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Orientable open string theories containing both bosons and fermions without the GSO projection are expected to have the 10 dimensional N=2(A) space-time supersymmetry in a spontaneously broken phase. We study the low-energy theorem for the…

High Energy Physics - Theory · Physics 2009-10-31 Tabito Hara , Tamiaki Yoneya

N=2 supersymmetric gauge theories in four dimensions are studied by formulating them as the quantum field theories derived from configurations of fourbranes, fivebranes, and sixbranes in Type IIA superstrings, and then reinterpreting those…

High Energy Physics - Theory · Physics 2010-04-07 Edward Witten

By turning on antisymmetric background fluxes, we study how multiple M2-branes are coupled to them. Our investigation concentrates on the gauge invariance conditions for the Myers-Chern-Simons action. Furthermore, the dimensional reduction…

High Energy Physics - Theory · Physics 2014-11-18 Miao Li , Tower Wang

We propose a deformation of ${\cal N}=4$ SYM theoery induced by nonanticommutative star product. The deformation introduces new bosonic terms which we identify with the corresponding Myers terms of a stack of D3-branes in the presence of a…

High Energy Physics - Theory · Physics 2009-11-11 Reza Abbaspur , Ali Imaanpur

The fivebrane of M theory is used in order to study the moduli space of vacua of confining phase N=1 supersymmetric gauge theories in four dimensions. The supersymmetric vacua correspond to the condensation of massless monopoles and…

High Energy Physics - Theory · Physics 2009-09-29 Jan de Boer , Yaron Oz

We study the world volume theory of D3-branes wrapping the Melvin universe supported by background NSNS B-field. In the appropriate decoupling limit, the open string dynamics is that of non-commutative guage field theory with non-constant…

High Energy Physics - Theory · Physics 2010-02-03 Akikazu Hashimoto , Keith Thomas

N=2 quiver Chern-Simons theory has lately attracted attention as the world volume theory of multiple M2 branes on a Calabi-Yau 4-fold. We study the connection between the stringy derivation of M2 brane theories and the forward algorithm…

High Energy Physics - Theory · Physics 2009-10-05 Masato Taki

We argue that there is an equivalence of M-theory on T^3 \times A_{N-1} with a four-dimensional non-supersymmetric quiver gauge theory on the Higgs branch. The quiver theory in question has gauge group SU(N)^{N_4N_6N_8} and is considered in…

High Energy Physics - Theory · Physics 2009-11-10 Ingo Kirsch , Dan Oprisa

We study metastable nonsupersymmetric configurations in type IIA string theory, obtained by suspending D4-branes and anti-D4-branes between holomorphically curved NS5's, which are related to those of hep-th/0610249 by T-duality. When the…

High Energy Physics - Theory · Physics 2008-11-26 Joseph Marsano , Kyriakos Papadodimas , Masaki Shigemori

A number of N=2 gauge theories can be realized by brane configurations in Type IIA string theory. One way of solving them involves lifting the brane configuration to M-theory. In this paper we present an alternative way of analyzing a…

High Energy Physics - Theory · Physics 2009-10-31 Anton Kapustin

We study open string amplitudes with the D3-branes in type IIB superstring theory compactified on C^2/Z_2. We introduce constant graviphoton background along the branes and calculate disk amplitudes using the NSR formalism. We take the zero…

High Energy Physics - Theory · Physics 2009-11-11 Katsushi Ito , Shin Sasaki

We construct a Z_2 orbifold projection of SU(N) gauge theories formulated in five dimensions with a compact fifth dimension. We show through a non-perturbative argument that no boundary mass term for the Higgs field, identified with some of…

High Energy Physics - Lattice · Physics 2009-11-10 Nikos Irges , Francesco Knechtli

We study N=1 four dimensional gauge theories as the world volume theory of D4-branes between NS 5-branes. We find constructions for a number of known field theory dualities involving $SU(N_c)\times SU(N_c')$ groups, coupled by matter fields…

High Energy Physics - Theory · Physics 2009-10-30 John H. Brodie , Amihay Hanany

The $\mathcal{A}$-theory takes U-duality symmetry as a guiding principle, with the SL(5) U-duality symmetry being described as the world-volume theory of a 5-brane. Furthermore, by unifying the 6-dimensional world-volume Lorentz symmetry…

High Energy Physics - Theory · Physics 2025-07-09 Machiko Hatsuda , Ondřej Hulík , William D. Linch , Warren D. Siegel , Di Wang , Yu-Ping Wang

It is known that if we compactify D0-branes on a torus with constant B-field, the resulting theory becomes SYM theory on a noncommutative dual torus. We discuss the extension to the case of a H-field background. In the case of constant…

High Energy Physics - Theory · Physics 2010-11-19 Masahiro Anazawa

We investigate the worldvolume theory that describes N coincident M2-branes ending on an M5 brane. We argue that the fields that describe the transverse spacetime coordinates take values in a non-associative algebra. We postulate a set of…

High Energy Physics - Theory · Physics 2008-11-26 Jonathan Bagger , Neil Lambert

We present a construction of non-Abelian gauge theories on the R^4 x S^1/Z_2 orbifold. We show that no divergent boundary mass term for the Higgs field, identified with some of the fifth dimensional components of the gauge field, is…

High Energy Physics - Lattice · Physics 2007-05-23 Francesco Knechtli , Burkhard Bunk , Nikos Irges

A geometric formulation of a generalization of Nambu mechanics is proposed. This formulation is carried out, wherever possible, in analogy with that of Hamiltonian systems. In this formulation, a strictly nondegenerate constant 3-form is…

chao-dyn · Physics 2008-02-03 Sagar A. Pandit , Anil D. Gangal

This thesis is devoted to derivative corrections to the effective action of D-branes, and to mirror symmetry with D-branes. Series of derivative corrections first predicted by non-commutative gauge theory are completed by couplings between…

High Energy Physics - Theory · Physics 2009-09-29 Pascal Grange

The presence of the antisymmetric background field $B_{\mu\nu}$ leads to the noncommutativity of the Dp-brane manifold, while the linear dilaton field in the form $\Phi(x)=\Phi_0+a_\mu x^\mu$, causes the appearance of the commutative…

High Energy Physics - Theory · Physics 2008-11-26 B. Nikolic , B. Sazdovic