{"created":"2021-03-01T06:12:00.760550+00:00","id":5450,"links":{},"metadata":{"_buckets":{"deposit":"b09d834e-ddb8-4ed3-ab73-cdd1ca7a4037"},"_deposit":{"id":"5450","owners":[],"pid":{"revision_id":0,"type":"depid","value":"5450"},"status":"published"},"_oai":{"id":"oai:nagoya.repo.nii.ac.jp:00005450"},"item_10_biblio_info_6":{"attribute_name":"\u66f8\u8a8c\u60c5\u5831","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2006-06","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"6","bibliographicPageEnd":"063110","bibliographicPageStart":"063110","bibliographicVolumeNumber":"13","bibliographic_titles":[{"bibliographic_title":"Physics of Plasmas"}]}]},"item_10_description_4":{"attribute_name":"\u6284\u9332","attribute_value_mlt":[{"subitem_description":"Electron acceleration in shock waves propagating perpendicular to an external magnetic field, which\nis inhomogeneous and reversed in a finite region, is studied with relativistic particle simulations. By\nthe time a shock wave reaches the inhomogeneous region, some electrons are energized by a small\ncompressive pulse generated in the shock wave. After penetrating this region, the original shock\nwave is damped. However, a new shock wave with the magnetic polarity opposite to that of the\noriginal shock wave is excited. In this secondary shock wave, particle-accelerating compressive\npulses are also generated. Further, after the encounter with the original shock wave, the magnetic\nnull point starts to move with a slightly slower speed than the secondary shock wave, and electric\nfields are formed around it. Some electrons also gain energy in meandering orbits around the\nfield-reversed pulse.","subitem_description_type":"Abstract"}]},"item_10_description_5":{"attribute_name":"\u5185\u5bb9\u8a18\u8ff0","attribute_value_mlt":[{"subitem_description":"8pages","subitem_description_type":"Other"}]},"item_10_identifier_60":{"attribute_name":"URI","attribute_value_mlt":[{"subitem_identifier_type":"HDL","subitem_identifier_uri":"http://hdl.handle.net/2237/7054"}]},"item_10_publisher_32":{"attribute_name":"\u51fa\u7248\u8005","attribute_value_mlt":[{"subitem_publisher":"American Institute of Physics"}]},"item_10_relation_11":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"http://dx.doi.org/10.1063/1.2217709","subitem_relation_type_select":"DOI"}}]},"item_10_rights_12":{"attribute_name":"\u6a29\u5229","attribute_value_mlt":[{"subitem_rights":"Copyright (2006) American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics."}]},"item_10_select_15":{"attribute_name":"\u8457\u8005\u7248\u30d5\u30e9\u30b0","attribute_value_mlt":[{"subitem_select_item":"publisher"}]},"item_10_source_id_7":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"1070-664X","subitem_source_identifier_type":"ISSN"}]},"item_10_text_14":{"attribute_name":"\u30d5\u30a9\u30fc\u30de\u30c3\u30c8","attribute_value_mlt":[{"subitem_text_value":"application/pdf"}]},"item_creator":{"attribute_name":"\u8457\u8005","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"Sato, Masatoshi"}],"nameIdentifiers":[{"nameIdentifier":"14034","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Ohsawa, Yukiharu"}],"nameIdentifiers":[{"nameIdentifier":"14035","nameIdentifierScheme":"WEKO"}]}]},"item_files":{"attribute_name":"\u30d5\u30a1\u30a4\u30eb\u60c5\u5831","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2018-02-19"}],"displaytype":"detail","filename":"PhysPlasmas_13_063110.pdf","filesize":[{"value":"150.7 kB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"PhysPlasmas_13_063110.pdf","url":"https://nagoya.repo.nii.ac.jp/record/5450/files/PhysPlasmas_13_063110.pdf"},"version_id":"df216c26-7826-4cd7-97c1-082ad3fe5f25"}]},"item_language":{"attribute_name":"\u8a00\u8a9e","attribute_value_mlt":[{"subitem_language":"eng"}]},"item_resource_type":{"attribute_name":"\u8cc7\u6e90\u30bf\u30a4\u30d7","attribute_value_mlt":[{"resourcetype":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"Electron acceleration due to small pulses in shock waves in inhomogeneous plasmas: Perpendicular propagation","item_titles":{"attribute_name":"\u30bf\u30a4\u30c8\u30eb","attribute_value_mlt":[{"subitem_title":"Electron acceleration due to small pulses in shock waves in inhomogeneous plasmas: Perpendicular propagation"}]},"item_type_id":"10","owner":"1","path":["336/695/696"],"pubdate":{"attribute_name":"\u516c\u958b\u65e5","attribute_value":"2006-10-24"},"publish_date":"2006-10-24","publish_status":"0","recid":"5450","relation_version_is_last":true,"title":["Electron acceleration due to small pulses in shock waves in inhomogeneous plasmas: Perpendicular propagation"],"weko_creator_id":"1","weko_shared_id":3},"updated":"2021-03-01T13:11:07.142627+00:00"}