Abstract

The pure spinor formalism for the superstring was recently obtained by gauge-fixing a purely bosonic classical action involving a twistor-like constraint ∂x m (γ m λ) α = 0 where λ α is a d=10 pure spinor. This twistor-like constraint replaces the usual Virasoro constraint ∂x m ∂x m = 0, and the Green-Schwarz fermionic spacetime spinor variables θα arise as Faddeev-Popov ghosts for this constraint. In this paper, the purely bosonic classical action is simplified by replacing the classical d=10 pure spinor λ α with a d=10 projective pure spinor. The pure spinor and Green-Schwarz formalisms for the superparticle and superstring are then obtained as different gauge-fixings of this purely bosonic classical action, and the Green-Schwarz kappa symmetry is directly related to the pure spinor BRST symmetry. Since a d=10 projective pure spinor parameterizes $$ \frac{\mathrm{SO}(10)}{\mathrm{U}(5)} $$ , this action can be interpreted as a standard ĉ = 5 topological action where one integrates over the $$ \frac{\mathrm{SO}(10)}{\mathrm{U}(5)} $$ choice of complex structure. Finally, a purely bosonic action for the d=11 supermembrane is proposed which reduces upon double-dimensional reduction to the purely bosonic action for the d=10 Type IIA superstring.

Highlights

  • The purely bosonic classical action is simplified by replacing the classical d=10 pure spinor λα with a d=10 projective pure spinor

  • The pure spinor and Green-Schwarz formalisms for the superparticle and superstring are obtained as different gauge-fixings of this purely bosonic classical action, and the Green-Schwarz kappa symmetry is directly related to the pure spinor BRST symmetry

  • Different gauge-fixings of this purely bosonic classical action will produce either the pure spinor or GS formalisms, and the GS kappa symmetry will be related in a simple manner to the pure spinor BRST symmetry

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Summary

Twistor-like superparticle

Before discussing the d=10 superstring, it will be useful to first discuss the d=10 superparticle and show how its twistor-like action can be interpreted as an action for a topological particle in which one integrates over the choices of complex structure. Where χ = paLa is the gauge-fixing fermion, Q = θaPa is the BRST operator which generates the transformation of (2.2), and Ma ≡ Qpa is the Nakanishi-Lautrup field whose auxiliary equation of motion is Ma = Pa. Physical states in the BRST cohomology are shown to be anti-holomorphic functions V = f (xa) which satisfy PaV = 0. Physical states in the BRST cohomology are shown to be anti-holomorphic functions V = f (xa) which satisfy PaV = 0 This topological theory is not SO(10) invariant, one can write the action of (2.1) using ten-dimensional notation as. It will be shown that if one makes the theory SO(10) invariant by integrating over the choice of complex structure, the theory is no longer topological and describes the d=10 super-Maxwell theory coming from quantizing the d=10 superparticle

Worldline action
Pure spinor superparticle
Green-Schwarz superparticle
Worldsheet action
Pure spinor superstring
Green-Schwarz superstring
Twistor-like supermembrane
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