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New backlund-transformations and superposition principle for gravitational-fields with symmetries

dc.contributor.authorChinea Trujillo, Francisco Javier
dc.date.accessioned2023-06-21T02:08:55Z
dc.date.available2023-06-21T02:08:55Z
dc.date.issued1983
dc.description©1983 The American Physical Society. Financial support by Comision Asesora de Investigacion Científica y Técnica is gratefully acknowledged.
dc.description.abstractVector Bäcklund transformations which relate solutions of the vacuum Einstein equations having two commuting Killing fields are introduced. Such transformations generalize those found by Pohlmeyer in connection with the nonlinear δ model. A simple algebraic superposition principle, which permits the combination of Bäcklund transforms in order to get new solutions, is given. The superposition preserves the asymptotic flatness condition, and the whole scheme is manisfestly O(2, 1) invariant.
dc.description.departmentDepto. de Física Teórica
dc.description.facultyFac. de Ciencias Físicas
dc.description.refereedTRUE
dc.description.sponsorshipComision Asesora de Investigacion Científica y Técnica
dc.description.statuspub
dc.eprint.idhttps://eprints.ucm.es/id/eprint/31183
dc.identifier.doi10.1103/PhysRevLett.50.221
dc.identifier.issn0031-9007
dc.identifier.officialurlhttp://dx.doi.org/10.1103/PhysRevLett.50.221
dc.identifier.relatedurlhttp://journals.aps.org
dc.identifier.urihttps://hdl.handle.net/20.500.14352/64979
dc.issue.number4
dc.journal.titlePhysical review letters
dc.language.isoeng
dc.page.final224
dc.page.initial221
dc.publisherAmerican Physical Society
dc.rights.accessRightsopen access
dc.subject.cdu51-73
dc.subject.keywordPhysics
dc.subject.keywordMultidisciplinary
dc.subject.ucmFísica-Modelos matemáticos
dc.subject.ucmFísica matemática
dc.titleNew backlund-transformations and superposition principle for gravitational-fields with symmetries
dc.typejournal article
dc.volume.number50
dcterms.references1. F. J. Ernst, Phys. Bev. 167, 1175 (1968). 2. D. Kramer and G. Neugebauer, Commun. Math. Phys. 10, 132 (1968). 3. R. Geroch, J. Math. Phys. (N.Y.) 13, 394 (1972). 4. W. Kinnersley, J. Math. Phys. (N.Y.) 18, 1529 (1977). 5. W. Kinnersley and D. M. Chitre, Phys. Bev. Lett. 4O, 1608 (1978). 6. D. Maison, Phys. Bev. Lett. 41, 521 (1978), and J. Math. Phys. (N.Y.) 20, 871 (1979). 7. C. Hoenselaers, W. Kinnersley, and B. C. Xanthopoulos, Phys. Bev. Lett. 42, 481 (1978), and J. Math. Phys. (N.Y.) 20, 2530 (1979). 8. V. A. Belinskii and V. E. Zakharov, Zh. Eksp. Teor. Fiz. 75, 1955 (1978) [ Sov. Phys. JETP 48, 985 (1978)]. 8. Backlund transformations for the Ernst equation of general relativity were independently introduced for the first time in the following: B. K. Harrison, Phys. Bev. Lett. 41, 1197, 1835(E) (1978); G. Neugebauer, J. Phys. A12, L67 (1979). Other expressions for Bäcklund transformations of the same problem, and their relation with gauge transformations, may be seen in the followirg: M. Omote and M. Wadati, J. Math. Phys. (N.Y.) 22, 961 (1981); F.J. Chinea, Phys. Bev. D 24, 1053 (1981), and 26, 2175(E) (1982), and Physica (Utrecht) 114A, 151 (1982). 10. T. Lewis, Proc. Boy. Soc. London, Ser. A 136, 176 (1932); A. Papapetrou, Ann. Phys. (Leipzig) 12, 309 (1953). 11. G. Neugebauer and D. Kramer, Exp. Tech. Phys. 28, 3 (1980); G. Neugebauer, J. Phys. A 13, L19 (1980); D. Kramer and G. Neugebauer, Phys. Lett. 75A, 259 (1980). 12. B. K. Harrison, Phys. Bev. D 21, 1695 (1980). 13. K. Pohlmeyer, Commun. Math. Phys. 46, 207 (1976). 14. A permutability property for Bäcklund transformations of the Ernst equation was found by G. Neugebauer (Ref. 9)
dspace.entity.typePublication
relation.isAuthorOfPublicatione4399503-cd94-463f-9f57-413f91e12fc8
relation.isAuthorOfPublication.latestForDiscoverye4399503-cd94-463f-9f57-413f91e12fc8

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