{"_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. 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