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Related papers: Notes on the 11D pure spinor wordline vertex opera…

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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

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 $D=11$ 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 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

In this Thesis we study first- and second-quantized approaches describing $D=11$ supergravity using pure spinor variables. We introduce the so-called $D=11$ pure spinor superparticle through BRST cohomology arguments starting from the…

High Energy Physics - Theory · Physics 2020-06-12 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

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 construct closed string vertex operators with various ghost numbers in addition to the conventional ones, using the Faddeev-Popov procedure for the gauge fixing of the conformal Killing group, from matter primary fields. We find that…

High Energy Physics - Theory · Physics 2024-10-21 Isao Kishimoto , Mako Kouga , Shigenori Seki , Tomohiko Takahashi

We present a modification of the Berkovits superparticle. This is firstly in order to covariantly quantize the pure spinor ghosts, and secondly to covariantly calculate matrix elements of a generic operator between two states. We proceed by…

High Energy Physics - Theory · Physics 2010-02-03 Michael Chesterman

11D pure spinors have been shown to successfully describe 11D supergravity in a manifestly super-Poincar\'e covariant manner. The feasibility of its actual usage for scattering amplitude computations requires an efficient manipulation of…

High Energy Physics - Theory · Physics 2023-06-01 Maor Ben-Shahar , Max Guillen

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 $b$ 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, 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

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

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

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

By extending the six-dimensional hybrid formalism for the superstring to include $d=6$ $\mathcal{N}=1$ superspace variables along with unconstrained bosonic ghost fields, we construct a manifestly spacetime supersymmetric vertex operator…

High Energy Physics - Theory · Physics 2025-05-27 Cassiano A. Daniel

The general fluctuations, in the form of vertex operators, for the heterotic superstring in the pure spinor formalism are considered. The case of a flat background is reviewed and the case of a curved case is studied. The left-moving ghosts…

High Energy Physics - Theory · Physics 2019-03-27 Osvaldo Chandia

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

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
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