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Related papers: Duality and $O(d,d)$ Symmetries in String Theory

200 papers

The simplest possible noncommutative harmonic oscillator in two dimensions is used to quantize the free closed bosonic string in two flat dimensions. The partition function is not deformed by the introduction of noncommutativity, if we…

High Energy Physics - Theory · Physics 2014-11-18 Agapitos Hatzinikitas , Ioannis Smyrnakis

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

This is a very brief survey of some results in the geometry of string duality delivered at a lecture given at ICM 1998, Berlin. String Duality is the statement that one kind of string theory compactified on one space is equivalent in some…

Algebraic Geometry · Mathematics 2007-05-23 Paul S. Aspinwall

We discuss the duality symmetries of Type II string effective actions in nine, ten and eleven dimensions. As a by-product we give a covariant action underlying the ten--dimensional Type IIB supergravity theory. We apply duality symmetries…

High Energy Physics - Theory · Physics 2009-10-28 Eric Bergshoeff

The T-duality transformations between open and closed superstrings in different D-manifolds are generalized to curved backgrounds with commuting isometries. We address some global aspects like the occurrence of orientifold boundaries in…

High Energy Physics - Theory · Physics 2009-10-30 E. Alvarez , J. L. F. Barbon , J. Borlaf

In this paper, our focus is on exploring the gauge-invariant basis for bosonic couplings within the framework of heterotic string theories, specifically examining 3-, 5-, and 7-derivative terms. We thoroughly analyze the invariance of these…

High Energy Physics - Theory · Physics 2024-08-06 Mohammad R. Garousi

A two dimensional string effective action is obtained by dimensionally reducing the bosonic part of the ten dimensional heterotic string effective action. It is shown that this effective action, with a few restrictions on some backgrounds…

High Energy Physics - Theory · Physics 2015-06-26 Jnanadeva Maharana

I review the covariant quantization of the critical $N{=}2$ fermionic string with and without a global ${\bf Z}_2$ twist. The BRST analysis yields massless bosonic and fermionic vertex operators in various ghost and picture number sectors,…

High Energy Physics - Theory · Physics 2007-05-23 Olaf Lechtenfeld

The tree-level string effective action reduced from $D$ to $D-d$ dimensions possesses a continuous $O(d,d)$ symmetry, closely related to T-duality. A necessary condition for a higher derivative correction to preserve this symmetry is that…

High Energy Physics - Theory · Physics 2024-11-26 Linus Wulff

In this paper we consider the previously proposed generalised space-time and investigate the structure of the field theory upon which it is based. In particular, we derive a SO(D,D) formulation of the bosonic string as a non-linear…

High Energy Physics - Theory · Physics 2014-11-21 Peter West

We describe some of the novel 6d quantum field theories which have been discovered in studies of string duality. The role these theories (and their 4d descendants) may play in alleviating the vacuum degeneracy problem in string theory is…

High Energy Physics - Theory · Physics 2007-05-23 Shamit Kachru

The low-energy limit of string theory contains additional gravitational degrees of freedom, a skew-symmetric tensor $B$-field and a scalar dilaton, that are not present in general relativity. Together with the metric, these three fields are…

High Energy Physics - Theory · Physics 2025-03-21 Stephen Angus , Shinji Mukohyama

String theory requires two kinds of loop expansion: classical $(\alpha')$ worldsheet loops with expansion parameter $<T>$ where $T$ is a modulus field, and quantum $(\hbar)$ spacetime loops with expansion parameter $<S>$ where $S$ is the…

High Energy Physics - Theory · Physics 2008-02-03 M. J. Duff

Duality symmetries in M--theory and string theory are reviewed, with particular emphasis on the way in which string winding modes and brane wrapping modes can lead to new spatial dimensions. Brane world-volumes wrapping around Lorentzian…

High Energy Physics - Theory · Physics 2007-05-23 C. M. Hull

Upon treating the whole closed-string massless NS-NS sector as stringy graviton fields, Double Field Theory may evolve into `Stringy Gravity'. In terms of an $\mathbf{O}(D,D)$ covariant differential geometry beyond Riemann, we present the…

High Energy Physics - Theory · Physics 2019-10-02 Jeong-Hyuck Park

We reformulate bosonic boundary string field theory in terms of boundary state. In our formulation, we can formally perform the integration of target space equations of motion for arbitrary field configurations without assuming decoupling…

High Energy Physics - Theory · Physics 2010-10-27 Shunsuke Teraguchi

We present a pair of symmetric formulations of the matter sector of the stationary effective action of heterotic string theory that arises after the toroidal compactification of d dimensions. The first formulation is written in terms of a…

High Energy Physics - Theory · Physics 2010-11-19 Nandinii Barbosa-Cendejas , Alfredo Herrera-Aguilar

A universal symmetric truncation of the bosonic string Hilbert space yields all known closed fermionic string theories in ten dimensions, their D-branes and their open descendants. We highlight the crucial role played by group theory and…

High Energy Physics - Theory · Physics 2010-04-28 Auttakit Chattaraputi , Francois Englert , Laurent Houart , Anne Taormina

The symmetries of the tree level string effective action are discussed. An appropriate effective action is constructed starting from the manifestly SL(2,R) invarint form of string effective action introduced by Schwarz and Sen. The…

High Energy Physics - Theory · Physics 2009-10-30 J. Maharana , H. Singh

After simultaneous compactification of spacetime and worldvolume on $K3$, the $D=10$ heterotic fivebrane with gauge group $SO(32)$ behaves like a $D=6$ heterotic string with gauge group $SO(28) \times SU(2)$, but with Kac--Moody levels…

High Energy Physics - Theory · Physics 2009-10-28 M. J. Duff , R. Minasian