{"@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/1361137045976075904.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/0022-0396(90)90064-v"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:002203969090064V?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:002203969090064V?httpAccept=text/plain"}}],"dc:title":[{"@value":"Radial entire solutions of a class of quasilinear elliptic equations"}],"description":[{"notation":[{"@value":"will be examined under suitable conditions on the functions f: 8, x R -+ R and g: R, -+R+, where R, =(O, 00); R, = [0, co), and 2 is a real parameter. The capillarity equation and the equation of prescribed mean curvature are important special cases of (1.1) for which g(p) = (1 + P’)-“~ and fir, U) is suitably specialized [ 1, 2, 3, 4, 10, 11, 12, 131. An entire solution of (1.1) is defined to be a function u E C*(R”) satisfying (1.1) at every point XE RN. Our primary objective is to obtain sufficient conditions on f and g for (1.1) to have positive radial entire solutions of the following three types:"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381137045976075904","@type":"Researcher","foaf:name":[{"@value":"Takaŝi Kusano"}]},{"@id":"https://cir.nii.ac.jp/crid/1381137045976075905","@type":"Researcher","foaf:name":[{"@value":"Charles A Swanson"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00220396"}],"prism:publicationName":[{"@value":"Journal of Differential Equations"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"1990-02","prism:volume":"83","prism:number":"2","prism:startingPage":"379","prism:endingPage":"399"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/","https://www.elsevier.com/open-access/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:002203969090064V?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:002203969090064V?httpAccept=text/plain"}],"createdAt":"2005-01-11","modifiedAt":"2019-01-30","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Analysis","dc:title":"Analysis"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360572092481963904","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Ground state solutions for quasilinear scalar field equations arising in nonlinear optics"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1016/0022-0396(90)90064-v"},{"@type":"OPENAIRE","@value":"doi_dedup___::7b016d6a656f96d41e2704fad42f16b9"},{"@type":"CROSSREF","@value":"10.1007/s00030-021-00687-7_references_DOI_S7hYZMrfa6PbwAfwy3d53JW1cfy"}]}