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

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We construct the Neveu-Schwarz sector of heterotic string field theory using the large Hilbert space of the superghosts and the multi-string products of bosonic closed string field theory. No picture-changing operators are required as in…

High Energy Physics - Theory · Physics 2009-11-10 Yuji Okawa , Barton Zwiebach

We study the compactification of the pure spinor superstring down to four dimensions. We find that the compactified string is described by a conformal invariant system for both the four dimensional and for the compact six dimensional…

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

Massless spinning particle and tensionless string models on $AdS_d$ background in the projective-space realization are proposed as constrained Hamiltonian systems. Various forms of particle and string Lagrangians are derived and classical…

High Energy Physics - Theory · Physics 2023-03-29 D. V. Uvarov

Let G be a compact, semi-simple Lie group and H a maximal rank reductive subgroup. The irreducible representations of G can be constructed as spaces of harmonic spinors with respect to a Dirac operator on the homogeneous space G/H twisted…

Differential Geometry · Mathematics 2007-05-23 Gregory D. Landweber

We compute the BRST cohomology of the holomorphic part of the N=2 string at arbitrary ghost and picture number. We confirm the expectation that the relative cohomology at non-zero momentum consists of a single massless state in each…

High Energy Physics - Theory · Physics 2009-10-30 Klaus Junemann , Olaf Lechtenfeld

It is shown that for suitable roots of unity, there exist finite--dimensional unitary representations of $U_q(so(2,3))$ corresponding to all classical one-particle representations with (half)integer spin, with the correct low-energy limit.…

q-alg · Mathematics 2007-05-23 Harold Steinacker

For a finite group $G$, we define a ghost ring and a mark homomorphism for the double Burnside ring of left-free $(G,G)$-bisets. In analogy to the case of the Burnside ring $B(G)$, the ghost ring has a much simpler ring structure, and after…

Group Theory · Mathematics 2012-03-27 Robert Boltje , Susanne Danz

The grading Becchi-Rouet-Stora-Tyutin (BRST) method gives a way to construct the integer $W_{2,s}$ strings, where the BRST charge is written as $Q_B=Q_0+Q_1$. Using this method, we reconstruct the nilpotent BRST charges $Q_{0}$ for the…

High Energy Physics - Theory · Physics 2009-01-26 Shao-Wen Wei , Yu-Xiao Liu , Li-Jie Zhang , Ji-Rong Ren

We propose a new BRST operator for the B-twist of $N=2$ Landau-Ginzburg (LG) models. It solves the problem of the fractional ghost numbers of Vafa's old BRST operator and shows how the model is obtained by gauge fixing a zero action. An…

High Energy Physics - Theory · Physics 2009-10-28 F. De Jonghe , P. Termonia , W. Troost , S. Vandoren

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 quantum version of pure D=4 N=2 supergravity can be topologically twisted, to yield a formulation of topological gravity in four dimensions. The topological BRST complex is just a rearrangement of the old BRST complex,…

High Energy Physics - Theory · Physics 2014-11-18 Damiano Anselmi , Pietro Fre

We examine the BRS cohomology of chiral matter in $N=1$, $D=4$ supersymmetry to determine a general form of composite superfield operators which can suffer from supersymmetry anomalies. Composite superfield operators $\Y_{(a,b)}$ are…

High Energy Physics - Theory · Physics 2008-11-26 J. A. Dixon , R. Minasian , J. Rahmfeld

We construct the integrated vertex operator for the first massive states of open superstrings with $(mass)^2=1/\alpha'$ in the pure spinor formalism of the superstring theory. This vertex operator is expressed in terms of the ten…

High Energy Physics - Theory · Physics 2018-12-04 Subhroneel Chakrabarti , Sitender Pratap Kashyap , Mritunjay Verma

We consider Polyakov theory of Bosonic strings in conformal gauge which are used to study conformal anomaly. However it exhibits ghost number anomaly. We show how this anomaly can be avoided by connecting this theory to that of in…

High Energy Physics - Theory · Physics 2019-05-22 Vipul Kumar Pandey , Bhabani Prasad Mandal

We present a general algorithm which permits to construct solutions in string cosmology for heterotic and type-IIB superstrings in four dimensions. Using a chain of transformations applied in sequence: conformal, T-duality and SL(2,R)…

High Energy Physics - Theory · Physics 2009-10-30 A. Feinstein , Ruth Lazkoz , M. A. Vazquez-Mozo

The Becchi-Rouet-Stora-Tyutin (BRST) ghost field is a key element in constructing Witten's cubic open string field theory. However, to date, the ghost sector of the string field theory has not received a great deal of attention. In this…

High Energy Physics - Theory · Physics 2022-08-10 Taejin Lee

We describe a new realization of supersymmetry, called scalar supersymmetry, acting in spaces of differential forms (bi-spinors), where transformation parameters are Lorentz scalars instead of spinors. The realization is related but is not…

High Energy Physics - Phenomenology · Physics 2015-06-11 Alex Jourjine

In these lecture notes presented at the 2015 Villa de Leyva Summer School, we give an introduction to superstring theory. We begin by studying the particle and superparticle in order to get a better understanding on the superstring side.…

High Energy Physics - Theory · Physics 2017-11-29 Nathan Berkovits , Humberto Gomez

In the Type II superstring the 4-point function for massless NS-NS bosons at one-loop is well known [1][14]. The overall constant factor in this amplitude is very important because it needs to satisfy the unitarity and S-duality conditions…

High Energy Physics - Theory · Physics 2010-02-04 Humberto Gomez
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