scholarly journals Theta expansion of first massive vertex operator in pure spinor

2018 ◽  
Vol 2018 (1) ◽  
Author(s):  
Subhroneel Chakrabarti ◽  
Sitender Pratap Kashyap ◽  
Mritunjay Verma
Keyword(s):  
Vertex Operator ◽  
Pure Spinor

scholarly journals Relating the b ghost and the vertex operators of the pure spinor superstring

2021 ◽  
Vol 2021 (3) ◽  
Author(s):  
Osvaldo Chandia ◽  
Brenno Carlini Vallilo
Keyword(s):  
Vertex Operator ◽  
Bosonic String ◽  
Vertex Operators ◽  
Pure Spinor ◽  
Double Pole ◽  
Lorenz Gauge

Abstract 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 double pole vanishes in the Lorenz gauge and the single pole is shown to be equal to the corresponding integrated vertex operator.

scholarly journals A construction of integrated vertex operator in the pure spinor sigma-model in AdS 5 × S 5

2013 ◽  
Vol 2013 (11) ◽  
Author(s):  
Osvaldo Chandia ◽  
Andrei Mikhailov ◽  
Brenno C. Vallilo
Keyword(s):  
Vertex Operator ◽  
Sigma Model ◽  
Pure Spinor

scholarly journals Integrated massive vertex operator in pure spinor formalism

2018 ◽  
Vol 2018 (10) ◽  
Author(s):  
Subhroneel Chakrabarti ◽  
Sitender Pratap Kashyap ◽  
Mritunjay Verma
Keyword(s):  
Vertex Operator ◽  
Pure Spinor ◽  
Spinor Formalism ◽  
Pure Spinor Formalism

scholarly journals COVARIANT QUANTIZATION OF THE SUPERSTRING

2001 ◽  
Vol 16 (05) ◽  
pp. 801-811 ◽  
Author(s):  
NATHAN BERKOVITS
Keyword(s):  
Vertex Operator ◽  
Vertex Operators ◽  
Pure Spinor ◽  
Covariant Quantization ◽  
Brst Operator ◽  
First Time

After reviewing the Green-Schwarz superstring using the approach of Siegel, the superstring is covariantly quantized by constructing a BRST operator from the fermionic constraints and a bosonic pure spinor ghost variable. Physical massless vertex operators are constructed and, for the first time, N-point tree amplitudes are computed in a manifestly ten-dimensional super-Poincaré covariant manner. Quantization can be generalized to curved supergravity backgrounds and the vertex operator for fluctuations around AdS5×S5 is explicitly constructed.

scholarly journals Notes on the 11D pure spinor wordline vertex operators

2020 ◽  
Vol 2020 (8) ◽  
Author(s):  
Max Guillen
Keyword(s):  
Vertex Operator ◽  
Ghost Number ◽  
Vertex Operators ◽  
Pure Spinor ◽  
Full Form

Abstract 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 ghost number -2 operator made out of physical operators defined on the 11D non-minimal pure spinor superspace. This procedure will make explicit and transparent the relation between the ghost number three and one vertex operators. In addition, using a non-Lorentz covariant b-ghost, ghost number zero and two vertex operators satisfying standard descent equations will be presented in full form.

scholarly journals (NON)TRIVIALITY OF PURE SPINORS AND EXACT PURE SPINOR–RNS MAP

2009 ◽  
Vol 24 (14) ◽  
pp. 2677-2687 ◽  
Author(s):  
DIMITRI POLYAKOV
Keyword(s):  
Hilbert Space ◽  
String Theory ◽  
Vertex Operator ◽  
Similarity Transformation ◽  
Pure Spinor ◽  
Brst Operator ◽  
Variable Λ ◽  
Brst Cohomology ◽  
Spinor Formalism ◽  
Pure Spinor Formalism

All the BRST-invariant operators in pure spinor formalism in d = 10 can be represented as BRST commutators, such as [Formula: see text] where λ+ is the U(5) component of the pure spinor transforming as [Formula: see text]. Therefore, in order to secure nontriviality of BRST cohomology in pure spinor string theory, one has to introduce "small Hilbert space" and "small operator algebra" for pure spinors, analogous to those existing in RNS formalism. As any invariant vertex operator in RNS string theory can also represented as a commutator V = {Q brst , LV} where L = -4c∂ξξe-2ϕ, we show that mapping [Formula: see text] to L leads to identification of the pure spinor variable λα in terms of RNS variables without any additional nonminimal fields. We construct the RNS operator satisfying all the properties of λα and show that the pure spinor BRST operator ∮λαdα is mapped (up to similarity transformation) to the BRST operator of RNS theory under such a construction.

scholarly journals W algebras, cosets and VOAs for 4d $$ \mathcal{N} $$ = 2 SCFTs from M5 branes

2021 ◽  
Vol 2021 (4) ◽  
Author(s):  
Dan Xie ◽  
Wenbin Yan
Keyword(s):  
Vertex Operator ◽  
Operator Algebras ◽  
Nilpotent Orbit ◽  
Vertex Operator Algebras ◽  
Flavor Symmetries ◽  
Conformal Embedding

Abstract We identify vertex operator algebras (VOAs) of a class of Argyres-Douglas (AD) matters with two types of non-abelian flavor symmetries. They are the W algebras defined using nilpotent orbit with partition [qm, 1s]. Gauging above AD matters, we can find VOAs for more general $$ \mathcal{N} $$ N = 2 SCFTs engineered from 6d (2, 0) theories. For example, the VOA for general (AN − 1, Ak − 1) theory is found as the coset of a collection of above W algebras. Various new interesting properties of 2d VOAs such as level-rank duality, conformal embedding, collapsing levels, coset constructions for known VOAs can be derived from 4d theory.

Z2k-code vertex operator algebras

2021 ◽  
Vol 573 ◽  
pp. 451-475
Author(s):  
Hiromichi Yamada ◽  
Hiroshi Yamauchi
Keyword(s):  
Vertex Operator ◽  
Operator Algebras ◽  
Vertex Operator Algebras
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