dc.contributorUniversidade Estadual Paulista (UNESP)
dc.creatorSuzuki, A. T.
dc.creatorSchmidt, A. G. M.
dc.date2014-05-27T11:19:47Z
dc.date2016-10-25T18:15:55Z
dc.date2014-05-27T11:19:47Z
dc.date2016-10-25T18:15:55Z
dc.date1999-12-01
dc.date.accessioned2017-04-06T00:55:02Z
dc.date.available2017-04-06T00:55:02Z
dc.identifierEuropean Physical Journal C, v. 10, n. 2, p. 357-362, 1999.
dc.identifier1434-6044
dc.identifierhttp://hdl.handle.net/11449/65898
dc.identifierhttp://acervodigital.unesp.br/handle/11449/65898
dc.identifier10.1007/s100529900074
dc.identifierWOS:000082906900017
dc.identifier2-s2.0-0002415741
dc.identifierhttp://dx.doi.org/10.1007/s100529900074
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/887554
dc.descriptionThe negative-dimensional integration method (NDIM) is revealing itself as a very useful technique for computing massless and/or massive Feynman integrals, covariant and noncovanant alike. Up until now however, the illustrative calculations done using such method have been mostly covariant scalar integrals/without numerator factors. We show here how those integrals with tensorial structures also can be handled straightforwardly and easily. However, contrary to the absence of significant features in the usual approach, here the NDIM also allows us to come across surprising unsuspected bonuses. Toward this end, we present two alternative ways of working out the integrals and illustrate them by taking the easiest Feynman integrals in this category that emerge in the computation of a standard one-loop self-energy diagram. One of the novel and heretofore unsuspected bonuses is that there are degeneracies in the way one can express the final result for the referred Feynman integral.
dc.languageeng
dc.relationEuropean Physical Journal C
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.titleFeynman integrals with tensorial structure in the negative dimensional integration scheme
dc.typeOtro


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