Abstract

In the paper [1] we showed that in double space, where all initial coordinates $x^\mu$ are doubled $x^\mu \to y_\mu$, the T-duality transformations can be performed by exchanging places of some coordinates $x^a$ and corresponding dual coordinates $y_a$. Here we generalize this result to the case of weakly curved background where in addition to the extended coordinate we will also transform extended argument of background fields with the same operator $\hat {\cal T}^a$. So, in the weakly curved background T-duality leads to the physically equivalent theory and complete set of T-duality transformations form the same group as in the flat background. Therefore, the double space represent all T-dual theories in unified manner.

Highlights

  • The T-duality is one of the stringy properties, because it has no analogy in particle physics

  • We proved that T-duality transformations in the double space (2.22), for weakly curved background, unites equations of motion and Bianchi identities

  • We introduced the extended 2D dimensional space with the coordinates ZM =, which beside initial D dimensional space-time coordinates xμ contains the corresponding T-dual coordinates yμ

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Summary

Introduction

The T-duality is one of the stringy properties, because it has no analogy in particle physics. ◦ Td−1, can be realized by exchanging their places, xa ↔ ya It has been proven for constant background fields, the metric Gμν and the Kalb-Ramond field Bμν , when Buscher’s approach can be applied. This interpretation shows that T-duality leads to the equivalent theory, because replacement of coordinates does not change the physics. We will show that this expression is enough to find background fields from all nodes of the chain (1.1) and T-duality transformations between arbitrary nodes In such a way, as well as in the flat background, we unify all T-dual theories of the chain (1.1).

T-duality in the weakly curved background
Sigma-model approach to T-duality in the weakly curved background
T-duality transformations in the weakly curved background
Equations of motions as consistency condition of T-duality relations
T-duality as coordinates permutations in flat double space
The complete T-duality chain in the weakly curved background
Notation for arguments of background fields
Relations between arguments of background fields
T-duality transformations as coordinates permutations
The T-dualities in the double space along all coordinates
The arguments of the dual background fields
The T-dual background fields in the weakly curved background
Dilaton
Path integral in the weakly curved background
Functional measure in the weakly curved background
Dilaton in the double space
Example
Background of the initial theory
General form of T-duality transformations for Three torus
The expression for V 3 as solutions of zero order T-duality transformation
Collection of all metrics and Kalb-Ramond fields for Three torus
Conclusion
G GT G G
Block-wise expressions for weakly curved background fields
Full Text
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