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Related papers: The Loop Group of E8 and Targets for Spacetime

200 papers

For the simply connected compact exceptional Lie group $E_8$, we determine the structure of subgroup $(E_8)^{\sigma, \sigma'}$ of $E_8$ which is the intersection $(E_8)^\sigma \cap (E_8)^{\sigma'}$. Then the space $E_8/(E_8)^{\sigma,…

Differential Geometry · Mathematics 2010-12-17 Toshikazu Miyashita

A correspondence between type IIB string theory with N D7-branes on R^{1,3} x C^1/Z_2 x T^2/Z_2 x T^2/Z_2 and pure N=1 SU(N) gauge theory in four dimensions is proposed and argued. First the supergravity background of unwrapped and flat…

High Energy Physics - Theory · Physics 2013-05-29 Girma Hailu

We use an exactly solvable (0,2) supersymmetric conformal field theory with gauge group SO(10) to investigate the superpotential of the corresponding classical string vacuum. We provide evidence that the rational point lies in the…

High Energy Physics - Theory · Physics 2009-10-30 Ralph Blumenhagen , Andreas Wisskirchen

The Coset Space Dimensional Reduction scheme is briefly reviewed. Then a ten-dimensional supersymmetric $E_8$ gauge theory is reduced over symmetric and non-symmetric six-dimensional coset spaces. In general a four-dimensional…

High Energy Physics - Phenomenology · Physics 2017-08-23 P. Manousselis , G. Zoupanos

As shown by Ho\v{r}ava and Witten, there are gravitational anomalies at the boundaries of $M^{10}\times S^1/Z_2$ of 11 dimensional supergravity. They showed that only 10 dimensional vector multiplets belonging to $E_8$ gauge group can be…

High Energy Physics - Theory · Physics 2009-10-30 F. Aldabe

By identifying the moduli space of coupling constants in the SYM description of toroidal compactifications of M(atrix)-Theory, we construct the M(atrix) description of the moduli spaces of Type IIA string theory compactified on T^n.…

High Energy Physics - Theory · Physics 2010-11-19 David Berenstein , Richard Corrado , Jacques Distler

We show that in the context of two-dimensional sigma models minimal coupling of an ordinary rigid symmetry Lie algebra $\mathfrak{g}$ leads naturally to the appearance of the "generalized tangent bundle" $\mathbb{T}M \equiv TM \oplus T^*M$…

High Energy Physics - Theory · Physics 2015-06-22 Alexei Kotov , Vladimir Salnikov , Thomas Strobl

A factorization of spacetime of the form M^3xM^3xM^3 is considered in this paper as the closed string background in type IIA. The idea behind this construction is that each M^3 might give rise to one large spatial dimension of 4-dimensional…

High Energy Physics - Theory · Physics 2009-11-11 Tassilo Ott

We study limits of four-dimensional type II Calabi-Yau compactifications with vanishing four-cycle singularities, which are dual to $\IT^2$ compactifications of the six-dimensional non-critical string with $E_8$ symmetry. We define proper…

High Energy Physics - Theory · Physics 2016-09-06 W. Lerche , P. Mayr , N. P. Warner

We describe three previously unnoticed components of the moduli space of minimally supersymmetric string theories in $d\geq 7$, describing in some detail their spectrum and duality properties. We find a new component in nine and eight…

High Energy Physics - Theory · Physics 2023-02-01 Miguel Montero , Hector Parra de Freitas

First, we review the basic mathematical structures and results concerning the gauge orbit space stratification. This includes general properties of the gauge group action, fibre bundle structures induced by this action, basic properties of…

High Energy Physics - Theory · Physics 2009-11-07 G. Rudolph , M. Schmidt , I. P. Volobuev

The compactification from the 11-dimensional Horava-Witten orbifold to 5-dimensional heterotic M-theory on a Schoen Calabi-Yau threefold is reviewed, as is the specific $SU(4)$ vector bundle leading to the "heterotic standard model" in the…

High Energy Physics - Theory · Physics 2020-02-17 Burt A. Ovrut

We derive the precise relation between level matching condition and fractional instanton numbers in six dimensional, abelian and supersymmetric orbifolds of E8 x E8 heterotic string theory. The fractional part of the two E8 instanton…

High Energy Physics - Theory · Physics 2009-10-31 Jan O. Conrad

The pull back of a flat bundle $E\rightarrow X$ along the evaluation map $\pi: \mathcal{L} X \to X$ from the free loop space $\mathcal{L} X$ to $X$ comes equipped with a canonical automorphism given by the holonomies of $E$. This…

Differential Geometry · Mathematics 2015-10-19 Camilo Arias Abad , Florian Schaetz

The fields of the conjectured ``heterotic" super--fivebrane sigma--model in ten dimensions are made out of a well known gravitational sector, the $X$ and the $\vartheta$, and of a still unknown heterotic sector which should be coupled to…

High Energy Physics - Theory · Physics 2009-10-30 K. Lechner , M. Tonin

The supermembrane in light-cone gauge gives rise to a supersymmetric quantum mechanics system with SU(N) gauge symmetry when the group of area preserving diffeomorphisms is suitably regulated. de Wit, Marquard and Nicolai showed how…

High Energy Physics - Theory · Physics 2010-02-03 David A. Lowe

We extend the analysis of arXiv:1009.2624, which constructed the non-linear realisation of the semi-direct product of E11 and the l1 representation at level zero, to level one. Thus we add to the previously considered NS-NS fields those of…

High Energy Physics - Theory · Physics 2011-04-06 Andreas Rocen , Peter West

Research at the intersection of quantum gravity and quantum information theory has seen significant success in describing the emergence of spacetime and gravity from quantum states whose entanglement entropy approximately obeys an area law.…

Quantum Physics · Physics 2025-12-22 Jochen Szangolies

We present a new duality between the F-terms of supersymmetric field theories defined in two- and four-dimensions respectively. The duality relates N=2 supersymmetric gauge theories in four dimensions, deformed by an Omega-background in one…

High Energy Physics - Theory · Physics 2015-05-27 Nick Dorey , Timothy J. Hollowood , Sungjay Lee

We propose a new class of gravity-matter-gauge theories in terms of two different non-Riemannian volume-forms independent of the Riemannian metric. The nonlinear gauge field system contains a square-root $\sqrt{-F^2}$ of the standard…

General Relativity and Quantum Cosmology · Physics 2015-07-23 Eduardo Guendelman , Emil Nissimov , Svetlana Pacheva