{"created":"2021-03-01T06:19:13.241547+00:00","id":12274,"links":{},"metadata":{"_buckets":{"deposit":"a5e11942-cb5f-47e3-b16c-bdfbddaaa327"},"_deposit":{"id":"12274","owners":[],"pid":{"revision_id":0,"type":"depid","value":"12274"},"status":"published"},"_oai":{"id":"oai:nagoya.repo.nii.ac.jp:00012274","sets":["336:695:696"]},"author_link":["38750","38751"],"item_10_biblio_info_6":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2009-11","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"11","bibliographicPageEnd":"112305","bibliographicPageStart":"112305","bibliographicVolumeNumber":"16","bibliographic_titles":[{"bibliographic_title":"PHYSICS OF PLASMAS","bibliographic_titleLang":"en"}]}]},"item_10_description_4":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"A magnetosonic shock wave propagating obliquely to an external magnetic field can trap electrons and accelerate them to ultrarelativistic energies. The effect of trapped electrons on electromagnetic fields in a shock wave is studied by theory and particle simulations. The expressions for field strengths are analytically obtained, including the number of trapped electrons nt as a factor. It is shown that as nt increases, the magnitude of F increases, where F is the integral of the parallel electric field, E∥ = (E⋅B)/B, along B. Theoretical analysis also suggests that the increase in F causes the electrons to be trapped deeper and accelerated to higher kinetic energies. These theoretical predictions are verified with relativistic electromagnetic particle simulations.","subitem_description_language":"en","subitem_description_type":"Abstract"}]},"item_10_identifier_60":{"attribute_name":"URI","attribute_value_mlt":[{"subitem_identifier_type":"HDL","subitem_identifier_uri":"http://hdl.handle.net/2237/14154"},{"subitem_identifier_type":"DOI","subitem_identifier_uri":"http://dx.doi.org/10.1063/1.3264736"}]},"item_10_publisher_32":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"American Institute of Physics","subitem_publisher_language":"en"}]},"item_10_relation_11":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type":"isVersionOf","subitem_relation_type_id":{"subitem_relation_type_id_text":"https://doi.org/10.1063/1.3264736","subitem_relation_type_select":"DOI"}}]},"item_10_rights_12":{"attribute_name":"権利","attribute_value_mlt":[{"subitem_rights":"Copyright (2010) 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.","subitem_rights_language":"en"}]},"item_10_select_15":{"attribute_name":"著者版フラグ","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":"PISSN"}]},"item_10_text_14":{"attribute_name":"フォーマット","attribute_value_mlt":[{"subitem_text_value":"application/pdf"}]},"item_1615787544753":{"attribute_name":"出版タイプ","attribute_value_mlt":[{"subitem_version_resource":"http://purl.org/coar/version/c_970fb48d4fbd8a85","subitem_version_type":"VoR"}]},"item_access_right":{"attribute_name":"アクセス権","attribute_value_mlt":[{"subitem_access_right":"open access","subitem_access_right_uri":"http://purl.org/coar/access_right/c_abf2"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"Toida, Mieko","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"38750","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Shikii, Kenta","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"38751","nameIdentifierScheme":"WEKO"}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2018-02-20"}],"displaytype":"detail","filename":"PHYSICS_OF_PLASMAS_16_11_112305.pdf","filesize":[{"value":"2.7 MB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"PHYSICS_OF_PLASMAS_16_11_112305.pdf","objectType":"fulltext","url":"https://nagoya.repo.nii.ac.jp/record/12274/files/PHYSICS_OF_PLASMAS_16_11_112305.pdf"},"version_id":"940e98c5-d471-405e-b639-23a5d0463263"}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"eng"}]},"item_resource_type":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"resourcetype":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"Effects of trapped electrons on electromagnetic fields in an oblique shock wave","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Effects of trapped electrons on electromagnetic fields in an oblique shock wave","subitem_title_language":"en"}]},"item_type_id":"10","owner":"1","path":["696"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2010-09-16"},"publish_date":"2010-09-16","publish_status":"0","recid":"12274","relation_version_is_last":true,"title":["Effects of trapped electrons on electromagnetic fields in an oblique shock wave"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-01-16T04:59:12.287030+00:00"}