{"created":"2025-02-21T04:13:03.438552+00:00","id":2008107,"links":{},"metadata":{"_buckets":{"deposit":"f3e03beb-70f0-4cba-b45a-83b66c29054b"},"_deposit":{"created_by":41,"id":"2008107","owners":[41],"pid":{"revision_id":0,"type":"depid","value":"2008107"},"status":"published"},"_oai":{"id":"oai:hiroshima.repo.nii.ac.jp:02008107","sets":["1730444907710"]},"author_link":[],"item_1617186331708":{"attribute_name":"Title","attribute_value_mlt":[{"subitem_title":"Spin Berry phase in the Fermi-arc states","subitem_title_language":"en"}]},"item_1617186419668":{"attribute_name":"Creator","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"Imura, Ken-Ichiro","creatorNameLang":"en"}],"familyNames":[{"familyName":"Imura","familyNameLang":"en"}],"givenNames":[{"givenName":"Ken-Ichiro","givenNameLang":"en"}]},{"creatorNames":[{"creatorName":"Takane, Yositake","creatorNameLang":"en"}],"familyNames":[{"familyName":"Takane","familyNameLang":"en"}],"givenNames":[{"givenName":"Yositake","givenNameLang":"en"}]}]},"item_1617186476635":{"attribute_name":"Access Rights","attribute_value_mlt":[{"subitem_access_right":"open access","subitem_access_right_uri":"http://purl.org/coar/access_right/c_abf2"}]},"item_1617186499011":{"attribute_name":"Rights","attribute_value_mlt":[{"subitem_rights":"(c) 2011 American Physical Society"}]},"item_1617186609386":{"attribute_name":"Subject","attribute_value_mlt":[{"subitem_subject":"420","subitem_subject_scheme":"NDC"}]},"item_1617186626617":{"attribute_name":"Description","attribute_value_mlt":[{"subitem_description":"An unusual electronic property of a Weyl semimetallic nanowire is revealed. Its band dispersion exhibits multiple subbands of partially flat dispersion, originating from the Fermi-arc states. Remarkably, the lowest energy flat subbands bear a finite size energy gap, implying that electrons in the Fermi-arc surface states are susceptible to the spin Berry phase. This is shown to be a consequence of spin-to-surface locking in the surface electronic states. We verify this behavior and the existence of the spin Berry phase in the low-energy effective theory of Fermi-arc surface states on a cylindrical nanowire by deriving the latter from a bulk Weyl Hamiltonian. We point out that in any surface state exhibiting a spin Berry phase π, a zero-energy bound state is formed along a magnetic flux tube of strength Φ0/2=hc/(2e). This effect is highlighted in a surfaceless bulk system pierced by a dislocation line, which shows a 1D chiral mode along the dislocation line.","subitem_description_language":"en"}]},"item_1617186643794":{"attribute_name":"Publisher","attribute_value_mlt":[{"subitem_publisher":"American Physical Society"}]},"item_1617186702042":{"attribute_name":"Language","attribute_value_mlt":[{"subitem_language":"eng"}]},"item_1617186920753":{"attribute_name":"Source Identifier","attribute_value_mlt":[{"subitem_source_identifier":"1098-0121","subitem_source_identifier_type":"ISSN"},{"subitem_source_identifier":"AA11187113","subitem_source_identifier_type":"NCID"}]},"item_1617187024783":{"attribute_name":"Page Start","attribute_value_mlt":[{"subitem_start_page":"245415"}]},"item_1617187056579":{"attribute_name":"Bibliographic Information","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2011","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"24","bibliographicPageStart":"245415","bibliographicVolumeNumber":"84","bibliographic_titles":[{"bibliographic_title":"Physical Review B"},{"bibliographic_title":"Physical Review B"}]}]},"item_1617258105262":{"attribute_name":"Resource Type","attribute_value_mlt":[{"resourcetype":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_1617265215918":{"attribute_name":"Version Type","attribute_value_mlt":[{"subitem_version_resource":"http://purl.org/coar/version/c_970fb48d4fbd8a85","subitem_version_type":"VoR"}]},"item_1617353299429":{"attribute_name":"Relation","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.1103/PhysRevB.84.245415","subitem_relation_type_select":"DOI"}},{"subitem_relation_type_id":{"subitem_relation_type_id_text":"http://dx.doi.org/10.1103/PhysRevB.84.245415","subitem_relation_type_select":"DOI"}}]},"item_1617605131499":{"attribute_name":"File","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_access","date":[{"dateType":"Available","dateValue":"2023-03-18"}],"displaytype":"simple","filename":"PhysRevB.84.245415.pdf","filesize":[{"value":"2.4 MB"}],"mimetype":"application/pdf","url":{"objectType":"fulltext","url":"https://hiroshima.repo.nii.ac.jp/record/2008107/files/PhysRevB.84.245415.pdf"},"version_id":"2803b597-b7c0-488d-91f9-d4959354fd41"}]},"item_1732771732025":{"attribute_name":"旧ID","attribute_value":"33945"},"item_title":"Spin Berry phase in the Fermi-arc states","item_type_id":"40003","owner":"41","path":["1730444907710"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2023-03-18"},"publish_date":"2023-03-18","publish_status":"0","recid":"2008107","relation_version_is_last":true,"title":["Spin Berry phase in the Fermi-arc states"],"weko_creator_id":"41","weko_shared_id":-1},"updated":"2025-02-22T03:11:33.669963+00:00"}