dc.contributor | Universidade Estadual Paulista (UNESP) | |
dc.creator | Berkovits, Nathan | |
dc.date | 2014-05-27T11:30:03Z | |
dc.date | 2016-10-25T18:51:47Z | |
dc.date | 2014-05-27T11:30:03Z | |
dc.date | 2016-10-25T18:51:47Z | |
dc.date | 2013-07-26 | |
dc.date.accessioned | 2017-04-06T02:32:35Z | |
dc.date.available | 2017-04-06T02:32:35Z | |
dc.identifier | Journal of High Energy Physics, v. 2013, n. 6, 2013. | |
dc.identifier | 1126-6708 | |
dc.identifier | 1029-8479 | |
dc.identifier | http://hdl.handle.net/11449/76052 | |
dc.identifier | http://acervodigital.unesp.br/handle/11449/76052 | |
dc.identifier | 10.1007/JHEP06(2013)091 | |
dc.identifier | WOS:000321381800037 | |
dc.identifier | 2-s2.0-84880443375.pdf | |
dc.identifier | 2-s2.0-84880443375 | |
dc.identifier | http://dx.doi.org/10.1007/JHEP06(2013)091 | |
dc.identifier.uri | http://repositorioslatinoamericanos.uchile.cl/handle/2250/896765 | |
dc.description | After adding an RNS-like fermionic vector ψ m to the pure spinor formalism, the non-minimal b ghost takes a simple form similar to the pure spinor BRST operator. The N=2 superconformal field theory generated by the b ghost and the BRST current can be interpreted as a dynamical twisting of the RNS formalism where the choice of which spin 1/2 ψ m variables are twisted into spin 0 and spin 1 variables is determined by the pure spinor variables that parameterize the coset SO(10)/U(5). © 2013 SISSA, Trieste, Italy. | |
dc.language | eng | |
dc.relation | Journal of High Energy Physics | |
dc.rights | info:eu-repo/semantics/closedAccess | |
dc.subject | Superstrings and Heterotic Strings | |
dc.subject | Topological Strings | |
dc.title | Dynamical twisting and the b ghost in the pure spinor formalism | |
dc.type | Otro | |