Explaining the pure spinor formalism for the superstring
Contribuinte(s) |
Universidade Estadual Paulista (UNESP) |
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Data(s) |
30/09/2013
20/05/2014
30/09/2013
20/05/2014
01/01/2008
|
Resumo |
After adding a pair of non-minimal fields and performing a similarity transformation, the BRST operator in the pure spinor formalism is expressed as a conventional-looking BRST operator involving the Virasoro constraint and (b, c) ghosts, together with 12 fermionic constraints. This BRST operator can be obtained by gauge-fixing the Green-Schwarz superstring where the 8 first-class and 8 second-class Green-Schwarz constraints are combined into 12 first-class constraints. Alternatively, the pure spinor BRST operator can be obtained from the RNS formalism by twisting the ten spin-half RNS fermions into five spin-one and five spin-zero fermions, and using the SO(10)/U(5) pure spinor variables to parameterize the different ways of twisting. GSO(-) vertex operators in the pure spinor formalism are constructed using spin fields and picture-changing operators in a manner analogous to Ramond vertex operators in the RNS formalism. |
Formato |
27 |
Identificador |
http://dx.doi.org/10.1088/1126-6708/2008/01/065 Journal of High Energy Physics. Trieste: Int School Advanced Studies, n. 1, p. 27, 2008. 1126-6708 http://hdl.handle.net/11449/24340 10.1088/1126-6708/2008/01/065 WOS:000252983400012 |
Idioma(s) |
eng |
Publicador |
Int School Advanced Studies |
Relação |
Journal of High Energy Physics |
Direitos |
closedAccess |
Palavras-Chave | #superstrings and heterotic strings #topological strings |
Tipo |
info:eu-repo/semantics/article |