dc.contributor | Universidade Estadual Paulista (Unesp) | |
dc.date.accessioned | 2014-05-27T06:35:49Z | |
dc.date.available | 2014-05-27T06:35:49Z | |
dc.date.created | 2014-05-27T06:35:49Z | |
dc.date.issued | 1989-12-01 | |
dc.identifier | Journal of Mathematical Physics, v. 30, n. 8, p. 1866-1870, 1989. | |
dc.identifier | 0022-2488 | |
dc.identifier | http://hdl.handle.net/11449/130456 | |
dc.identifier | 10.1063/1.528273 | |
dc.identifier | WOS:A1989AH02700026 | |
dc.identifier | 2-s2.0-3043002427 | |
dc.identifier | 2-s2.0-3043002427.pdf | |
dc.description.abstract | The basic field equations of a field theory are not always derivable from a Lagrangian. Lagrangian theories are perturbatively coherent, in the sense that they have well-defined vertices. Non-Lagrangian theories may be coherent or not. Coherent theories are, in principle, quantizable by perturbative methods. The general condition for a theory to have well-defined vertices is given. © 1989 American Institute of Physics. | |
dc.language | eng | |
dc.publisher | American Institute of Physics (AIP) | |
dc.relation | Journal of Mathematical Physics | |
dc.relation | 1.165 | |
dc.relation | 0,644 | |
dc.rights | Acesso restrito | |
dc.source | Scopus | |
dc.title | Perturbative coherence in field theory | |
dc.type | Artículos de revistas | |