{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1390282679163841024.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1143/jpsj.57.887"}},{"identifier":{"@type":"BIBCODE","@value":"1988JPSJ...57..887A"}},{"identifier":{"@type":"NDL_BIB_ID","@value":"3178481"}},{"identifier":{"@type":"URI","@value":"http://id.ndl.go.jp/bib/3178481"}},{"identifier":{"@type":"URI","@value":"https://ndlsearch.ndl.go.jp/books/R000000004-I3178481"}},{"identifier":{"@type":"URI","@value":"http://journals.jps.jp/doi/pdf/10.1143/JPSJ.57.887"}},{"identifier":{"@type":"NAID","@value":"210000094483"}},{"identifier":{"@type":"NAID","@value":"110001976529"}},{"identifier":{"@type":"NAID","@value":"130003899732"}}],"dc:title":[{"@language":"en","@value":"Probe Diagnostics in Negative Ion Containing Plasma"},{"@language":"ja-Kana","@value":"Probe Diagnostics in Negative Ion Conta"}],"dc:language":"en","description":[{"type":"abstract","notation":[{"@language":"en","@value":"The effect of negative ions on the probe characteristics is studied theoretically and experimentally by using iodine and iodine-argon mixture plasmas. For a small ratio of negative ion to electron densities, the negative ion density and temperature can be determined from a sharp peak on the second derivative of the probe characteristics. At a higher ratio, the ratio of saturation currents at positive and negative probe biases should be used by calibrating the ratio with that of the case without negative ions. For a negative ion dominating plasma, a change of the Bohm criterion by negative ions should be considered and the parameters can be obtained from the probe characteristics which are nearly symmetric at positive and negative biases."}],"abstractLicenseFlag":"disallow"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1410282679163841024","@type":"Researcher","personIdentifier":[{"@type":"NRID","@value":"9000254564543"},{"@type":"NRID","@value":"9000401859898"}],"foaf:name":[{"@language":"en","@value":"Amemiya Hiroshi"}],"jpcoar:affiliationName":[{"@language":"en","@value":"The Institute of Physical and Chemical Research"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00319015"},{"@type":"LISSN","@value":"00319015"},{"@type":"EISSN","@value":"13474073"},{"@type":"NDL_BIB_ID","@value":"000000118709"},{"@type":"ISSN","@value":"00319015"},{"@type":"NCID","@value":"AA00704814"}],"prism:publicationName":[{"@language":"en","@value":"Journal of the Physical Society of Japan"},{"@language":"ja","@value":"Ｊｏｕｒｎａｌ　ｏｆ　ｔｈｅ　Ｐｈｙｓｉｃａｌ　Ｓｏｃｉｅｔｙ　ｏｆ　Ｊａｐａｎ"},{"@language":"en","@value":"JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN"},{"@language":"en","@value":"JPSJ"},{"@language":"ja","@value":"ＪＰＳＪ"}],"dc:publisher":[{"@language":"en","@value":"THE PHYSICAL SOCIETY OF JAPAN"},{"@language":"ja","@value":"一般社団法人 日本物理学会"}],"prism:publicationDate":"1988","prism:volume":"57","prism:number":"3","prism:startingPage":"887","prism:endingPage":"902"},"reviewed":"false","url":[{"@id":"http://id.ndl.go.jp/bib/3178481"},{"@id":"https://ndlsearch.ndl.go.jp/books/R000000004-I3178481"},{"@id":"http://journals.jps.jp/doi/pdf/10.1143/JPSJ.57.887"}],"availableAt":"1988","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360003446838626688","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Experiments on the Energy Distribution Function in Hydrogen Plasmas"}]},{"@id":"https://cir.nii.ac.jp/crid/1360003446840777728","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Production of Electron-Free Plasma by Using a Magnetic Filter in Radio Frequency Discharge"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011146562141952","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant=\"normal\">H</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant=\"normal\">D</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>Production in Plasmas"}]},{"@id":"https://cir.nii.ac.jp/crid/1360284921815492480","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Negative Ions and Energy Distribution in a Hydrogen Plasma Device"}]},{"@id":"https://cir.nii.ac.jp/crid/1360284921817404288","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Floating Potential in Negative-Ion-Containing Plasma"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292618739575040","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The operation of Langmuir probes in electro-negative plasmas"}]},{"@id":"https://cir.nii.ac.jp/crid/1360566396792738304","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Characteristics of Double Probe in Negative Ion-Containing Plasmas"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574094610521344","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Electron energy distributions in plasmas IV. 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