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dc.contributor.authorLin, MFen_US
dc.contributor.authorChuu, DSen_US
dc.date.accessioned2019-04-03T06:35:45Z-
dc.date.available2019-04-03T06:35:45Z-
dc.date.issued1998-03-15en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.57.6731en_US
dc.identifier.urihttp://hdl.handle.net/11536/32726-
dc.description.abstractThe geometric structure of the toroidal carbon nanotubes (TCN's) determines the electronic structure and thus the characteristics of the persistent current. Such current is caused by the magnetic flux phi through TCN's. The semiconducting TCN's exhibit diamagnetism at small phi, which is in great contrast with paramagnetism of the metallic TCN's. The induced magnetic moment is proportional to the toroid radius, but independent of the toroid width. The magnetic response is weak, while it is much stronger than that of a mesoscopic semiconductor or metal ring. The persistent current is a linearly periodical function of phi, with a period phi(0)(hc/e). Such an oscillation is the manifestation of the Aharonov-Bohm (AB) effect. Temperature (T) does not destroy the periodical AB oscillation, although it would significantly reduce the persistent currents. The Zeeman splitting may lead to the destruction of the periodicity at very large phi. A larger TCN at lower T and phi is relatively suitable for verifying the AB effect.en_US
dc.language.isoen_USen_US
dc.titlePersistent currents in toroidal carbon nanotubesen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.57.6731en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume57en_US
dc.citation.issue11en_US
dc.citation.spage6731en_US
dc.citation.epage6737en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000072726400082en_US
dc.citation.woscount98en_US
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