Abstract

We consider the closed string propagating in the weakly curved background which consists of constant metric and Kalb-Ramond field with infinitesimally small coordinate dependent part. We propose the procedure for constructing the T-dual theory, performing T-duality transformations along coordinates on which the Kalb-Ramond field depends. The obtained theory is defined in the non-geometric double space, described by the Lagrange multiplier $y_\mu$ and its $T$-dual $\tilde{y}_\mu$. We apply the proposed T-duality procedure to the T-dual theory and obtain the initial one. We discuss the standard relations between T-dual theories that the equations of motion and momenta modes of one theory are the Bianchi identities and the winding modes of the other.

Highlights

  • Duality symmetry was for the first time described in the context of toroidal compactification in [1,2,3]

  • We show that the T -dual of the T -dual is the original theory

  • We will investigate the closed bosonic string moving in the weakly curved background, with the goal to find the generalization of the Buscher construction of the T -dual theory

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Summary

Introduction

Duality symmetry was for the first time described in the context of toroidal compactification in [1,2,3] (thoroughly explained in [4,5]). To preserve the physical meaning of the original theory, one requires that the new fields vαμ do not carry the additional degrees of freedom. To obtain a theory physically equivalent to the original one, all degrees of freedom carried by the gauge fields vαμ should be eliminated. The first one is that the target space of the T dual theory in the weakly curved background turns out to be a non-geometrical one [15,16,17,18,19,20,21,22,23,24,25,26,27,28] This is a doubled space with two coordinates, one of them being the Lagrange multiplier as in the case of the flat background. We show that the T -dual of the T -dual is the original theory

Bosonic string in the weakly curved background
Generalized Buscher construction
Gauging shift symmetry
From gauge-fixed action to the original and T -dual action
Eliminating the Lagrange multiplier
Eliminating the gauge fields
The T -dual of the T -dual theory
The features of the T -duality
T -dualities in terms of the conserved currents and charges
Conclusion

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