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Related papers: Non-singlet Baryons in Less Supersymmetric Backgro…

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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 classify and construct all the smooth Kaluza-Klein reductions to ten dimensions of the M2- and M5-brane configurations which preserve some of the supersymmetry. In this way we obtain a wealth of new supersymmetric IIA backgrounds…

High Energy Physics - Theory · Physics 2008-11-26 José Figueroa-O'Farrill , Joan Simón

We write supersymmetry preserving conditions for infinite M5-branes intersecting on a (3+1)-dimensional space. In contrast to previously known solutions, these intersections are completely localized. We solve the equations for a particular…

High Energy Physics - Theory · Physics 2009-10-31 Ansar Fayyazuddin , Douglas J. Smith

We discuss consistent truncations of eleven-dimensional supergravity on a six-dimensional manifold $M$, preserving minimal $\mathcal{N}=2$ supersymmetry in five dimensions. These are based on $G_S \subseteq USp(6)$ structures for the…

High Energy Physics - Theory · Physics 2021-06-07 Davide Cassani , Gregoire Josse , Michela Petrini , Daniel Waldram

We investigate the transition between singular and non-singular geometries from the vantage point of perturbative field dynamics. In particular, we obtain the closed-form absorption probability for minimally-coupled massless scalars…

High Energy Physics - Theory · Physics 2010-02-03 J. F. Vazquez-Poritz

The existence of supersymmetric D0-branes at an arbitrary distance from a flux 5-brane is proven. The physical picture in type IIA is consistent with the Kaluza-Klein reduction origin of the flux 5-brane. An analysis of the fluctuations…

High Energy Physics - Theory · Physics 2015-06-26 Joan Simón

We study the effect of adding lower dimensional brane charges to the 't Hooft monopole, di-baryon and baryon vertex configurations in AdS_4 x CP^3. We show that these configurations capture the background fluxes in a way that depends on the…

High Energy Physics - Theory · Physics 2015-05-27 Norberto Gutierrez , Yolanda Lozano , Diego Rodriguez-Gomez

We consider Einstein gravity coupled to an n-form field strength in D dimensions. Such a theory cannot be supersymmetrized in general, we nevertheless propose a pseudo-Killing spinor equation and show that the AdS X Sphere vacua have the…

High Energy Physics - Theory · Physics 2011-07-05 H. Lu , Zhao-Long Wang

We perform a complete integration of the Einstein-dilaton-antisymmetric form action describing black p-branes in arbitrary dimensions assuming the transverse space to be homogeneous and possessing spherical, toroidal or hyperbolic topology.…

High Energy Physics - Theory · Physics 2009-11-10 Dmitri V. Gal'tsov , Jose P. S. Lemos , Gerard Clement

We find non-critical string backgrounds in five and eight dimensions, holographically related to four-dimensional conformal field theories with N=0 and N=1 supersymmetries. In the five-dimensional case we find an AdS_5 background metric for…

High Energy Physics - Theory · Physics 2010-12-03 F. Bigazzi , R. Casero , A. L. Cotrone , E. Kiritsis , A. Paredes

We discuss marginal deformations of warped AdS$_3\times$S$^2$ solutions preserving small $\mathcal{N}=(0,4)$ supersymmetry in massive IIA and eleven-dimensional supergravity and obtain a whole family of new solutions. We characterise these…

High Energy Physics - Theory · Physics 2021-02-12 Salomon Zacarias

A non-critical holographic QCD model constructed in the six dimensional Anti-de-Sitter ($AdS_6$) supergravity background is employed to study a the baryon. It is shown that the size of the baryon is of order one with respect to the…

High Energy Physics - Theory · Physics 2013-09-04 M. R. Pahlavani , J. Sadeghi , R. Morad

We study a new embedding solutions of D5 brane in an asymptotic AdS${}_5\times S^5$ space-time, which is dual to a confining $SU(N_c)$ gauge theory. The D5 brane is wrapped on $S^5$ as in the case of the vertex of holographic baryon.…

High Energy Physics - Theory · Physics 2015-03-13 Kazuo Ghoroku , Akihiro Nakamura , Tomoki Taminato , Fumihiko Toyoda

This work focuses on an unexplored aspect of non-symmetric geometry where {\it only} the off-diagonal metric components along the extra dimension, in a 5-dimensional spacetime, are non-symmetric. We show that the energy densities of the…

General Relativity and Quantum Cosmology · Physics 2013-07-03 Suman Ghosh , S. Shankaranarayanan

We consider generalisations of the recently proposed supersymmetry breaking deformation of the 5d rank-1 $E_1$ superconformal field theory to higher rank. We generalise the arguments to theories which admit a mass deformation leading to…

High Energy Physics - Theory · Physics 2024-01-31 Mohammad Akhond , Masazumi Honda , Francesco Mignosa

I present a mini-review on the physics of heavy flavour baryons where I concentrate on the HQET description of their exclusive decay modes. In particular I discuss the structure of current-induced bottom baryon to charm baryon transitions,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jürgen G. Körner

In the mapping from four-dimensional gauge theories to string theory in $AdS$ space, many features of gauge theory can be described by branes wrapped in different ways on $\S^5$, $\RP^5$, or subspaces thereof. These include a baryon vertex…

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

We consider general aspects of the realization of R and non-R flavor symmetries in the AdS_5 x H_5 dual of 4d N=1 superconformal field theories. We find a general prescription for computing the charges under these symmetries for baryonic…

High Energy Physics - Theory · Physics 2008-11-26 Ken Intriligator , Brian Wecht

Coincident D3-branes placed at a conical singularity are related to string theory on $AdS_5\times X_5$, for a suitable five-dimensional Einstein manifold $X_5$. For the example of the conifold, which leads to $X_5=T^{1,1}=(SU(2)\times…

High Energy Physics - Theory · Physics 2016-08-25 Steven S. Gubser , Igor R. Klebanov

We consider N =1 supersymmetric QCD with the gauge group U(N) and N_f=N quark flavors. To get rid of flat directions we add a meson superfield. The theory has no adjoint fields and, therefore, no 't Hooft-Polyakov monopoles in the…

High Energy Physics - Theory · Physics 2010-05-27 A. Gorsky , M. Shifman , A. Yung