Abstract

In this article we offer the interpretation of the fermionic T-duality of the type II superstring theory in double space. We generalize the idea of double space doubling the fermionic sector of the superspace. In such doubled space fermionic T-duality is represented as permutation of the fermionic coordinates θα and θ¯α with the corresponding fermionic T-dual ones, ϑα and ϑ¯α, respectively. Demanding that T-dual transformation law has the same form as initial one, we obtain the known form of the fermionic T-dual NS–R and R–R background fields. Fermionic T-dual NS–NS background fields are obtained under some assumptions. We conclude that only symmetric part of R–R field strength and symmetric part of its fermionic T-dual contribute to the fermionic T-duality transformation of dilaton field and analyze the dilaton field in fermionic double space. As a model we use the ghost free action of type II superstring in pure spinor formulation in approximation of constant background fields up to the quadratic terms.

Highlights

  • Two theories T-dual to one another can be viewed as being physically identical [1, 2]

  • In this article we offer the interpretation of the fermionic T-duality of the type II superstring theory in double space

  • 2.1 Action and supergravity constraints. In this manuscript we use the action of type II superstring theory in pure spinor formulation [24] up to the quadratic terms with constant background fields

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Summary

Introduction

Two theories T-dual to one another can be viewed as being physically identical [1, 2]. In Refs.[14, 15] we doubled all bosonic coordinates and showed that such theory contained the initial and all corresponding T-dual theories. Introducing double space T-duality ceases to be transformation which connects two physically equivalent theories but it becomes symmetry transformation in extended space with respect to permutation group. We proved this in the bosonic string case both for constant and for weakly curved background with linear dependence on coordinates. In the first step of our approach to the formulation of M-theory (unification of types II theories) we must include T-dualization along fermionic variables (πα and πα in particular case).

A B exchanges θα and θα with their
Type II superstring and fermionic T-duality
Action and supergravity constraints
Fixing the chiral gauge invariance
Fermionic T-duality
Fermionic T-dualization in fermionic double space
Transformation laws in fermionic double space
Double action
Dilaton field in double fermionic space
Concluding remarks
A Gamma matrices
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