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Related papers: Heterotic and type I strings from twisted supermem…

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We study perturbative compactifications of Type II string theory that rely on a fibration structure of the extra dimensions a la SYZ. Non-geometric spaces are obtained by using T-dualities as monodromies. These vacua generically preserve…

High Energy Physics - Theory · Physics 2009-03-04 David Vegh , John McGreevy

Taking the N=2 strings as the starting point, we discuss the equivalent self-dual field theories and analyse their symmetry structure in 2+2 dimensions. Restoring the full `Lorentz' invariance in the target space necessarily leads to an…

High Energy Physics - Theory · Physics 2009-10-30 Sergei V. Ketov

We construct the non-linear realisation of the semi-direct product of E11 and its vector representation in five and eleven dimensions and find the dynamical equations it predicts at low levels. Restricting these results to contain only the…

High Energy Physics - Theory · Physics 2016-07-20 Alexander G. Tumanov , Peter West

We establish a relation, conjectured recently by E. Witten, between the hypermultiplet moduli space in compactifications of the heterotic string on an A-D-E singularities, and the moduli spaces of three dimensional pure gauge theories with…

High Energy Physics - Theory · Physics 2009-10-31 Moshe Rozali

In heterotic string theories consistency requires the introduction of a non-trivial vector bundle. This bundle breaks the original ten-dimensional gauge groups $\text{E}_8\times\text{E}_8$ or $\text{SO}(32)$ for the supersymmetric heterotic…

High Energy Physics - Theory · Physics 2016-03-31 Stefan Groot Nibbelink , Fabian Ruehle

The common statement that any consistent quantum gravity theory contains dynamical objects with all possible charges suggests that there are still a number of hitherto-unidentified branes in string theory. Here we give the exact worldsheet…

High Energy Physics - Theory · Physics 2023-04-03 Justin Kaidi , Kantaro Ohmori , Yuji Tachikawa , Kazuya Yonekura

We investigate the possibility of large CP- violating phases in the soft breaking terms derived in superstring models. The bounds on the electric dipole moments (EDM's) of the electron and neutron are satisfied through cancellations…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Brhlik , L. Everett , G. L. Kane , J. Lykken

In this thesis, we consider heterotic string vacua based on a warped product of a four-dimensional domain wall and a six-dimensional internal manifold preserving only two supercharges. Thus, they correspond to half-BPS states of heterotic…

High Energy Physics - Theory · Physics 2012-04-17 Cyril Matti

We construct, following \cite{mpgm14,mpgm17}, a massive M2-brane (supermembrane) as the limit of a genus two M2-brane that becomes a twice punctured Riemann surface with particular boundary conditions on the fields defined on the punctures.…

High Energy Physics - Theory · Physics 2023-11-06 M. P. Garcia del Moral , P. Leon , A. Restuccia

Characters of $E_8\otimes E_8$ and SO(32) heterotic strings involving the full internal symmetry Cartan subalgebra generators are defined after circle compactification so that they are T dual. The novel point, as compared with an earlier…

High Energy Physics - Theory · Physics 2009-10-31 Jean-Loup Gervais

Type-IIB supergravity in ten dimensions admits two consistent $Z_2$ truncations. After the insertion of D9-branes, one of them leads to the low-energy action of type-I string theory, and it can be performed in two different ways, in…

High Energy Physics - Theory · Physics 2009-11-10 F. Riccioni

We look at the vertical dimensional reduction of the supermembrane of M-theory to the D2-brane of Type IIA string theory. Our approach considers the soliton solutions of the two low energy field limits, D=11 and D=10 Type IIA…

High Energy Physics - Theory · Physics 2009-10-31 C. Codirla , M. J. Perry

We demonstrate that, in an appropriate limit, the off-shell M5-brane worldvolume action effectively captures the scalar potential of Seiberg-Witten theory perturbed by a small superpotential and, consequently, any nonsupersymmetric vacua…

High Energy Physics - Theory · Physics 2010-06-28 Joseph Marsano , Kyriakos Papadodimas , Masaki Shigemori

In this paper we consider Type I string theory compactified on a Z_7 orbifold. The model has N=1 supersymmetry, a U(4) \otimes U(4) \otimes U(4) \otimes SO(8) gauge group, and chiral matter. There are only D9-branes (for which we discuss…

High Energy Physics - Theory · Physics 2010-11-19 Zurab Kakushadze , Gary Shiu

The weakly coupled vacuum of E_8 x E_8 heterotic string theory remains a promising candidate for the underlying theory of the Standard Model. The particle spectrum and the issue of dilaton stabilization are reviewed. Specific models for…

High Energy Physics - Phenomenology · Physics 2007-05-23 Mary K. Gaillard

We present a geometric formulation of type-IIA and -IIB superstring theories in which the Wess-Zumino term is second order in the supersymmetric currents. The currents are constructed using supergroup manifolds corresponding to…

High Energy Physics - Theory · Physics 2011-04-05 M. Sakaguchi

Motivated by the study of black attractors in 8D supergravity with 16 supersymmetries, we use the field theory approach and 8D supersymmetry with non trivial central charges to shed light on the exact duality between heterotic string on T^2…

High Energy Physics - Theory · Physics 2015-03-17 El Hassan Saidi

M-theory accessed via eleven-dimensional supergravity admits globally consistent warped solutions with eight-dimensional compact spaces if background fluxes and higher derivative terms are considered. The internal background is conformally…

High Energy Physics - Theory · Physics 2014-12-17 Thomas W. Grimm , Tom G. Pugh , Matthias Weissenbacher

$N=2$ string theories are formulated in space-times with 2 space and 2 time dimensions. If the world-sheet matter system consists of 2 chiral superfields, the space-time is Kahler and the dynamics are those of anti-self-dual gravity. If…

High Energy Physics - Theory · Physics 2009-10-30 C. M. Hull

After simultaneous compactification of spacetime and worldvolume on $K3$, the $D=10$ heterotic fivebrane with gauge group $SO(32)$ behaves like a $D=6$ heterotic string with gauge group $SO(28) \times SU(2)$, but with Kac--Moody levels…

High Energy Physics - Theory · Physics 2009-10-28 M. J. Duff , R. Minasian