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We study the four-dimensional low energy effective $\mathcal{N}=1$ supergravity theory of the dimensional reduction of M-theory on $G_2$-manifolds, which are constructed by Kovalev's twisted connected sum gluing suitable pairs of…

High Energy Physics - Theory · Physics 2018-01-17 Thaisa C. da C. Guio , Hans Jockers , Albrecht Klemm , Hung-Yu Yeh

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

We test various conjectures about quantum gravity for six-dimensional string compactifications in the framework of F-theory. Starting with a gauge theory coupled to gravity, we analyze the limit in K\"ahler moduli space where the gauge…

High Energy Physics - Theory · Physics 2018-11-14 Seung-Joo Lee , Wolfgang Lerche , Timo Weigand

We present gauge theories in 2+1 and 4+1 dimensions with 16 supersymmetries which are invariant under rotations and translations but not boosts. The on-shell conditions reduce the dynamics to motion on a moduli space of BPS states graded by…

High Energy Physics - Theory · Physics 2018-11-14 Neil Lambert , Miles Owen

M(atrix) theory defines light-front description of M-theory boosted along positive direction of eleventh, M-coordinate. Rank of M(atrix) gauge group is directly related to M-momentum $P_{11} = N / R_{11}$ or, equivalently, to total number…

High Energy Physics - Theory · Physics 2007-05-23 Soo-Jong Rey

We give a unified description of all BPS states of M-theory compactified on $T^5$ in terms of the five-brane. We compute the mass spectrum and degeneracies and find that the $SO(5,5,Z)$ U-duality symmetry naturally arises as a T-duality by…

High Energy Physics - Theory · Physics 2009-07-09 R. Dijkgraaf , E. Verlinde , H. Verlinde

We find giant graviton configurations of an M5-brane probe in the D=11 supergravity background generated by a stack of non-threshold (M2,M5) bound states. The M5-brane probe shares three directions with the background and wraps a two-sphere…

High Energy Physics - Theory · Physics 2008-11-26 J. M. Camino , A. V. Ramallo

We construct new M-theory solutions of M5 branes that are a realization of the fully localized ten dimensional NS5/D6 and NS5/D5 brane intersections. These solutions are obtained by embedding self-dual geometries lifted to M-theory. We…

High Energy Physics - Theory · Physics 2009-11-10 R. Clarkson , A. M. Ghezelbash , R. B. Mann

We construct supergravity solutions dual to the twisted field theories arising when M-theory fivebranes wrap general supersymmetric cycles. The solutions are constructed in maximal D=7 gauged supergravity and then uplifted to D=11. Our…

High Energy Physics - Theory · Physics 2009-10-31 Jerome P. Gauntlett , Nakwoo Kim , Daniel Waldram

We study compactifications of string theory and M-theory to six dimensions with background fluxes. The nonzero fluxes lead to additional mass parameters. We derive the S- and T-duality rules for the corresponding (massive) supergravity…

High Energy Physics - Theory · Physics 2008-12-18 K. Behrndt , E. Bergshoeff , D. Roest , P. Sundell

The proposal that a strong coupling limit of the five-dimensional type II string theory (M-theory compactified on a 6-torus) in which the Planck length becomes infinite could give a six-dimensional superconformal phase of M-theory is…

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

In this paper we introduce the concept of MV-topology, a special class of fuzzy topological spaces, and prove a proper extension of Stone Duality to the categories of limit cut complete MV-algebras and Stone MV-spaces, namely,…

Logic · Mathematics 2015-11-13 Ciro Russo

We study M theory compactifications on manifolds of $G_2$-holonomy with gauge and matter fields supported at singularities. We show that, under certain topological conditions, the combination of background $G$-flux and background fields at…

High Energy Physics - Theory · Physics 2007-05-23 Bobby S Acharya

We present three lectures on heterotic M-theory and a fourth lecture extending this theory to more general orbifolds. In Lecture 1, Horava-Witten theory is briefly discussed. We then compactify this theory on Calabi-Yau threefolds, choosing…

High Energy Physics - Theory · Physics 2007-05-23 Burt A. Ovrut

Horava--Witten M theory -- heterotic string duality poses special problems for the twisted sectors of heterotic orbifolds. In [1] we explained how in M theory the twisted states couple to gauge fields apparently living on M9 branes at both…

High Energy Physics - Theory · Physics 2014-11-18 E. Gorbatov , V. S. Kaplunovsky , J. Sonnenschein , S. Theisen , S. Yankielowicz

We discuss the properties of the bound state (F1, D1, D3) in IIB supergravity in three different scaling limits and the $SL(2,{\bf Z})$ transformation of the resulting theories. In the simple decoupling limit with finite electric and…

High Energy Physics - Theory · Physics 2009-10-31 Rong-Gen Cai , Nobuyoshi Ohta

We consider a brane world scenario which arises as the near-horizon region of a non-extremal D5-brane. There is a quasi-localized massive graviton mode, as well as harmonic modes of higher mass which are bound to the brane to a lesser…

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

We consider M-theory on (T^2\times R^2)/Z_n with M5 branes wrapped on R^2. One can probe this background with M5 branes wrapped on T^2. The theories on the probes provide many new examples of N=2 field theories without Lagrangian…

High Energy Physics - Theory · Physics 2009-02-23 Sergei Gukov , Anton Kapustin

We analyze $M$-theory compactified on $(K3\times S^1)/Z_2$ where the $Z_2$ changes the sign of the three form gauge field, acts on $S^1$ as a parity transformation and on K3 as an involution with eight fixed points preserving SU(2)…

High Energy Physics - Theory · Physics 2009-09-15 Ashoke Sen

We show that the existence of semiclassical black holes of size as small as a minimal length scale $l_{UV}$ implies a bound on a gravitational analogue of 't-Hooft's coupling $\lambda_G(l)\equiv N(l) G_N/l^2$ at all scales $l \ge l_{UV}$.…

High Energy Physics - Theory · Physics 2009-11-09 R. Brustein , G. Dvali , G. Veneziano
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