dc.contributor | Universidade Estadual Paulista (Unesp) | |
dc.date.accessioned | 2014-05-27T11:20:20Z | |
dc.date.accessioned | 2022-10-05T17:44:42Z | |
dc.date.available | 2014-05-27T11:20:20Z | |
dc.date.available | 2022-10-05T17:44:42Z | |
dc.date.created | 2014-05-27T11:20:20Z | |
dc.date.issued | 2001-12-01 | |
dc.identifier | Journal of High Energy Physics, v. 5, n. 11, 2001. | |
dc.identifier | 1029-8479 | |
dc.identifier | 1126-6708 | |
dc.identifier | http://hdl.handle.net/11449/66653 | |
dc.identifier | 10.1088/1126-6708/2001/11/047 | |
dc.identifier | WOS:000174174000047 | |
dc.identifier | 2-s2.0-33744777815 | |
dc.identifier.uri | http://repositorioslatinoamericanos.uchile.cl/handle/2250/3916389 | |
dc.description.abstract | Although 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.language | eng | |
dc.relation | Journal of High Energy Physics | |
dc.relation | 5.541 | |
dc.relation | 1,227 | |
dc.relation | 1,227 | |
dc.rights | Acesso restrito | |
dc.source | Scopus | |
dc.subject | Brst symmetry | |
dc.subject | Superstrings and heterotic strings | |
dc.title | The Ramond sector of open superstring field theory | |
dc.type | Artigo | |