{"@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/1363951794496367488.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1017/s026303460018406x"}},{"identifier":{"@type":"URI","@value":"https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S026303460018406X"}},{"identifier":{"@type":"HANDLE","@value":"20.500.14243/7271"}}],"dc:title":[{"@value":"MHD simulations of plasma dynamics in pinch discharges in capillary plasmas"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>Magnetohydrodynamic simulation results related to the \ncapillary discharge dynamics are presented. The main physical \nprocess that should be taken into account is the ablation \nof the capillary wall material evaporated by the heat flux \nfrom the capillary plasma. The possible applications of \nthe capillary discharges related to the physics of the \nX-ray lasers and the use of the capillary plasma to provide \na guiding for ultrashort high-intensity laser pulses over \na distance greater than the defocusing length are discussed.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1383951794496367360","@type":"Researcher","foaf:name":[{"@value":"N.A. BOBROVA"}]},{"@id":"https://cir.nii.ac.jp/crid/1383951794496367490","@type":"Researcher","foaf:name":[{"@value":"S.V. BULANOV"}]},{"@id":"https://cir.nii.ac.jp/crid/1383951794496367493","@type":"Researcher","foaf:name":[{"@value":"D. FARINA"}]},{"@id":"https://cir.nii.ac.jp/crid/1383951794496367488","@type":"Researcher","foaf:name":[{"@value":"R. POZZOLI"}]},{"@id":"https://cir.nii.ac.jp/crid/1383951794496367361","@type":"Researcher","foaf:name":[{"@value":"T.L. RAZINKOVA"}]},{"@id":"https://cir.nii.ac.jp/crid/1383951794496367492","@type":"Researcher","foaf:name":[{"@value":"J.I. SAKAI"}]},{"@id":"https://cir.nii.ac.jp/crid/1383951794496367489","@type":"Researcher","foaf:name":[{"@value":"P.V. SASOROV"}]},{"@id":"https://cir.nii.ac.jp/crid/1383951794496367491","@type":"Researcher","foaf:name":[{"@value":"I.V. SOKOLOV"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"02630346"},{"@type":"EISSN","@value":"1469803X"}],"prism:publicationName":[{"@value":"Laser and Particle Beams"}],"dc:publisher":[{"@value":"Cambridge University Press (CUP)"}],"prism:publicationDate":"2000-10","prism:volume":"18","prism:number":"4","prism:startingPage":"623","prism:endingPage":"638"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://www.cambridge.org/core/terms"],"url":[{"@id":"https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S026303460018406X"}],"createdAt":"2003-10-15","modifiedAt":"2023-11-08","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=___","dc:title":"___"},{"@id":"https://cir.nii.ac.jp/all?q=Electrical%20and%20Electronic%20Engineering","dc:title":"Electrical and Electronic Engineering"},{"@id":"https://cir.nii.ac.jp/all?q=Condensed%20Matter%20Physics","dc:title":"Condensed Matter Physics"},{"@id":"https://cir.nii.ac.jp/all?q=Atomic%20and%20Molecular%20Physics,%20and%20Optics","dc:title":"Atomic and Molecular Physics, and Optics"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360004233903483520","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Characteristics of argon plasma waveguide produced by alumina capillary discharge for short wavelength laser application"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285708873803008","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Properties of a capillary discharge-produced argon plasma waveguide for shorter wavelength source application"}]},{"@id":"https://cir.nii.ac.jp/crid/1520009407778965120","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Effects of plasma dynamics on lasing in fast capillaly discharge"},{"@language":"ja-Kana","@value":"Effects of plasma dynamics on lasing in fast capillaly discharge"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1017/s026303460018406x"},{"@type":"OPENAIRE","@value":"doi_dedup___::e2d70446b00f2720c7a9eac2fdaf2e89"},{"@type":"CROSSREF","@value":"10.1063/1.4712038_references_DOI_2TqDDa77Hvc8Cx4yOudC3Db10dK"},{"@type":"CROSSREF","@value":"10.1063/1.3657136_references_DOI_2TqDDa77Hvc8Cx4yOudC3Db10dK"},{"@type":"CROSSREF","@value":"10.1143/jjap.47.2250_references_DOI_2TqDDa77Hvc8Cx4yOudC3Db10dK"}]}