dc.contributorUniversidade Estadual Paulista (UNESP)
dc.creatorBerkovits, Nathan
dc.date2014-05-27T11:30:03Z
dc.date2016-10-25T18:51:47Z
dc.date2014-05-27T11:30:03Z
dc.date2016-10-25T18:51:47Z
dc.date2013-07-26
dc.date.accessioned2017-04-06T02:32:35Z
dc.date.available2017-04-06T02:32:35Z
dc.identifierJournal of High Energy Physics, v. 2013, n. 6, 2013.
dc.identifier1126-6708
dc.identifier1029-8479
dc.identifierhttp://hdl.handle.net/11449/76052
dc.identifierhttp://acervodigital.unesp.br/handle/11449/76052
dc.identifier10.1007/JHEP06(2013)091
dc.identifierWOS:000321381800037
dc.identifier2-s2.0-84880443375.pdf
dc.identifier2-s2.0-84880443375
dc.identifierhttp://dx.doi.org/10.1007/JHEP06(2013)091
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/896765
dc.descriptionAfter 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.languageeng
dc.relationJournal of High Energy Physics
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.subjectSuperstrings and Heterotic Strings
dc.subjectTopological Strings
dc.titleDynamical twisting and the b ghost in the pure spinor formalism
dc.typeOtro


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