{"_buckets": {"deposit": "38b2a9f5-022e-4259-a5c2-c107e4c43110"}, "_deposit": {"id": "28349", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "28349"}, "status": "published"}, "_oai": {"id": "oai:nagoya.repo.nii.ac.jp:00028349", "sets": ["881"]}, "author_link": ["92605", "92606", "92607", "92608", "92609", "92610", "92611", "92612", "92613", "92614", "92615", "92616", "92617", "92618", "92619"], "item_10_biblio_info_6": {"attribute_name": "書誌情報", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2019-03-05", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "3", "bibliographicPageStart": "032303", "bibliographicVolumeNumber": "26", "bibliographic_titles": [{"bibliographic_title": "Physics of Plasmas", "bibliographic_titleLang": "en"}]}]}, "item_10_description_4": {"attribute_name": "抄録", "attribute_value_mlt": [{"subitem_description": "A preliminary numerical experiment is conducted for laboratory experiments on the generation of magnetized collisionless shocks with high-power lasers by using one-dimensional particle-in-cell simulation. The present study deals with the interaction between a moving aluminum plasma and a nitrogen plasma at rest. In the numerical experiment, the nitrogen plasma is unmagnetized or magnetized by a weak external magnetic field. Since the previous study suggested the generation of a spontaneous magnetic field in the piston (aluminum) plasma due to the Biermann battery, the effect of the magnetic field is of interest. Sharp jumps of the electron density and magnetic field are observed around the interface between the two plasmas as long as one of the two plasmas is magnetized, which indicates the formation of tangential electron-magneto-hydro-dynamic discontinuity. When the aluminum plasma is magnetized, strong compression of both the density and the magnetic field takes place in the pure aluminum plasma during the gyration of nitrogen ions in the aluminum plasma region. The formation of a shock downstream is obtained from the shock jump condition. The results suggest that the spontaneous magnetic field in the piston (aluminum) plasma plays an essential role in the formation of a perpendicular collisionless shock.", "subitem_description_language": "en", "subitem_description_type": "Abstract"}]}, "item_10_description_5": {"attribute_name": "内容記述", "attribute_value_mlt": [{"subitem_description": "ファイル公開：2020-03-05", "subitem_description_language": "ja", "subitem_description_type": "Other"}]}, "item_10_publisher_32": {"attribute_name": "出版者", "attribute_value_mlt": [{"subitem_publisher": "AIP Publishing", "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/10.1063/1.5079906", "subitem_relation_type_select": "DOI"}}]}, "item_10_rights_12": {"attribute_name": "権利", "attribute_value_mlt": [{"subitem_rights": "Copyright 2019 American Institute of Physics. This article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing.The following article appeared in (Physics of Plasmas. v.26, n.3, 2019, p.032303) and may be found at (https://doi.org/10.1063/1.5079906).", "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_61": {"attribute_name": "ISSN（print）", "attribute_value_mlt": [{"subitem_source_identifier": "1070-664X", "subitem_source_identifier_type": "PISSN"}]}, "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": "Umeda, Takayuki", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "92605", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Yamazaki, Ryo", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "92606", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Ohira, Yutaka", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "92607", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Ishizaka, Natsuki", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "92608", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Kakuchi, Shin", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "92609", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Kuramitsu, Yasuhiro", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "92610", "nameIdentifierScheme": 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"http://hdl.handle.net/2237/00030544", "pubdate": {"attribute_name": "PubDate", "attribute_value": "2019-07-11"}, "publish_date": "2019-07-11", "publish_status": "0", "recid": "28349", "relation": {}, "relation_version_is_last": true, "title": ["Full particle-in-cell simulation of the interaction between two plasmas for laboratory experiments on the generation of magnetized collisionless shocks with high-power lasers"], "weko_shared_id": -1}