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A simplified pure spinor superstring $b$ ghost in a curved heterotic background was constructed recently. The $b$ ghost is a composite operator and it is not holomorphic. However, it satisfies $\bar\partial b = [ Q , \Omega ]$, where $Q$ is…

High Energy Physics - Theory · Physics 2016-05-04 Thiago Fleury

The construction of the ghost number zero and one vertex operators for the 11D pure spinor superparticle will be revisited. In this sense, an alternative way of defining the ghost number one vertex operator will be given after introducing a…

High Energy Physics - Theory · Physics 2022-12-29 Max Guillen

We provide an alternative compact expression for the 11D pure spinor b-ghost by introducing a new set of negative ghost number operators made out of non-minimal pure spinor variables. Using the algebraic properties satisfied by these…

High Energy Physics - Theory · Physics 2023-04-05 Max Guillen

Since the b ghost in the pure spinor formalism is a composite operator depending on non-minimal variables, it is not trivial to impose the Siegel gauge condition b_0 V=0 on BRST-invariant vertex operators. Using the antifield vertex…

High Energy Physics - Theory · Physics 2009-08-03 Yuri Aisaka , Nathan Berkovits

In this work, some aspects of the ambitwistor pure spinor string are investigated. The $b$ ghost is presented and its main properties are derived in a simple way, very similar to the usual pure spinor $b$ ghost construction. The heterotic…

High Energy Physics - Theory · Physics 2016-05-27 Renann Lipinski Jusinskas

In the pure spinor formalism for the superstring, the b-ghost is a composite operator satisfying {Q,b}=T where Q is the pure spinor BRST operator and T is the holomorphic stress tensor. The b-ghost is holomorphic in a flat target-space…

High Energy Physics - Theory · Physics 2015-06-17 Ilya Bakhmatov , Nathan Berkovits

In this work, the DDF-like approach to the pure spinor cohomology is extended to the next ghost number level, the so called antifields. In a direct (supersymmetric) parallel to the bosonic string, some properties of the ghost number two…

High Energy Physics - Theory · Physics 2015-12-22 Renann Lipinski Jusinskas

In this work we give an explicit construction for the vertex operators of massless states in the pure spinor superstring in a plane wave background. The construction is based on the observation that the full action can be divided in two…

High Energy Physics - Theory · Physics 2018-10-19 Osvaldo Chandia , Brenno Carlini Vallilo

The $b$ ghost, or $b$ operator, used for fixing Siegel gauge in the pure spinor superfield formalism, is a composite operator of negative ghost number, satisfying $\{q,b\}=\square$, where $q$ is the pure spinor differential (BRST operator).…

High Energy Physics - Theory · Physics 2023-01-02 Martin Cederwall

We show that the BRST cohomology of the massless sector of the Type IIB superstring on AdS5xS5 can be described as the relative cohomology of an infinite-dimensional Lie superalgebra. We explain how the vertex operators of ghost number 1,…

High Energy Physics - Theory · Physics 2013-08-26 Andrei Mikhailov

We construct the unintegrated vertex operator at the first mass level of the open superstring from the OPE of massless vertices. Using BRST cohomology manipulations, the tree amplitude of two massless and one massive state is rewritten in…

High Energy Physics - Theory · Physics 2025-03-06 Sitender Pratap Kashyap , Carlos R. Mafra , Mritunjay Verma , Luis Ypanaqué

We study the cohomology of the massless BRST complex of the Type IIB pure spinor superstring in flat space. In particular, we find that the cohomology at the ghost number three is nontrivial and transforms in the same representation of the…

High Energy Physics - Theory · Physics 2015-10-27 Andrei Mikhailov

We study the zero mode cohomology of the sum of two pure spinors. The knowledge of this cohomology allows us to better understand the structure of the massless vertex operator of the Type IIB pure spinor superstring.

High Energy Physics - Theory · Physics 2013-01-16 Andrei Mikhailov , Renjun Xu

The $D=11$ pure spinor superparticle has been shown to describe linearized $D=11$ supergravity in a manifestly covariant way. A number of authors have proposed that its correlation functions be used to compute amplitudes. The use of the…

High Energy Physics - Theory · Physics 2019-10-02 Nathan Berkovits , Eduardo Casali , Max Guillen , Lionel Mason

The 11D pure spinor worldline has been proved to successfully describe the physical states of 11D supergravity in a manifestly super-Poincar\'e covariant fashion. Within this framework, the computation of scattering amplitudes requires the…

High Energy Physics - Theory · Physics 2026-01-08 Max Guillen , Marcelo dos Santos , Eggon Viana

Vertex operators in string theory come in two varieties: integrated and unintegrated. Understanding both types is important for the calculation of the string theory amplitudes. The relation between them is a descent procedure typically…

High Energy Physics - Theory · Physics 2015-06-16 Osvaldo Chandia , Andrei Mikhailov , Brenno C. Vallilo

This paper considers the Free Differential Algebra and rheonomic parametrization of type IIA Supergravity, extended to include the BRS differential and the ghosts. We consider not only the ghosts lambda's of supersymmetry but also the…

High Energy Physics - Theory · Physics 2014-11-20 Mario Tonin

Recently Berkovits has constructed a picture raised, compound field $b_B$ which is used to compute higher loop amplitudes in the pure spinor approach of superstrings. On the other hand, in the twisted and gauge fixed, superembedding…

High Energy Physics - Theory · Physics 2010-04-05 Ichiro Oda , Mario Tonin

The ghost for world-sheet reparametrization invariance is not a fundamental field in the pure spinor formalism. It is written as a combination of pure spinor variables which have conformal dimension two and such that it commutes with the…

High Energy Physics - Theory · Physics 2011-04-28 Osvaldo Chandia

We study the the properties of a BRST ghost degree of freedom complementary to a two-state spinor. We show that the ghost may be regarded as a unit carrier of negative entropy. We construct an irreducible representation of the su(2) Lie…

High Energy Physics - Theory · Physics 2007-05-23 Andre van Tonder
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