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The conjectured equivalence of the heterotic string to a $K_3$ compactified type IIA superstring is combined with the conjectured equivalence of the latter to a compactified 11-dimensional supermembrane to derive a string membrane duality…

High Energy Physics - Theory · Physics 2010-11-01 P. K. Townsend

The (q_1,q_2) SL(2,Z) string bound states of type IIB superstring theory admit two inequivalent (T-dual) representations in eleven dimensions in terms of a fundamental 2-brane. In both cases, the spectrum of membrane oscillations can be…

High Energy Physics - Theory · Physics 2009-10-30 J. G. Russo

In a recent paper Townsend suggested to associate to the D=11 solitonic membrane of N=1 supergravity a certain thickness, and then to identify this membrane with the fundamental supermembrane. By integrating out the 8 transverse dimensions…

High Energy Physics - Theory · Physics 2015-06-26 F. Aldabe , A. L. Larsen

We propose a method for constructing super-brane actions where every background tensor potential corresponds to a world-volume field strength. The procedure provides a natural coupling to the background and automatically displays the…

High Energy Physics - Theory · Physics 2009-10-30 Martin Cederwall , Anders Westerberg

We show that the supermembrane theory compactified on a torus is invariant under T-duality. There are two different topological sectors of the compactified supermembrane (M2) classified according to a vanishing or nonvanishing second…

High Energy Physics - Theory · Physics 2016-11-23 M. P. Garcia del Moral , J. M. Pena , A. Restuccia

Certain limits of the duality between M-theory on ${T^5/Z_2}$ and IIB on K3 are analyzed in Matrix theory. The correspondence between M-theory five-branes and ALE backgrounds is realized as three dimensional mirror symmetry. Non-critical…

High Energy Physics - Theory · Physics 2010-11-19 Duiliu-Emanuel Diaconescu , Jaume Gomis

In this note I review the role played by dualities in the Supermembrane Theory compactified on a torus. Supermembrane theory realize S, T, so U-duality, as exact symmetries of the theory. There are two well defined sectors: with and without…

High Energy Physics - Theory · Physics 2012-11-28 M. P. Garcia del Moral

We present a class of orthogonal membrane configurations which preserve 1/4 of the full type IIA supersymmetry. These membrane configurations carry additional F-string charges. We further analyze the D1-D3 configuration after applying T-…

High Energy Physics - Theory · Physics 2009-11-07 Anindya Biswas , Kamal Lochan Panigrahi

Effective world-brane actions for solitons of ten-dimensional type IIA and IIB superstring theory are derived using the formulation of solitons as Dirichlet branes. The one-brane actions are used to recover predictions of SL(2,Z)…

High Energy Physics - Theory · Physics 2009-10-30 Christof Schmidhuber

We examine the extent to which the action for the membrane of M-theory (the eleven-dimensional construct which underlies and unifies all of the known string theories) simplifies in the so-called Open Membrane (OM) limit, a limit which lies…

High Energy Physics - Theory · Physics 2009-11-10 J. Antonio Garcia , Alberto Guijosa , J. David Vergara

Through direct examination of the effect of the OM limit on the M2-brane worldvolume action, we derive a membrane action for OM theory, and more generally, for the eleven-dimensional M-theoretic construct known as Galilean or Wrapped…

High Energy Physics - Theory · Physics 2009-11-07 J. Antonio Garcia , Alberto Guijosa , J. David Vergara

It is proved that a basic superembedding equation for the 2-dimensional worldsheet superspace $\S^{(2|8+8)}$ embedded into D=10 type IIB superspace $M^{(10|16+16)}$ provides a universal, S-duality invariant description of a fundamental…

High Energy Physics - Theory · Physics 2008-11-26 Igor Bandos

Dual super Dp-brane actions are constructed by carrying out a duality transformation of the world-volume U(1) gauge field. The resulting world-volume actions, which contain a (p - 2)-form gauge field, are shown to have the expected…

High Energy Physics - Theory · Physics 2009-10-30 Mina Aganagic , Jaemo Park , Costin Popescu , John H. Schwarz

We outline a formulation of membrane dynamics in D=8 which is fully covariant under the U-duality group SL(2,Z) x SL(3,Z), and encodes all interactions to fields in the eight-dimensional supergravity, which is constructed through…

High Energy Physics - Theory · Physics 2008-11-26 Viktor Bengtsson , Martin Cederwall , Henric Larsson , Bengt E. W. Nilsson

Just as string T-duality originates from transforming field equations into Bianchi identities on the string worldsheet, so it has been suggested that M-theory U-dualities originate from transforming field equations into Bianchi identities…

High Energy Physics - Theory · Physics 2015-12-09 M. J. Duff , J. X. Lu , R. Percacci , C. N. Pope , H. Samtleben , E. Sezgin

We realize the string/$(D-5)$-brane duality on the action level between the $T^{10-D}$-compactified heterotic string effective action and the $(D-5)$- brane effective action in $D$ dimensions by managing a Lagrange multiplier field. A dual…

High Energy Physics - Theory · Physics 2009-10-30 Shijong Ryang

We use compatibility of D-brane action with linear T-duality, S-duality and with S-matrix elements as guiding principles to find all world volume couplings of one massless closed and two open strings at order $\alpha'^2$ in type II…

High Energy Physics - Theory · Physics 2015-11-25 Ali Jalali , Mohammad R. Garousi

The problem with the U-duality transformation of membrane on $T^{n}$ is recently addressed in [arXiv:1509.02915 [hep-th]]. We will consider the U-duality transformation rule of membrane on $T^{n}\times R$. It turns out that winding modes on…

High Energy Physics - Theory · Physics 2016-10-17 Shan Hu , Tianjun Li

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 show how the $T$--duality between $D$--branes is realized (i) on $p$--brane solutions $(p=0,\cdots ,9)$ of IIA/IIB supergravity and (ii) on the $D$--brane actions ($p=0,\cdots ,3)$ that act as source terms for the $p$--brane solutions.…

High Energy Physics - Theory · Physics 2009-10-30 E. Bergshoeff , M. de Roo
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