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After reviewing the general structure of supersymmetric intersecting brane world models, we discuss the issue of stringy gauge coupling unification for a natural class of MSSM-like models.

High Energy Physics - Theory · Physics 2007-05-23 Ralph Blumenhagen

We study supersymmetric intersecting configurations of D-branes with B-field backgrounds. Noncommutative D-brane or M-brane pairs can intersect supersymmetrically over (p-1)-brane, as well as over (p-2)-brane like ordinary branes. d=10 and…

High Energy Physics - Theory · Physics 2009-10-31 Nakwoo Kim

Using the relation between D-brane charges and K-theory, we study non-BPS D-branes and their behavior under T-duality. We point out that in general compactifications, D-brane charges are classified by relative K-theory groups. T-duality is…

High Energy Physics - Theory · Physics 2009-10-31 Oren Bergman , Eric G. Gimon , Petr Horava

We construct intersecting D-brane configurations that encode the gauge groups and field content of dual N=4 supersymmetric gauge theories in three dimensions. The duality which exchanges the Coulomb and Higgs branches and the…

High Energy Physics - Theory · Physics 2009-09-17 Jan de Boer , Kentaro Hori , Hirosi Ooguri , Yaron Oz , Zheng Yin

The study of brane-antibrane configurations in string theory leads to the understanding of supersymmetric D$p$-branes as the bound states of higher dimensional branes. Configurations of pairs brane-antibrane do admit in a natural way their…

High Energy Physics - Theory · Physics 2009-10-31 Hugo Garcia-Compean

We study the theory of NS five-branes in string theory with a smooth non-trivial transverse space. We show that in the limit that the bulk physics decouples, these theories become equivalent to theories with a flat and non-compact…

High Energy Physics - Theory · Physics 2007-05-23 Nathan Seiberg , Savdeep Sethi

Starting with the non-BPS D0-brane solution of IIB/$(-1)^{F_L}I_4$ constructed recently by Eyras and Panda we construct via T-duality the non-BPS D2-brane and D1-brane solutions of IIB/$(-1)^{F_L}I_4$ and IIA/$(-1)^{F_L}I_4$ predicted by…

High Energy Physics - Theory · Physics 2009-10-31 Yolanda Lozano

Five-branes lead in four dimensions to massless N=1 supermultiplets if M-theory is compactified on S1/Z2 x (a Calabi-Yau threefold). One of them describes the modulus associated with the position of the five-brane along the circle S1. We…

High Energy Physics - Theory · Physics 2009-10-31 Jean-Pierre Derendinger , Roger Sauser

We study a ${{\IZ}}_2$ orbifold of Type 0B string theory by reflection of six of the coordinates (this theory may also be thought of as a ${{\IZ}}_4$ orbifold of Type IIB string theory by a rotation by $\pi$ in three independent planes). We…

High Energy Physics - Theory · Physics 2009-10-31 Igor R. Klebanov , Nikita A. Nekrasov , Samson L. Shatashvili

The moduli space of vacua for the confining phase of N=1 $Sp(N_c)$ supersymmetric gauge theories in four dimensions is studied by M theory fivebrane. We construct M theory fivebrane configuration corresponding to the perturbation of…

High Energy Physics - Theory · Physics 2009-10-30 Changhyun Ahn

We systematically analyze supersymmetric D-branes in the type IIB plane wave background using Green-Schwarz superstring theory. We find several new supersymmetric oblique and curved D-branes. The supersymmetries preserved by various…

High Energy Physics - Theory · Physics 2009-11-10 Kyung-Seok Cha , Bum-Hoon Lee , Hyun Seok Yang

By using O(7,7) transformations, to deform D6-branes, we obtain half-supersymmetric bound state solutions of type IIA supergravity, containing D6, D4, D2, D0, F1-branes and waves. We lift the solutions to M-theory which gives…

High Energy Physics - Theory · Physics 2009-11-07 Henric Larsson

We find novel bound states of NS5, D6 and D8-branes in massive Type IIA string theory. As the NS gauge transformations can change the Chern class of the RR field these configurations should be thought of as nonlocal objects called gerbes.…

High Energy Physics - Theory · Physics 2010-02-03 Jussi Kalkkinen

We determine the low energy description of N=2 supersymmetric SU(k) product group theories with bifundamental and fundamental matter based on M-theory fivebrane configurations. The dependence on moduli and scales of the coefficients in the…

High Energy Physics - Theory · Physics 2009-09-15 J. Erlich , A. Naqvi , L. Randall

We discuss the consistency conditions of a novel orientifold projection of type IIB string theory on C^2/Z_N singularities, in which one mods out by the combined action of world-sheet parity and a geometric operation which exchanges the two…

High Energy Physics - Theory · Physics 2009-10-09 Angel M. Uranga

We derive general BPS boundary conditions in two-dimensional $\mathcal{N}=(2,2)$ supersymmetric gauge theories. We analyze the solutions of these boundary conditions, and in particular those that allow the bulk fields to have poles at the…

High Energy Physics - Theory · Physics 2021-03-19 Tadashi Okazaki , Douglas J. Smith

We investigate solutions of type II supergravity which have the product R^4 x M^6 structure with non-compact M^6 factor and which preserve at least four supersymmetries. In particular, we consider various conifolds and the N=1…

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

We complete the classification of supersymmetric configurations of two M5-branes, started by Ohta and Townsend. The novel configurations not considered before are those in which the two branes are moving relative to one another. These…

High Energy Physics - Theory · Physics 2010-02-03 BS Acharya , JM Figueroa-O'Farrill , B Spence , S Stanciu

We study the SUSY/non-SUSY duality proposed by Aganagic et al. from Type IIA string and M-theory perspectives. We find that our brane configuration generalizes the so-called $extended$ Seiberg-Witten theory on the one hand, and provides a…

High Energy Physics - Theory · Physics 2010-02-03 Kazutoshi Ohta , Ta-Sheng Tai

We extend the study of superinstantons presented in 1905.01513 to include orthosymplectic supergroup gauge theories, $B_{n_0|n_1}$, $C_n$, and $D_{n_0|n_1}$. We utilize equivariant localization to obtain the LMNS contour integral formula…

High Energy Physics - Theory · Physics 2024-01-09 Taro Kimura , Yilu Shao
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