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Related papers: E8(8) in Light Cone Superspace

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All fields of the standard model and gravity are unified as an E8 principal bundle connection. A non-compact real form of the E8 Lie algebra has G2 and F4 subalgebras which break down to strong su(3), electroweak su(2) x u(1), gravitational…

High Energy Physics - Theory · Physics 2007-11-13 A. Garrett Lisi

We present a simple form of the on-shell gauge-invariant 1-loop effective action of N=8 supergravity which is manifestly N=8 supersymmetric at the linear level. By generalizing the dimensional arguments in superspace to non-local…

High Energy Physics - Theory · Physics 2007-11-15 Renata Kallosh

Models of interactions of D-dimensional hypermultiplets and supersymmetric gauge multiplets with $\mathcal{N}=8$ supercharges $(D{\leq} 6)$ can be formulated in the framework of harmonic superspaces. The effective Coulomb low-energy action…

High Energy Physics - Theory · Physics 2017-09-07 B. M. Zupnik

Light-cone gauge manifestly supersymmetric formulation of eleven dimensional supergravity is developed. The formulation is given entirely in terms of light cone scalar superfield, allowing us to treat all component fields on an equal…

High Energy Physics - Theory · Physics 2009-11-10 R. R. Metsaev

We re-examine the question of heterotic - heterotic string duality in six dimensions and argue that the $E_8\times E_8$ heterotic string, compactified on $K3$ with equal instanton numbers in the two $E_8$'s, has a self-duality that inverts…

High Energy Physics - Theory · Physics 2010-04-07 M. J. Duff , R. Minasian , Edward Witten

We study the (2,0) superconformal theories in six dimensions, which arise from the low-energy limit of k coincident 5-branes, using their discrete light-cone formulation as a superconformal quantum mechanical sigma model. We analyze the…

High Energy Physics - Theory · Physics 2016-09-06 O. Aharony , M. Berkooz , N. Seiberg

In this article actions for N=4 SYM and N=8 supergravity are formulated in terms of a chiral superfield, which contains only the physical degrees of freedom of either theory. In these new actions, which originate from the lightcone…

High Energy Physics - Theory · Physics 2011-08-29 Johannes Broedel , Renata Kallosh

We construct a new two-dimensional N=8 supersymmetric mechanics with nonlinear chiral supermultiplet. Being intrinsically nonlinear this multiplet describes 2 physical bosonic and 8 fermionic degrees of freedom. We construct the most…

High Energy Physics - Theory · Physics 2008-11-26 S. Bellucci , A. Beylin , S. Krivonos , A. Shcherbakov

We construct a pseudo-Lagrangian that is invariant under rigid $E_{11}$ and transforms as a density under $E_{11}$ generalised diffeomorphisms. The gauge-invariance requires the use of a section condition studied in previous work on…

High Energy Physics - Theory · Physics 2021-07-14 Guillaume Bossard , Axel Kleinschmidt , Ergin Sezgin

We consider the 5-brane placed at one end of the world in the Heterotic $E_8 \times E_8$ theory. The low energy theory is a 6 dimensional $(1,0)$ superconformal theory with $E_8$ as a global symmetry. We calculate the two-point correlator…

High Energy Physics - Theory · Physics 2007-05-23 Morten Krogh

We reformulate self-dual supersymmetric theories directly in conformal chiral superspace, where superconformal invariance is manifest. The superspace can be interpreted as the generalization of the usual Atiyah-Drinfel'd-Hitchin-Manin…

High Energy Physics - Theory · Physics 2009-10-28 W. Siegel

N-extended massless arbitrary integer and half-integer spin supermultiplets in four dimensional flat space are studied in the framework of light-cone gauge formalism. For such multiplets, by using light-cone momentum superspace, we build…

High Energy Physics - Theory · Physics 2020-01-08 R. R. Metsaev

We present a superspace formulation for super eightbrane theory based on massive type IIA supergravity in ten-dimensions. Remarkably, in addition to the 10-form superfield strength originally needed for super eightbrane, we also need an…

High Energy Physics - Theory · Physics 2009-10-31 Hitoshi Nishino

We present a systematic analysis of the N=8 superspace constraints in three space-time dimensions. The general coupling between vector and scalar supermultiplets is encoded in an SO(8) tensor W_{AB} which is a function of the matter fields…

High Energy Physics - Theory · Physics 2010-03-17 Henning Samtleben , Robert Wimmer

We consider tachyon condensation in unstable ten-dimensional heterotic string theory with gauge group E8. In the background of a lightlike linear dilaton rolling to weak coupling, we find an exact solution in which the theory decays to a…

High Energy Physics - Theory · Physics 2008-04-29 Simeon Hellerman , Ian Swanson

The hyperbolic Kac-Moody algebra E10 has repeatedly been suggested to play a crucial role in the symmetry structure of M-theory. Recently, following the analysis of the asymptotic behaviour of the supergravity fields near a cosmological…

High Energy Physics - Theory · Physics 2009-11-11 S. de Buyl , M. Henneaux , L. Paulot

Starting from the QCD Hamiltonian in near-light cone coordinates, we study the dynamics of the gluonic zero modes. Euclidean 2+1 dimensional lattice simulations show that the gap at strong coupling vanishes at intermediate coupling. This…

High Energy Physics - Phenomenology · Physics 2009-10-31 E. -M. Ilgenfritz , Yu. P. Ivanov , H. -J. Pirner

A topological theory for euclidean gravity in eight dimensions is built by enforcing octonionic self-duality conditions on the spin connection. The eight-dimensional manifold must be of a special type, with G_2 or Spin(7) holonomy. The…

High Energy Physics - Theory · Physics 2015-06-26 Laurent Baulieu , Marc Bellon , Alessandro Tanzini

Maximally supersymmetric theories can be described by a single scalar superfield in light-cone superspace. When they are also (super)conformally invariant, they are uniquely specified by the form of the dynamical supersymmetry. We present…

High Energy Physics - Theory · Physics 2010-03-09 Dmitry V. Belyaev

We construct the non-linear realisation of the E8 motion group and compare this with the bosonic sector of eleven dimensional supergravity. The construction naturally leads to the introduction of a new potential field. We identify this new…

High Energy Physics - Theory · Physics 2015-06-15 Hadi Godazgar , Mahdi Godazgar , Malcolm J. Perry