. The recognition of the field-dependent origin of the AB effect also requires to re-express the Hamiltonian of a charged particle through the EM field, which we show can be done in the only possible way. We discuss the physical meaning of the AB effect with the primary role of the EM field and also discuss some general quantum mechanical implications.en_US
dc.identifier.citation0
dc.identifier.doi10.1515/zna-2023-0297
dc.identifier.endpage430en_US
dc.identifier.issn0932-0784
dc.identifier.issn1865-7109
dc.identifier.issue4en_US
dc.identifier.scopus2-s2.0-85182243262
dc.identifier.scopusqualityQ3
dc.identifier.startpage417en_US
dc.identifier.urihttps://doi.org/10.1515/zna-2023-0297
dc.identifier.urihttps://hdl.handle.net/20.500.14517/1113
dc.identifier.volume79en_US
dc.identifier.wosWOS:001143103400001
dc.identifier.wosqualityQ3
dc.language.isoen
dc.publisherWalter de Gruyter Gmbhen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectAharonov-Bohm effecten_US
dc.subjectHamiltonian of electromagnetic fielden_US
dc.subjectHamiltonian of electrically charged particleen_US
dc.subjectenergy-momentum operatoren_US
dc.titleNew expressions for the Aharonov-Bohm phase and consequences for the fundamentals of quantum mechanicsen_US
dc.typeArticleen_US
dspace.entity.typePublication
relation.isAuthorOfPublicatione8750528-f58f-486e-9a0a-eb4ab45fb468
relation.isAuthorOfPublication.latestForDiscoverye8750528-f58f-486e-9a0a-eb4ab45fb468
relation.isOrgUnitOfPublicatione2c8b290-2656-4ea1-8e8f-954383d6b397
relation.isOrgUnitOfPublication.latestForDiscoverye2c8b290-2656-4ea1-8e8f-954383d6b397

Files