Representation of solutions to Helmholtz's equation
dc.citation.doi | 10.1063/1.526225 | en_US |
dc.citation.epage | 809 | en_US |
dc.citation.issue | 4 | en_US |
dc.citation.jtitle | Journal of Mathematical Physics | en_US |
dc.citation.spage | 807 | en_US |
dc.citation.volume | 25 | en_US |
dc.contributor.author | Ramm, Alexander G. | |
dc.contributor.authoreid | ramm | en_US |
dc.date.accessioned | 2013-05-08T20:15:55Z | |
dc.date.available | 2013-05-08T20:15:55Z | |
dc.date.issued | 1983-04-01 | |
dc.date.published | 1984 | en_US |
dc.description.abstract | It is proved that any potential of a single layer v is identically equal to a potential of a double layer w in the bounded domain, D, and a necessary and sufficient condition for v≡w in Ω=R³/D, the exterior domain, is given. | en_US |
dc.identifier.uri | http://hdl.handle.net/2097/15763 | |
dc.language.iso | en_US | en_US |
dc.relation.uri | http://doi.org/10.1063/1.526225 | en_US |
dc.rights | This Item is protected by copyright and/or related rights. You are free to use this Item in any way that is permitted by the copyright and related rights legislation that applies to your use. For other uses you need to obtain permission from the rights-holder(s). | en_US |
dc.subject | Helmholtz's equation | en_US |
dc.title | Representation of solutions to Helmholtz's equation | en_US |
dc.type | Article (publisher version) | en_US |