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Related papers: S-duality of S-matrix

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We propose a method to obtain a manifestly supersymmetric action functional for interacting brane systems. It is based on the induced map of the worldvolume of low-dimensional branes into the worldvolume of the space-time filling brane…

High Energy Physics - Theory · Physics 2011-07-19 Igor Bandos , Wolfgang Kummer

We study a non-standard decoupling limit of the D1/D5-brane system, which interpolates between the near-horizon geometry of the D1/D5 background and the near-horizon limit of the pure D5-brane geometry. The S-dual description of this…

High Energy Physics - Theory · Physics 2010-02-03 Dan Israel , Costas Kounnas , Marios P Petropoulos

The Wess-Zumino coupling on D-branes in string theory is known to receive higher derivative corrections which couple the Ramond-Ramond potential to terms involving the square of the spacetime curvature tensor. Consistency with T-duality…

High Energy Physics - Theory · Physics 2010-09-16 Katrin Becker , Guangyu Guo , Daniel Robbins

We carry out a systematic study of 4d $\mathcal{N} = 2$ preserving S-folds of F-theory 7-branes and the worldvolume theories on D3-branes probing them. They consist of two infinite series of theories, which we denote following the original…

High Energy Physics - Theory · Physics 2020-10-20 Simone Giacomelli , Mario Martone , Yuji Tachikawa , Gabi Zafrir

We consider the S-duality transformation of gauge invariant operators and states in $\mathcal{N}$ $=4$ SYM theory. The transformation is realized through an operator $ S $ which is the $ SL(2,Z) $ canonical transformation in loop space with…

High Energy Physics - Theory · Physics 2019-05-23 Shan Hu

The effective field equations of motion for a mixed theory of open and closed (2,2) world-sheet supersymmetric critical strings are shown to be integrable in the case of an abelian gauge group. The Born-Infeld-type effective action in 2+2…

High Energy Physics - Theory · Physics 2007-05-23 Sergei V. Ketov

Non-perturbative features of the derivative expansion of the effective action of a single D3-brane are obtained by considering scattering amplitudes of open and closed strings. This motivates expressions for the coupling constant dependence…

High Energy Physics - Theory · Physics 2014-11-18 Michael B. Green , Michael Gutperle

We construct the full effective action including DBI and WZ terms for solitonic 5-branes covariant under T-duality. The result is a completion of results known in the literature to a full T-duality covariant expression. The covariant WZ…

High Energy Physics - Theory · Physics 2022-11-03 Edvard T. Musaev , Jeffrey P. Molina

We derive level-rank duality in pure Chern-Simons gauge theories from a non-supersymmetric Seiberg duality by using a non-supersymmetric brane configuration in type IIB string theory. The brane configuration consists of fivebranes, N D3…

High Energy Physics - Theory · Physics 2015-06-22 Adi Armoni , Edwin Ireson

We study the action of S-duality on half-BPS Wilson loop operators in 5d $\mathcal{N}=1$ theories. The duality is the statement that different massive deformations of a single 5d SCFT are described by different gauge theories, or…

High Energy Physics - Theory · Physics 2018-11-14 Benjamin Assel , Antonio Sciarappa

We present a Matrix theory action and Matrix configurations for spherical 4-branes. The dimension of the representations is given by N=2(2j+1) (j=1/2,1,3/2,...). The algebra which defines these configurations is not invariant under SO(5)…

High Energy Physics - Theory · Physics 2009-11-10 Ryuichi Nakayama , Yusuke Shimono

We study the noncommutative superspace of arbitrary dimensions in a systematic way. Superfield theories on a noncommutative superspace can be formulated in two folds, through the star product formalism and in terms of the supermatrices. We…

High Energy Physics - Theory · Physics 2016-09-06 Jeong-Hyuck Park

Duality transformations involving compactifications on timelike as well as spacelike circles link M-theory, the 10+1-dimensional strong coupling limit of IIA string theory, to other 11-dimensional theories in signatures 9+2 and 6+5 and to…

High Energy Physics - Theory · Physics 2009-10-31 Chris M. Hull , Ramzi R. Khuri

We present a supersymmetric and $\kappa$-symmetric D-string action on $AdS_5 \times S^5$ in supercoset construction. As in the previous work of the super D-string action in the flat background, the super D-string action on $AdS_5 \times…

High Energy Physics - Theory · Physics 2009-10-31 Ichiro Oda

We consider non-critical heterotic strings compactified on $S^1$. For full rank theories, they are related to odd self-dual lattices and are structurally of the same form as the critical non-supersymmetric theories. For dimensions up to 14…

High Energy Physics - Theory · Physics 2024-12-31 Héctor Parra De Freitas

A naive dimensional reduction of the $N=1, D=10$ supergravity theory that naturally arises in five-brane models is used to determine the r\^ole of two fields which are basic ingredients of string models: the dilaton and, among the moduli,…

High Energy Physics - Theory · Physics 2009-10-22 P. Binetruy

String duality suggests a fascinating juxtoposition of world-volume and target-space dynamics. This is particularly apparent in the $D$-brane description of stringy solitons that forms a major focus of this article (which is {\it not}…

High Energy Physics - Theory · Physics 2009-10-30 Michael B. Green

We describe a simple method for generating new string solutions for which the brane worldvolume is a curved space. As a starting point we use solutions with NS-NS charges combined with 2-d CFT's representing different parts of space-time.…

High Energy Physics - Theory · Physics 2009-09-17 G. Papadopoulos , J. Russo , A. A. Tseytlin

We examine duality transformations of supersymmetric and $\kappa$-symmetric Dp-brane actions in a general type II supergravity background where in particular the dilaton and the axion are supposed to not be zero or a constant but a general…

High Energy Physics - Theory · Physics 2015-06-26 Tadahiko Kimura , Ichiro Oda

We show that the open membrane action on $T^3\times S^1/Z^2$ is equivalent to the closed membrane action on K3. The main difference between the two actions is that one generates the KK modes in the worldvolume action which is the strong…

High Energy Physics - Theory · Physics 2009-10-30 F. Aldabe