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Related papers: On the Pure Spinor Heterotic Superstring $b$ Ghost

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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, 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

Using the RNS-like fermionic vector variables introduced in arXiv:1305.0693, the pure spinor $b$ ghost in a curved heterotic superstring background is easily constructed. This construction simplifies and completes the $b$ ghost construction…

High Energy Physics - Theory · Physics 2015-06-19 Nathan Berkovits , Osvaldo Chandia

A $b$-ghost was constructed for the $D=11$ non-minimal pure spinor superparticle by requiring that $\{Q , b\} = T$ where $Q = \Lambda^{\alpha}D_{\alpha} + R^{\alpha}\bar{W}_{\alpha}$ is the usual non-minimal pure spinor BRST operator. As…

High Energy Physics - Theory · Physics 2018-01-30 Nathan Berkovits , Max Guillen

We study the non-minimal pure spinor string in a curved background. We find that the minimal BRST invariance implies the existence of a non-trivial stress-energy tensor for the minimal and non-minimal variables in the heterotic curved…

High Energy Physics - Theory · Physics 2015-06-18 Osvaldo Chandia

The OPE between the composite $b$ ghost and the unintegrated vertex operator for massless states of the pure spinor superstring is computed and shown to reproduce the structure of the bosonic string result. The vanishing of the double pole…

High Energy Physics - Theory · Physics 2021-03-31 Osvaldo Chandia , Brenno Carlini Vallilo

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

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

In this work, a particular BRST-exact class of deformations of the b ghost in the non-minimal pure spinor formalism is investigated and the impact of this construction in the $\mathcal{N}=2$ $\hat{c}=3$ topological string algebra is…

High Energy Physics - Theory · Physics 2013-07-24 Renann Lipinski Jusinskas

We present the Y-formalism for the non-minimal pure spinor quantization of superstrings. In the framework of this formalism we compute, at the quantum level, the explicit form of the compound operators involved in the construction of the…

High Energy Physics - Theory · Physics 2008-11-26 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

Recently, the superstring was covariantly quantized using the BRST-like operator $Q = \oint \lambda^\alpha d_\alpha$ where $\lambda^\alpha$ is a pure spinor and $d_\alpha$ are the fermionic Green-Schwarz constraints. By performing a field…

High Energy Physics - Theory · Physics 2009-11-07 Nathan Berkovits

In the pure spinor formalism for the superstring, the b antighost is necessary for multiloop amplitude computations and is a composite operator constructed to satisfy {Q,b}=T where Q is the BRST operator and T is the holomorphic…

High Energy Physics - Theory · Physics 2015-03-17 Nathan Berkovits , Luca Mazzucato

The pure spinor superstring in a type II curved background is considered. In order to define reparametrization ghosts, non-minimal pure spinor variables have to be present in the formalism. The BRST transformations of the non-minimal…

High Energy Physics - Theory · Physics 2019-10-30 Osvaldo Chandia

Starting with a classical action whose matter variables are a d=10 spacetime vector $x^m$ and a pure spinor $\lambda^\alpha$, the pure spinor formalism for the superstring is obtained by gauge-fixing the twistor-like constraint $\partial…

High Energy Physics - Theory · Physics 2015-05-28 Nathan Berkovits

The classical pure spinor version of the heterotic superstring in a supergravity and super Yang-Mills background is considered. We obtain the BRST transformations of the world-sheet fields. They are consistent with the constraints obtained…

High Energy Physics - Theory · Physics 2009-11-11 Osvaldo Chandia

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

We construct a covariant quantum superstring, extending Berkovits' approach by introducing new ghosts to relax the pure spinor constraints. The central charge of the underlying Kac-Moody algebra, which would lead to an anomaly in the BRST…

High Energy Physics - Theory · Physics 2009-11-07 P. A. Grassi , G. Policastro , M. Porrati , P. van Nieuwenhuizen

We perform a Hamiltonian analysis of the classical type IIB superstring on AdS(5) x S(5) in the pure spinor approach. Taking the spatial components of the left-invariant (super)currents and the pure spinor ghosts as canonical variables, we…

High Energy Physics - Theory · Physics 2009-11-11 M. Bianchi , J. Kluson

It has recently been shown that the ten-dimensional superstring can be quantized using the BRST operator $Q=\oint\lambda^\alpha d_\alpha$ where $\lambda^\alpha$ is a pure spinor satisfying $\lambda \gamma^m \lambda=0$ and $d_\alpha$ is the…

High Energy Physics - Theory · Physics 2015-06-26 Nathan Berkovits , Paul Howe
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