{"_buckets": {"deposit": "8dea1653-33b2-481a-8709-0d5f5d05dd35"}, "_deposit": {"id": "12272", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "12272"}, "status": "published"}, "_oai": {"id": "oai:nagoya.repo.nii.ac.jp:00012272"}, "item_10_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2010-05", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "5", "bibliographicPageEnd": "054506", "bibliographicPageStart": "054506", "bibliographicVolumeNumber": "17", "bibliographic_titles": [{"bibliographic_title": "PHYSICS OF PLASMAS"}]}]}, "item_10_description_4": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "In the present study, we analyze the data sets produced by a one-dimensional Vlasov.Poisson\nsimulation of the weak electron beam-plasma instability to clarify the nonlinearity of the Langmuir\nturbulence excited by the weak-beam interaction. The growth of wave number modes is analyzed by\nusing the momentum equation of the whole electrons. The analysis shows that the primary Langmuir\nwave mode is almost linear, while the nonlinear terms play important roles in the growth of the\nlower harmonic mode and the secondary higher harmonic mode. After the linear growth saturates,\nwhile the wave power of the primary mode is much larger than the other modes, linear and nonlinear\ninteractions occurring in both lower harmonic and secondary higher harmonic modes are more\nactive than those in the primary mode. Nonlinearity in the system comes from the advection rather\nthan the ponderomotive forces.", "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/2237/14152"}, {"subitem_identifier_type": "DOI", "subitem_identifier_uri": "http://dx.doi.org/10.1063/1.3425872"}]}, "item_10_publisher_32": {"attribute_name": "\u51fa\u7248\u8005", "attribute_value_mlt": [{"subitem_publisher": "American Institute of Physics"}]}, "item_10_rights_12": {"attribute_name": "\u6a29\u5229", "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."}]}, "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": "Nariyuki, Y."}], "nameIdentifiers": [{"nameIdentifier": "38741", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Umeda, T."}], "nameIdentifiers": [{"nameIdentifier": "38742", "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": "2018-02-20"}], "displaytype": "detail", "download_preview_message": "", "file_order": 0, "filename": "PHYSICS_OF_PLASMAS_17_5_054506.pdf", "filesize": [{"value": "303.7 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_free", "mimetype": "application/pdf", "size": 303700.0, "url": {"label": "PHYSICS_OF_PLASMAS_17_5_054506.pdf", "url": "https://nagoya.repo.nii.ac.jp/record/12272/files/PHYSICS_OF_PLASMAS_17_5_054506.pdf"}, "version_id": "50672bf8-b2f8-428a-8e01-c87533a5a266"}]}, "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": "On the nonlinearity of the Langmuir turbulence excited by a weak electron beam-plasma interaction", "item_titles": {"attribute_name": "\u30bf\u30a4\u30c8\u30eb", "attribute_value_mlt": [{"subitem_title": "On the nonlinearity of the Langmuir turbulence excited by a weak electron beam-plasma interaction"}]}, "item_type_id": "10", "owner": "1", "path": ["879/880/881"], "permalink_uri": "http://hdl.handle.net/2237/14152", "pubdate": {"attribute_name": "\u516c\u958b\u65e5", "attribute_name_i18n": "\u516c\u958b\u65e5", "attribute_value": "2010-09-16"}, "publish_date": "2010-09-16", "publish_status": "0", "recid": "12272", "relation": {}, "relation_version_is_last": true, "title": ["On the nonlinearity of the Langmuir turbulence excited by a weak electron beam-plasma interaction"], "weko_shared_id": null}