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Pure Spinor Formalism for Osp(N|4) backgrounds

Pietro Fré, Pietro Antonio Grassi

TL;DR

This work develops a covariant pure spinor formulation for strings on $AdS_4$-based backgrounds by deriving pure spinor constraints from the Maurer–Cartan structure of the $OSp(\mathcal{N}|4)$ supergroups and analyzing a family of cosets $G/H$ to balance bosonic and fermionic degrees of freedom. The authors ghostify the Maurer–Cartan forms, implement BRST symmetry, and identify viable backgrounds, with $OSp(6|4)/U(3)\times SO(1,3)$ yielding the critical $AdS_4\times\mathbb{P}^3$ case in which a consistent pure spinor sigma model can be constructed and quantized. They also study other cosets, showing that only a limited set lead to consistent backgrounds and DOF matching, while a fully gauged bosonic coset removes residual pure spinor degrees of freedom. The results provide a systematic framework for manifestly supersymmetric worldsheet descriptions on $AdS_4$ backgrounds and pave the way for RR-coupling analysis, amplitudes, and possible AdS/CFT interpretations involving Chern–Simons theories.

Abstract

We start from the Maurer-Cartan (MC) equations of the Osp(N|4) superalgebras satisfied by the left-invariant super-forms realized on supercoset manifolds of the corresponding supergroups and we derive some new pure spinor constraints. They are obtained by "ghostifying" the MC forms and extending the differential d to a BRST differential. From the superalgebras G =Osp(N|4) we single out different subalgebras H contained in G associated with the different cosets G/H: each choice of H leads to a different weakening of the pure spinor constraints. In each case, the number of parameter is counted and we show that in the cases of Osp(6|4)/U(3) x SO(1,3), Osp(4|4)/SO(3) x SO(1,3) and finally Osp(4|4) U(2)} x SO(1,3) the bosonic and fermionic degrees of freedom match in order to provide a c=0 superconformal field theory. We construct both the Green-Schwarz and the pure spinor sigma model for the case Osp(6|4)/U(3)x SO(1,3) corresponding to AdS_4 x P^3. The pure spinor sigma model can be consistently quantized.

Pure Spinor Formalism for Osp(N|4) backgrounds

TL;DR

This work develops a covariant pure spinor formulation for strings on -based backgrounds by deriving pure spinor constraints from the Maurer–Cartan structure of the supergroups and analyzing a family of cosets to balance bosonic and fermionic degrees of freedom. The authors ghostify the Maurer–Cartan forms, implement BRST symmetry, and identify viable backgrounds, with yielding the critical case in which a consistent pure spinor sigma model can be constructed and quantized. They also study other cosets, showing that only a limited set lead to consistent backgrounds and DOF matching, while a fully gauged bosonic coset removes residual pure spinor degrees of freedom. The results provide a systematic framework for manifestly supersymmetric worldsheet descriptions on backgrounds and pave the way for RR-coupling analysis, amplitudes, and possible AdS/CFT interpretations involving Chern–Simons theories.

Abstract

We start from the Maurer-Cartan (MC) equations of the Osp(N|4) superalgebras satisfied by the left-invariant super-forms realized on supercoset manifolds of the corresponding supergroups and we derive some new pure spinor constraints. They are obtained by "ghostifying" the MC forms and extending the differential d to a BRST differential. From the superalgebras G =Osp(N|4) we single out different subalgebras H contained in G associated with the different cosets G/H: each choice of H leads to a different weakening of the pure spinor constraints. In each case, the number of parameter is counted and we show that in the cases of Osp(6|4)/U(3) x SO(1,3), Osp(4|4)/SO(3) x SO(1,3) and finally Osp(4|4) U(2)} x SO(1,3) the bosonic and fermionic degrees of freedom match in order to provide a c=0 superconformal field theory. We construct both the Green-Schwarz and the pure spinor sigma model for the case Osp(6|4)/U(3)x SO(1,3) corresponding to AdS_4 x P^3. The pure spinor sigma model can be consistently quantized.

Paper Structure

This paper contains 16 sections, 92 equations.