English
Related papers

Related papers: Taming the b antighost with Ramond-Ramond flux

200 papers

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

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

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 $b$ 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

The B-RNS-GSS formalism containing both RNS and GS worldsheet variables is extended for the description of the Type II superstring in curved backgrounds. The BRST charge of the theory is expressed in terms of $N=(1,1)$ superconformal…

High Energy Physics - Theory · Physics 2023-12-19 Osvaldo Chandia , João Gomide

The pure spinor formalism for the superstring has the advantage over the more conventional Ramond-Neveu-Schwarz formalism of being manifestly spacetime supersymmetric, which simplifies the computation of multiparticle and multiloop…

High Energy Physics - Theory · Physics 2025-03-06 Nathan Berkovits , Carlos R. Mafra

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

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

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 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

The BRST operator cohomology of $N=2$ $2d$ supergravity coupled to matter is presented. Descent equations for primary superfields of the matter sector are derived. We find one copy of the cohomology at ghost number one, two independent…

High Energy Physics - Theory · Physics 2009-10-22 Amit Giveon , Martin Rocek

This paper provides a more detailed background to the results of arXiv:1004.2692 concerning properties of multi-loop amplitudes in a pure spinor formulation of field theories with maximal supersymmetry. This involves the development of a…

High Energy Physics - Theory · Physics 2011-03-07 Jonas Bjornsson

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

Although the AdS_5xS^5 worldsheet action is not quadratic, some features of the pure spinor formalism are simpler in an AdS_5xS^5 background than in a flat background. The BRST operator acts geometrically, the left and right-moving pure…

High Energy Physics - Theory · Physics 2009-09-28 Nathan Berkovits

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

We construct non-critical pure spinor superstrings in two, four and six dimensions. We find explicitly the map between the RNS variables and the pure spinor ones in the linear dilaton background. The RNS variables map onto a patch of the…

High Energy Physics - Theory · Physics 2009-11-11 Ido Adam , Pietro Antonio Grassi , Luca Mazzucato , Yaron Oz , Shimon Yankielowicz

We study the type IIB superstring in the plane-wave background with Ramond-Ramond flux and formulate it as an exact conformal field theory in operator formalism. One of the characteristic features of the superstring in a consistent…

High Energy Physics - Theory · Physics 2009-12-10 Yoichi Kazama , Naoto Yokoi

Using arguments based on BRST cohomology, the pure spinor formalism for the superstring in an AdS_5 x S^5 background is proven to be BRST invariant and conformally invariant at the quantum level to all orders in perturbation theory.…

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

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
‹ Prev 1 2 3 10 Next ›