{"created":"2021-03-01T06:25:49.946190+00:00","id":18424,"links":{},"metadata":{"_buckets":{"deposit":"8c06ba42-cdc4-4cc5-85a0-ac8e3520b51b"},"_deposit":{"id":"18424","owners":[],"pid":{"revision_id":0,"type":"depid","value":"18424"},"status":"published"},"_oai":{"id":"oai:nagoya.repo.nii.ac.jp:00018424"},"item_9_biblio_info_6":{"attribute_name":"\u66f8\u8a8c\u60c5\u5831","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2013","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"100","bibliographicPageStart":"93","bibliographicVolumeNumber":"60","bibliographic_titles":[{"bibliographic_title":"The Journal of Earth and Planetary Sciences, Nagoya University"}]}]},"item_9_description_4":{"attribute_name":"\u6284\u9332","attribute_value_mlt":[{"subitem_description":"Approximations of the mean ionization potential have been compared with the latest dataset. Obtained chemical compositions are sensitive to the chosen model of the mean ionization potential. Selection of the mean ionization potential model causes about 5% uncertainty of chemical compositions. However, Mg# (= Mg / (Mg + Fe)) and apparent U-Th-total Pb age are less sensitive to the mean ionization model, and uncertainty is less than 2 %. The conventional ZAF model is more sensitive to the mean ionization model than the double parabola model and surface-center Gaussian model.","subitem_description_type":"Abstract"}]},"item_9_identifier_60":{"attribute_name":"URI","attribute_value_mlt":[{"subitem_identifier_type":"HDL","subitem_identifier_uri":"http://hdl.handle.net/2237/20541"}]},"item_9_identifier_registration":{"attribute_name":"ID\u767b\u9332","attribute_value_mlt":[{"subitem_identifier_reg_text":"10.18999/joueps.60.93","subitem_identifier_reg_type":"JaLC"}]},"item_9_publisher_32":{"attribute_name":"\u51fa\u7248\u8005","attribute_value_mlt":[{"subitem_publisher":"Dept. of Earth and Planetary Sciences, Nagoya University"}]},"item_9_select_15":{"attribute_name":"\u8457\u8005\u7248\u30d5\u30e9\u30b0","attribute_value_mlt":[{"subitem_select_item":"publisher"}]},"item_9_source_id_7":{"attribute_name":"ISSN\uff08print\uff09","attribute_value_mlt":[{"subitem_source_identifier":"0919-875X","subitem_source_identifier_type":"ISSN"}]},"item_creator":{"attribute_name":"\u8457\u8005","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"KATO, Takenori"}],"nameIdentifiers":[{"nameIdentifier":"53522","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"JEEN, Mi-Jung"}],"nameIdentifiers":[{"nameIdentifier":"53523","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"CHO, Deung-Lyong"}],"nameIdentifiers":[{"nameIdentifier":"53524","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":"2018-02-21"}],"displaytype":"detail","filename":"60-2.pdf","filesize":[{"value":"469.4 kB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"60-2.pdf","url":"https://nagoya.repo.nii.ac.jp/record/18424/files/60-2.pdf"},"version_id":"2b9499ae-b070-465e-bd90-5ebe5a6d62d3"}]},"item_keyword":{"attribute_name":"\u30ad\u30fc\u30ef\u30fc\u30c9","attribute_value_mlt":[{"subitem_subject":"electron probe microanalysis","subitem_subject_scheme":"Other"},{"subitem_subject":"mean ionization potential","subitem_subject_scheme":"Other"},{"subitem_subject":"matrix correction","subitem_subject_scheme":"Other"},{"subitem_subject":"stopping power","subitem_subject_scheme":"Other"}]},"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":"departmental bulletin paper","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"Validation of physical parameters in quantitative electron probe microanalysis (EPMA) Part II : mean ionization potential","item_titles":{"attribute_name":"\u30bf\u30a4\u30c8\u30eb","attribute_value_mlt":[{"subitem_title":"Validation of physical parameters in quantitative electron probe microanalysis (EPMA) Part II : mean ionization potential"}]},"item_type_id":"9","owner":"1","path":["336/337/338/1636"],"pubdate":{"attribute_name":"\u516c\u958b\u65e5","attribute_value":"2014-09-02"},"publish_date":"2014-09-02","publish_status":"0","recid":"18424","relation_version_is_last":true,"title":["Validation of physical parameters in quantitative electron probe microanalysis (EPMA) Part II : mean ionization potential"],"weko_creator_id":"1","weko_shared_id":null},"updated":"2021-03-01T16:41:10.485366+00:00"}