dc.contributorUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2014-05-27T11:20:20Z
dc.date.accessioned2022-10-05T17:44:42Z
dc.date.available2014-05-27T11:20:20Z
dc.date.available2022-10-05T17:44:42Z
dc.date.created2014-05-27T11:20:20Z
dc.date.issued2001-12-01
dc.identifierJournal of High Energy Physics, v. 5, n. 11, 2001.
dc.identifier1029-8479
dc.identifier1126-6708
dc.identifierhttp://hdl.handle.net/11449/66653
dc.identifier10.1088/1126-6708/2001/11/047
dc.identifierWOS:000174174000047
dc.identifier2-s2.0-33744777815
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/3916389
dc.description.abstractAlthough the equations of motion for the Neveu-Schwarz (NS) and Ramond (R) sectors of open superstring field theory can be covariantly expressed in terms of one NS and one R string field, picture-changing problems prevent the construction of an action involving these two string fields. However, a consistent action can be constructed by dividing the NS and R states into three string fields which are real, chiral and antichiral. The open superstring field theory action includes a WZW-like term for the real field and holomorphic Chern-Simons-like terms for the chiral and antichiral fields. Different versions of the action can be constructed with either manifest d = 8 Lorentz covariance or manifest TV = 1 d = 4 super-Poincaré covariance. The lack of a manifestly d = 10 Lorentz covariant action is related to the self-dual five-form in the type-IIB R-R sector.
dc.languageeng
dc.relationJournal of High Energy Physics
dc.relation5.541
dc.relation1,227
dc.relation1,227
dc.rightsAcesso restrito
dc.sourceScopus
dc.subjectBrst symmetry
dc.subjectSuperstrings and heterotic strings
dc.titleThe Ramond sector of open superstring field theory
dc.typeArtigo


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