{"_buckets": {"deposit": "58adf171-1b41-40ce-98f4-2444eba31601"}, "_deposit": {"id": "5446", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "5446"}, "status": "published"}, "_oai": {"id": "oai:nagoya.repo.nii.ac.jp:00005446"}, "item_10_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2006-01", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "1", "bibliographicPageEnd": "013301", "bibliographicPageStart": "013301", "bibliographicVolumeNumber": "13", "bibliographic_titles": [{"bibliographic_title": "Physics of Plasmas"}]}]}, "item_10_description_4": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "The electron density and temperature obtained from the line intensity ratio method of He I\n(\u03bb=667.8, 706.5, and 728.1 nm) are compared to the probe method in a divertor simulator. When\na collisional radiative model that does not include the effect of the radiation transport was used for\nthe analysis, ne obtained from the spectroscopic method was significantly higher than that from the\nelectrostatic probe method. The discrepancy between the two methods increases with the gas\npressure; in other words, it increases with the optical thickness. In the case that the effect of the\nradiation trapping is taken into consideration using optical escape factor, the discrepancy becomes\nmoderate. And then, the parameters obtained from the line intensity ratio method agree with the\nprobe method within a factor of 2 in the case that the radiation trapping was introduced with\nR=0.05 m, which corresponds to the column radius of the spatial profile of the excited population\ndensity. In recombining plasmas, however, it was shown that the line intensity ratios might not be\nappropriate because the recombining component broke the monotonic increase/decrease\ndependences of the line intensity ratios on ne and Te. A measurement of another He I line intensity\nof 447.1 nm (2^3P\u21904^3D) is proposed for solving the problem.", "subitem_description_type": "Abstract"}]}, "item_10_description_5": {"attribute_name": "\u5185\u5bb9\u8a18\u8ff0", "attribute_value_mlt": [{"subitem_description": "9pages", "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/2237/7050"}]}, "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/10.1063/1.2164461", "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": "Kajita, Shin"}], "nameIdentifiers": [{"nameIdentifier": "14001", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Ohno, Noriyasu"}], "nameIdentifiers": [{"nameIdentifier": "14002", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Takamura, Shuichi"}], "nameIdentifiers": [{"nameIdentifier": "14003", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Nakano, Tomohide"}], "nameIdentifiers": [{"nameIdentifier": "14004", "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", "download_preview_message": "", "file_order": 0, "filename": "PhysPlasmas_13_013301.pdf", "filesize": [{"value": "717.8 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_free", "mimetype": "application/pdf", "size": 717800.0, "url": {"label": "PhysPlasmas_13_013301.pdf", "url": "https://nagoya.repo.nii.ac.jp/record/5446/files/PhysPlasmas_13_013301.pdf"}, "version_id": "7495d5bf-3bc1-4ef3-9aa4-b502c7fc872b"}]}, "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": "Comparison of He I line intensity ratio method and electrostatic probe for electron density and temperature measurements in NAGDIS-II", "item_titles": {"attribute_name": "\u30bf\u30a4\u30c8\u30eb", "attribute_value_mlt": [{"subitem_title": "Comparison of He I line intensity ratio method and electrostatic probe for electron density and temperature measurements in NAGDIS-II"}]}, "item_type_id": "10", "owner": "1", "path": ["320/321/322"], "permalink_uri": "http://hdl.handle.net/2237/7050", "pubdate": {"attribute_name": "\u516c\u958b\u65e5", "attribute_value": "2006-10-24"}, "publish_date": "2006-10-24", "publish_status": "0", "recid": "5446", "relation": {}, "relation_version_is_last": true, "title": ["Comparison of He I line intensity ratio method and electrostatic probe for electron density and temperature measurements in NAGDIS-II"], "weko_shared_id": 3}