FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2058549500> ?p ?o ?g. }

• W2058549500 endingPage "1897" @default.
• W2058549500 startingPage "1884" @default.
• W2058549500 abstract "We study classical solutions of SU(2) Yang-Mills field equations, with or without coupled scalar fields, in curved spacetimes. We consider, essentially, only static, spherically symmetric background metrics, for both Lorentz and Euclidean signatures. Section I presents the motivation for searching such solutions. In Sec. II, the equations of motion for a class of Ansatze and several static solutions are given, namely a class of scalar fields compatible with a point monopole and particular solutions, for gauge fields alone, in background Schwarzschild and de Sitter metrics, respectively. Some interesting properties are discussed. In Sec. III a finite-action, Prasad-Sommerfield-type solution is constructed for the O(4,1) de Sitter metric. In Sec. IV it is shown how one single, simple de Sitter solution can lead to various well-known flat-space solutions, and to new ones, through a systematic exploitation of conformal equivalence. Self-duality constraints are formulated explicitly in Sec. V for a static spherically symmetric metric. Certain results for the Robinson-Bertotti metric are given in Sec. VI." @default.
• W2058549500 created "2016-06-24" @default.
• W2058549500 creator A5068725978 @default.
• W2058549500 creator A5068959922 @default.
• W2058549500 creator A5074848635 @default.
• W2058549500 date "1979-10-15" @default.
• W2058549500 modified "2023-09-26" @default.
• W2058549500 title "Gauge field configurations in curved spacetimes. I" @default.
• W2058549500 cites W1972838432 @default.
• W2058549500 cites W1973321745 @default.
• W2058549500 cites W1984497992 @default.
• W2058549500 cites W1985246007 @default.
• W2058549500 cites W1986029234 @default.
• W2058549500 cites W1989439785 @default.
• W2058549500 cites W1992367107 @default.
• W2058549500 cites W1993417984 @default.
• W2058549500 cites W2000288860 @default.
• W2058549500 cites W2003089274 @default.
• W2058549500 cites W2009713237 @default.
• W2058549500 cites W2016885246 @default.
• W2058549500 cites W2032838741 @default.
• W2058549500 cites W2034280983 @default.
• W2058549500 cites W2034654895 @default.
• W2058549500 cites W2037438277 @default.
• W2058549500 cites W2038122285 @default.
• W2058549500 cites W2042049191 @default.
• W2058549500 cites W2042691154 @default.
• W2058549500 cites W2046588154 @default.
• W2058549500 cites W2048480494 @default.
• W2058549500 cites W2052707636 @default.
• W2058549500 cites W2057558486 @default.
• W2058549500 cites W2057592072 @default.
• W2058549500 cites W2071592106 @default.
• W2058549500 cites W2071633647 @default.
• W2058549500 cites W2072802599 @default.
• W2058549500 cites W2076669740 @default.
• W2058549500 cites W2077922437 @default.
• W2058549500 cites W2080143633 @default.
• W2058549500 cites W2090166146 @default.
• W2058549500 cites W2120830691 @default.
• W2058549500 cites W2127529674 @default.
• W2058549500 cites W2128737304 @default.
• W2058549500 cites W2149447505 @default.
• W2058549500 cites W4234514872 @default.
• W2058549500 cites W4243372458 @default.
• W2058549500 doi "https://doi.org/10.1103/physrevd.20.1884" @default.
• W2058549500 hasPublicationYear "1979" @default.
• W2058549500 type Work @default.
• W2058549500 sameAs 2058549500 @default.
• W2058549500 citedByCount "34" @default.
• W2058549500 countsByYear W20585495002014 @default.
• W2058549500 countsByYear W20585495002015 @default.
• W2058549500 countsByYear W20585495002016 @default.
• W2058549500 countsByYear W20585495002018 @default.
• W2058549500 countsByYear W20585495002020 @default.
• W2058549500 countsByYear W20585495002021 @default.
• W2058549500 crossrefType "journal-article" @default.
• W2058549500 hasAuthorship W2058549500A5068725978 @default.
• W2058549500 hasAuthorship W2058549500A5068959922 @default.
• W2058549500 hasAuthorship W2058549500A5074848635 @default.
• W2058549500 hasConcept C107829132 @default.
• W2058549500 hasConcept C110521144 @default.
• W2058549500 hasConcept C121332964 @default.
• W2058549500 hasConcept C129782007 @default.
• W2058549500 hasConcept C134306372 @default.
• W2058549500 hasConcept C136125196 @default.
• W2058549500 hasConcept C14037181 @default.
• W2058549500 hasConcept C147452769 @default.
• W2058549500 hasConcept C149298590 @default.
• W2058549500 hasConcept C181830111 @default.
• W2058549500 hasConcept C19262093 @default.
• W2058549500 hasConcept C2524010 @default.
• W2058549500 hasConcept C33923547 @default.
• W2058549500 hasConcept C37914503 @default.
• W2058549500 hasConcept C5667645 @default.
• W2058549500 hasConcept C57691317 @default.
• W2058549500 hasConcept C62520636 @default.
• W2058549500 hasConcept C74650414 @default.
• W2058549500 hasConcept C84999194 @default.
• W2058549500 hasConcept C98214594 @default.
• W2058549500 hasConceptScore W2058549500C107829132 @default.
• W2058549500 hasConceptScore W2058549500C110521144 @default.
• W2058549500 hasConceptScore W2058549500C121332964 @default.
• W2058549500 hasConceptScore W2058549500C129782007 @default.
• W2058549500 hasConceptScore W2058549500C134306372 @default.
• W2058549500 hasConceptScore W2058549500C136125196 @default.
• W2058549500 hasConceptScore W2058549500C14037181 @default.
• W2058549500 hasConceptScore W2058549500C147452769 @default.
• W2058549500 hasConceptScore W2058549500C149298590 @default.
• W2058549500 hasConceptScore W2058549500C181830111 @default.
• W2058549500 hasConceptScore W2058549500C19262093 @default.
• W2058549500 hasConceptScore W2058549500C2524010 @default.
• W2058549500 hasConceptScore W2058549500C33923547 @default.
• W2058549500 hasConceptScore W2058549500C37914503 @default.
• W2058549500 hasConceptScore W2058549500C5667645 @default.
• W2058549500 hasConceptScore W2058549500C57691317 @default.
• W2058549500 hasConceptScore W2058549500C62520636 @default.
• W2058549500 hasConceptScore W2058549500C74650414 @default.

• next