From geometry to non-geometry via T-duality
arXiv:1606.01938 · doi:10.1088/1674-1137/42/8/083106
Abstract
Reconsideration of the T-duality of the open string allows us to introduce some geometric features in non-geometric theories. First, we have found what symmetry is T-dual to the local gauge transformations. It includes transformations of background fields but does not include transformations of the coordinates. According to this we have introduced a new, up to now missing term, with additional gauge field (D denotes components with Dirichlet boundary conditions). It compensates non-fulfilment of the invariance under such transformations on the end-points of an open string, and the standard gauge field (N denotes components with Neumann boundary conditions) compensates non-fulfilment of the gauge invariance. Using a generalized procedure we will perform T-duality of vector fields linear in coordinates. We show that gauge fields and are T-dual to and respectively. We introduce the field strength of T-dual non-geometric theories as derivatives of T-dual gauge fields along both T-dual variable and its double . This definition allows us to obtain gauge transformation of non-geometric theories which leaves the T-dual field strength invariant. Therefore, we introduce some new features of non-geometric theories where field strength has both antisymmetric and symmetric parts. This allows us to define new kinds of truly non-geometric theories.
44 pages, To be published in Chinese Physics C
References in corpus (8)
- Double Field Theory
- Symmetry, Gravity and Noncommutativity
- T-duality and closed string non-commutative (doubled) geometry
- D-Branes, RR-Fields and Duality on Noncommutative Manifolds
- Sigma models for genuinely non-geometric backgrounds
- T-dualization in a curved background in absence of a global symmetry
- T-duality as coordinates permutation in double space for weakly curved background
- Open string T-duality in double space