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dc.contributor.authorChen, RBen_US
dc.contributor.authorChang, CPen_US
dc.contributor.authorHwang, JSen_US
dc.contributor.authorChuu, DSen_US
dc.contributor.authorLin, MFen_US
dc.date.accessioned2014-12-08T15:19:11Z-
dc.date.available2014-12-08T15:19:11Z-
dc.date.issued2005-05-01en_US
dc.identifier.issn0031-9015en_US
dc.identifier.urihttp://dx.doi.org/10.1143/JPSJ.74.1404en_US
dc.identifier.urihttp://hdl.handle.net/11536/13735-
dc.description.abstractMagnetoelectronic properties of finite carbon nanotubes (CNs) are studied for an arbitrary field direction. They are strongly affected by the nanotube geometry (length, radius; boundary structure), the magnitude and direction of the magnetic field, the Zeeman effect, and the temperature. Geometric structures determine electronic structures and magnetic properties, which thus leads to three types of energy gaps and induced magnetic fields. The critical angle, which corresponds to the change of magnetism, exists in armchair CNs, but not in zigzag CNs. It also depends on the length and the radius of CNs. Finite CNs are very different from infinite CNs. Zeeman splitting could induce complete energy-gap modulation, a drastic change in magnetization, and a gigantic paramagnetic response for all zigzag CNs. The predicted results are observable even at room temperature.en_US
dc.language.isoen_USen_US
dc.subjectcarbon nanotubesen_US
dc.subjectmagnetic propertiesen_US
dc.titleMagnetization of finite carbon nanotubesen_US
dc.typeArticleen_US
dc.identifier.doi10.1143/JPSJ.74.1404en_US
dc.identifier.journalJOURNAL OF THE PHYSICAL SOCIETY OF JAPANen_US
dc.citation.volume74en_US
dc.citation.issue5en_US
dc.citation.spage1404en_US
dc.citation.epage1407en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000229294400014-
dc.citation.woscount17-
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