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Related papers: T-Duality as a Duality of Loop Group Bundles

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We consider the closed string moving in the weakly curved background and its totally T-dualized background. Using T-duality transformation laws, we find the structure of the Poisson brackets in the T-dual space corresponding to the…

High Energy Physics - Theory · Physics 2014-02-04 Ljubica Davidovic , Bojan Nikolic , Branislav Sazdovic

The role of double space is essential in new interpretation of T-duality and consequently in an attempt to construct M-theory. The case of open string is missing in such approach because until now there have been no appropriate formulation…

High Energy Physics - Theory · Physics 2018-02-08 B. Sazdović

We state and prove a general result establishing that T-duality simplifies the bulk-boundary correspondence, in the sense of converting it to a simple geometric restriction map. This settles in the affirmative several earlier conjectures of…

High Energy Physics - Theory · Physics 2018-04-16 Keith C. Hannabuss , Varghese Mathai , Guo Chuan Thiang

Different compactifications of six-dimensional string theory on $M_4 \times T^2$ are considered. Particular attention is given to the roles of the reduced modes as the $S$ and $T$ fields. It is shown that there is a discrete group of…

High Energy Physics - Theory · Physics 2009-10-28 Nemanja Kaloper

We investigate the effect of T-duality on noncommutativity. Starting with open strings ending on a D2-brane wrapped on a $T^2$ torus in the presence of a Kalb Ramond field, we consider Buscher transformations on the coordinates and…

High Energy Physics - Theory · Physics 2010-05-28 C. A. Ballon Bayona , Nelson R. F. Braga , Rafael D'Andrea

String theory appears to admit a group of discrete field transformations -- called $S$ dualities -- as exact non-perturbative quantum symmetries. Mathematically, they are rather analogous to the better-known $T$ duality symmetries, which…

High Energy Physics - Theory · Physics 2011-04-15 John H. Schwarz

Under the assumption of axial symmetry we introduce a map from dilatonic gravity to a string-like action. This map allows one to introduce, in a rather simple way, the equivalent of string theory T-duality in dilatonic gravity. Here we…

High Energy Physics - Theory · Physics 2014-11-18 Pablo M. Llatas

The duality properties of perturbative string characters associated with the transverse space-time rotations are studied. T duality is achieved by suitably integrating over the total momentum, contrary to earlier discussions. The O(8)…

High Energy Physics - Theory · Physics 2009-10-30 Eugene Cremmer , Jean-Loup Gervais

We discuss various dual {\it pairs} of $M$-theory compactifications. Each pair consists of a compactification in which the two-brane plays the crucial role in relation to a string theory and a compactification in which the five-brane takes…

High Energy Physics - Theory · Physics 2007-05-23 B. S. Acharya

A rich pattern of gauge symmetries is found in the moduli space of heterotic string toroidal compactifications, at fixed points of the T-duality transformations. We analyze this pattern for generic tori, and scrutinize in full detail…

High Energy Physics - Theory · Physics 2018-10-17 Bernardo Fraiman , Mariana Graña , Carmen A. Núñez

We propose a manifestly U-duality invariant modular form for the D^4 R^4 interaction in type IIB string theory compactified on T^2. It receives perturbative contributions upto two loops, and non-perturbative contributions from D-instantons…

High Energy Physics - Theory · Physics 2008-11-26 Anirban Basu

We consider several orbifold compactifications of M-theory and their corresponding type II duals in two space-time dimensions. In particular, we show that while the orbifold compactification of M-theory on $T^9/J_9$ is dual to the orbifold…

High Energy Physics - Theory · Physics 2010-11-19 Shibaji Roy

String geometry theory is one of the candidates of non-perturbative formulation of string theory. In this paper, we have shown that dimensionally reduced string geometry theories have what we call T-symmetry. In case of the dimensional…

High Energy Physics - Theory · Physics 2025-03-04 Matsuo Sato , Taiki Tohshima

We provide the backreaction of the T-fold doubly T-dual to a background with NSNS three-form flux on a three-torus. We extend the backreacted T-fold to include cases with a flux localized in one out of three directions. We analyze the…

High Energy Physics - Theory · Physics 2009-01-17 Waldemar Schulgin , Jan Troost

We investigate the orbifold limits of string theory compactifications with geometric and non-geometric fluxes. Exploiting the connection between internal fluxes and structure constants of the gaugings in the reduced supergravity theory, we…

High Energy Physics - Theory · Physics 2015-06-16 Cezar Condeescu , Ioannis Florakis , Costas Kounnas , Dieter Lust

We study the topology of T-duality for pairs of U(1)-bundles and three-dimensional integral cohomology classes over orbispaces. In particular, our results apply to U(1)-spaces with finite isotropy. We generalize the theory developed in our…

Geometric Topology · Mathematics 2010-05-10 Ulrich Bunke , Thomas Schick

Target space duality (T duality), which interchanges Kaluza--Klein and winding-mode excitations of the compactified heterotic string, is realized as a symmetry of a world-sheet action. Axion-dilaton duality (S duality), a conjectured…

High Energy Physics - Theory · Physics 2009-09-15 John H. Schwarz , Ashoke Sen

We use a T-duality invariant action to investigate the behaviour of a string in non-geometric backgrounds, where there is a non-trivial global $O(D,D)$ patching or monodromy. This action leads to a set of Dirac brackets describing the…

High Energy Physics - Theory · Physics 2015-06-30 Chris D. A. Blair

In discussions of the T-duality between the two heterotic string theories, the duality is actually implemented through the "common" SO(16) x SO(16) subgroup of "SO(32)" and E_8 x E_8. In fact, however, a global investigation shows that no…

High Energy Physics - Theory · Physics 2008-11-26 Brett McInnes

The data required for heterotic string theory with gauge group G, which for anomaly cancellation reasons must either be E8 x E8 or Spin(32)/Z2, consist of the following: a ten-dimensional space-time X and a principal G-bundle P. The fields…

Differential Geometry · Mathematics 2007-05-23 Adrian Clingher