FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2036157570> ?p ?o ?g. }

• W2036157570 abstract "Abstract The dynamics of the spherically symmetric system of gravitation interacting with scalar and Yang-Mills fields is presented in the context of the canonical formalism. The gauge group considered is a general (compact and semisimple) N parameter group. The scalar (Higgs) field transforms according to an unspecified M-dimensional orthogonal representation of the gauge group. The canonical formalism is based on Dirac's techniques for dealing with constrained hamiltonian systems. First the condition that the scalar and Yang-Mills fields and their conjugate momenta be spherically symmetric up to a gauge is formulated and solved for global gauge transformations, finding, in a general gauge, the explicit angular dependence of the fields and conjugate momenta. It is shown that if the gauge group does not admit a subgroup (locally) isomorphic to the rotation group, then the dynamical variables can only be manifestly spherically symmetric. If the opposite is the case, then the number of allowed degrees of freedom is connected to the angular momentum content of the adjoint representation of the gauge group. Once the suitable variables with explicit angular dependence have been obtained, a reduced action is derived by integrating away the angular coordinates. The canonical formulation of the problem is now based on dynamical variables depending only on an arbitrary radial coordinate r and an arbitrary time coordinate t. Besides the gravitational variables, the formalism now contains two pairs of N-vector variables (R, π r ), (Θ, πΘ), corresponding to the allowed Yang-Mills degrees of freedom and one pair of M-vector variables, (h, πh), associated with the original scalar field. The reduced Hamiltonian is invariant under a group of r-dependent gauge transformations such that R plays the role of the gauge field (transforming in the typically inhomogeneous way) and in terms of which the gauge covariant derivatives of Θ and h naturally appear. No derivatives of R appear in the Hamiltonian and the gauge freedom allows us to define a gauge in which R is zero. Also the r and t coordinates are fixed in a way consistent with the equations of motion. Some nontrivial static solutions are found. One of these solutions is given in closed form; it is singular and corresponds to a generalization of the singular solution found in the literature with different degrees of generality and the geometry is described by the Reissner-Nordstrom metric. The other solution is defined through its asymptotic behavior. It generalizes to curved space the finite energy solution discyssed by Julia and Zee in flat space." @default.
• W2036157570 created "2016-06-24" @default.
• W2036157570 creator A5019256598 @default.
• W2036157570 date "1977-09-01" @default.
• W2036157570 modified "2023-09-30" @default.
• W2036157570 title "Canonical formulation of the spherically symmetric einstein-Yang-Mills-Higgs system for a general gauge group" @default.
• W2036157570 cites W145593370 @default.
• W2036157570 cites W1635626242 @default.
• W2036157570 cites W1994939569 @default.
• W2036157570 cites W1995686300 @default.
• W2036157570 cites W1996932869 @default.
• W2036157570 cites W2003182627 @default.
• W2036157570 cites W2027710569 @default.
• W2036157570 cites W2029400431 @default.
• W2036157570 cites W2042049191 @default.
• W2036157570 cites W2046692269 @default.
• W2036157570 cites W2052707636 @default.
• W2036157570 cites W2070427230 @default.
• W2036157570 cites W2104723177 @default.
• W2036157570 cites W2149447505 @default.
• W2036157570 cites W2168837599 @default.
• W2036157570 cites W2171403598 @default.
• W2036157570 cites W2180581473 @default.
• W2036157570 cites W2314212607 @default.
• W2036157570 cites W3041643375 @default.
• W2036157570 doi "https://doi.org/10.1016/0003-4916(77)90352-9" @default.
• W2036157570 hasPublicationYear "1977" @default.
• W2036157570 type Work @default.
• W2036157570 sameAs 2036157570 @default.
• W2036157570 citedByCount "10" @default.
• W2036157570 countsByYear W20361575702012 @default.
• W2036157570 countsByYear W20361575702016 @default.
• W2036157570 countsByYear W20361575702017 @default.
• W2036157570 crossrefType "journal-article" @default.
• W2036157570 hasAuthorship W2036157570A5019256598 @default.
• W2036157570 hasConcept C121332964 @default.
• W2036157570 hasConcept C151342819 @default.
• W2036157570 hasConcept C155675718 @default.
• W2036157570 hasConcept C181830111 @default.
• W2036157570 hasConcept C2524010 @default.
• W2036157570 hasConcept C2779430453 @default.
• W2036157570 hasConcept C3379466 @default.
• W2036157570 hasConcept C33923547 @default.
• W2036157570 hasConcept C37914503 @default.
• W2036157570 hasConcept C57691317 @default.
• W2036157570 hasConcept C62520636 @default.
• W2036157570 hasConcept C74650414 @default.
• W2036157570 hasConceptScore W2036157570C121332964 @default.
• W2036157570 hasConceptScore W2036157570C151342819 @default.
• W2036157570 hasConceptScore W2036157570C155675718 @default.
• W2036157570 hasConceptScore W2036157570C181830111 @default.
• W2036157570 hasConceptScore W2036157570C2524010 @default.
• W2036157570 hasConceptScore W2036157570C2779430453 @default.
• W2036157570 hasConceptScore W2036157570C3379466 @default.
• W2036157570 hasConceptScore W2036157570C33923547 @default.
• W2036157570 hasConceptScore W2036157570C37914503 @default.
• W2036157570 hasConceptScore W2036157570C57691317 @default.
• W2036157570 hasConceptScore W2036157570C62520636 @default.
• W2036157570 hasConceptScore W2036157570C74650414 @default.
• W2036157570 hasLocation W20361575701 @default.
• W2036157570 hasOpenAccess W2036157570 @default.
• W2036157570 hasPrimaryLocation W20361575701 @default.
• W2036157570 hasRelatedWork W158434167 @default.
• W2036157570 hasRelatedWork W1615345627 @default.
• W2036157570 hasRelatedWork W1641846756 @default.
• W2036157570 hasRelatedWork W1653511655 @default.
• W2036157570 hasRelatedWork W1984197722 @default.
• W2036157570 hasRelatedWork W1996932869 @default.
• W2036157570 hasRelatedWork W1998331608 @default.
• W2036157570 hasRelatedWork W2004171841 @default.
• W2036157570 hasRelatedWork W2009814748 @default.
• W2036157570 hasRelatedWork W2053318111 @default.
• W2036157570 hasRelatedWork W2056402307 @default.
• W2036157570 hasRelatedWork W2057810848 @default.
• W2036157570 hasRelatedWork W2076856893 @default.
• W2036157570 hasRelatedWork W2085394931 @default.
• W2036157570 hasRelatedWork W2091442414 @default.
• W2036157570 hasRelatedWork W2128753749 @default.
• W2036157570 hasRelatedWork W2952435767 @default.
• W2036157570 hasRelatedWork W2963164380 @default.
• W2036157570 hasRelatedWork W3122916119 @default.
• W2036157570 hasRelatedWork W342308737 @default.
• W2036157570 isParatext "false" @default.
• W2036157570 isRetracted "false" @default.
• W2036157570 magId "2036157570" @default.
• W2036157570 workType "article" @default.