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Related papers: Strong Coupling Dynamics of Branes from M-theory

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In type II string theories, we examine intersecting brane constructions containing brane-antibrane pairs suspended between 5-branes, and more general non-BPS constructions. The tree-level spectra are obtained in each case. We identify…

High Energy Physics - Theory · Physics 2009-10-31 Sunil Mukhi , Nemani V. Suryanarayana , David Tong

All the models of elementary particles and their interactions derived from String Theory involve a compact six-dimensional internal space. Its volume and shape should be fixed or stabilized, since otherwise massless scalar fields (moduli)…

High Energy Physics - Theory · Physics 2015-06-23 Noriaki Kitazawa

It is shown that many of the $p$-branes of type II string theory and $d=11$ supergravity can have boundaries on other $p$-branes. The rules for when this can and cannot occur are derived from charge conservation. For example it is found…

High Energy Physics - Theory · Physics 2009-09-17 Andrew Strominger

Negative mass brane-like objects known as orientifolds are crucial in the construction of all presently understood realistic string compactifications and I review in general the link between negative energy objects and the existence of a…

High Energy Physics - Theory · Physics 2013-03-21 Keith Copsey

String and M-theory contain a family of branes forming U-duality multiplets. In particular, standard branes with codimension higher than or equal to two, can be explicitly found as supergravity solutions. However, whether domain-wall branes…

High Energy Physics - Theory · Physics 2018-09-19 Jose J. Fernandez-Melgarejo , Tetsuji Kimura , Yuho Sakatani

We present the intersecting brane configurations consisting of NS-branes, D4-branes(and anti D4-branes) and O6-plane, of type IIA string theory corresponding to the meta-stable nonsupersymmetric vacua in four dimensional N=1 supersymmetric…

High Energy Physics - Theory · Physics 2008-11-26 Changhyun Ahn

We construct the T duals of certain type IIA brane configurations with one compact dimension (elliptic models) which contain orientifold planes. These configurations realize four-dimensional $\NN=2$ finite field theories. For elliptic…

High Energy Physics - Theory · Physics 2009-10-09 J. Park , A. M. Uranga

The type IIA nonsupersymmetric meta-stable brane configuration consisting of three NS5-branes, D4-branes and anti-D4-branes where the electric gauge theory superpotential has a quartic term for the bifundamentals besides a mass term is…

High Energy Physics - Theory · Physics 2010-03-04 Changhyun Ahn

The compactness of the closed string in the classical Type II string theory reveals the duality, whereas the compactness of the open string reveals that the end of the string is on the hypersurface which satisfies the Dirichlet boundary…

High Energy Physics - Theory · Physics 2018-02-01 Hanze Li , Maolin Bo

Synopsis: (i) how superstring theories are unified by M-theory; (ii) how superstring and supermembrane properties follow from the D=10 and D=11 supersymmetry algebras; (iii) how D=10 and D=11 supergravity theories determine the strong…

High Energy Physics - Theory · Physics 2008-02-03 P. K. Townsend

We study geometries produced by brane intersections preserving eight supercharges. Typical examples of such configurations are given by fundamental strings ending on Dp branes and we construct gravity solutions describing such…

High Energy Physics - Theory · Physics 2008-11-26 Oleg Lunin

We use the M theory approach of Witten to investigate N=1 SU($N_c$) SQCD with $N_f$ flavors. We reproduce the field theoretical results and identify in M theory the gluino condensate and the eigenvalues of the meson matrix. This approach…

High Energy Physics - Theory · Physics 2009-10-30 A. Brandhuber , N. Itzhaki , V. Kaplunovsky , J. Sonnenschein , S. Yankielowicz

We study several different kinds of bound states built from D-branes and orientifolds. These states are to atoms what branonium - the bound state of a brane and its anti-brane - is to positronium, inasmuch as they typically involve a light…

High Energy Physics - Theory · Physics 2009-08-13 C. P. Burgess , N. E. Grandi , F. Quevedo , R. Rabadan

Coupling of a membrane and a five-brane to the bosonic sector of D=11 supergravity is considered. The five--brane is a dyonic object which carries both an electric and a magnetic charge of the D=11 three-form gauge field $A^3$, and it…

High Energy Physics - Theory · Physics 2007-05-23 Dmitri Sorokin

The fact that both the D6-brane and the orientifold 6-plane have smooth, horizon-free descriptions in M-theory makes them especially useful in understanding certain aspects of brane physics. We briefly review how this connection has been…

High Energy Physics - Theory · Physics 2009-11-07 Donald Marolf

We discuss general supersymmetric brane configurations in flux backgrounds of string and M-theory and derive a necessary condition for the worldvolume theory to be supersymmetric on a given curved manifold. This condition resembles very…

High Energy Physics - Theory · Physics 2015-11-10 Hagen Triendl

Limits of a system of N Dn-branes in which the bulk and string degrees of freedom decouple to leave a `matter' theory are investigated and, for n>4, either give a free theory or require taking $N \to \infty$. The decoupled matter theory is…

High Energy Physics - Theory · Physics 2009-10-31 C. M. Hull

We give simple arguments for new non-renormalization theorems on higher derivative couplings of gauge theories to supergravity, with sixteen supersymmetries, by considerations of brane-bulk superamplitudes. This leads to some exact results…

High Energy Physics - Theory · Physics 2015-12-23 Ying-Hsuan Lin , Shu-Heng Shao , Yifan Wang , Xi Yin

String compactifications with D-branes may exhibit regular magnetic monopole solutions, whose presence does not rely on broken non-abelian gauge symmetry. These stringy monopoles exist on interesting metastable brane configurations, such as…

High Energy Physics - Theory · Physics 2007-05-23 Herman Verlinde

We study string theory propagating on R^6 times K3 by constructing orientifolds of Type IIB string theory compactified on the T^4/Z_N orbifold limits of the K3 surface. This generalises the Z_2 case studied previously. The orientifold…

High Energy Physics - Theory · Physics 2014-11-18 Eric G. Gimon , Clifford V. Johnson
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