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Related papers: Higher spin representations of K(E10)

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In recent work arXiv:1412.1715 it was shown how to modify Gell-Mann's proposal for identifying the 48 quarks and leptons of the Standard Model with the 48 spin-1/2 fermions of maximal SO(8) gauged supergravity that remain after the removal…

High Energy Physics - Theory · Physics 2015-07-02 Axel Kleinschmidt , Hermann Nicolai

We work out the decomposition of the indefinite Kac Moody algebras ${E_{10}}$ and ${E_{11}}$ w.r.t. their respective subalgebras $A_9$ and $A_{10}$ at low levels. Tables of the irreducible representations with their outer multiplicities are…

High Energy Physics - Theory · Physics 2007-05-23 Hermann Nicolai , Thomas Fischbacher

The involutory subalgebra K(E$_9$) of the affine Kac-Moody algebra E$_9$ was recently shown to admit an infinite sequence of unfaithful representations of ever increasing dimensions arXiv:2102.00870. We revisit these representations and…

High Energy Physics - Theory · Physics 2025-10-13 Axel Kleinschmidt , Hermann Nicolai

A lot of developments made during the last years show that Kac-Moody algebras play an important role in the algebraic structure of some supergravity theories. These algebras would generate infinite-dimensional symmetry groups. The possible…

High Energy Physics - Theory · Physics 2009-10-09 Nassiba Tabti

In this thesis we study algebraic structures in M-theory, in particular the exceptional Lie algebras arising in dimensional reduction of its low energy limit, eleven-dimensional supergravity. We focus on e8 and its infinite-dimensional…

High Energy Physics - Theory · Physics 2009-12-10 Jakob Palmkvist

We investigate the possibility to construct extended parafermionic conformal algebras whose generating current has spin $1+\frac{1}{K}$, generalizing the superconformal (spin 3/2) and the Fateev Zamolodchikov (spin 4/3) algebras. Models…

High Energy Physics - Theory · Physics 2015-06-26 F. Ravanini

We establish a dynamical equivalence between the bosonic part of pure type I supergravity in D=10 and a D=1 non-linear sigma-model on the Kac-Moody coset space DE(10)/K(DE(10)) if both theories are suitably truncated. To this end we make…

High Energy Physics - Theory · Physics 2008-11-26 Christian Hillmann , Axel Kleinschmidt

This article presents a new relation between the basic representation of split real simply-laced affine Kac-Moody algebras and finite dimensional representations of its maximal compact subalgebra $\mathfrak{k}$. We provide infinitely many…

Representation Theory · Mathematics 2024-07-18 Benedikt König

We define a level for a large class of Lorentzian Kac-Moody algebras. Using this we find the representation content of very extended $A_{D-3}$ and $E_8$ (i.e. $E_{11}$) at low levels in terms of $A_{D-1}$ and $A_{10}$ representations…

High Energy Physics - Theory · Physics 2016-09-06 P. West

We construct the E theory analogue of the particles that transform under the Poincare group, that is, the irreducible representations of the semi-direct product of the Cartan involution subalgebra of E11 with its vector representation. We…

High Energy Physics - Theory · Physics 2019-09-25 Peter West

Following up on our earlier work where we showed how to amend a scheme originally proposed by M. Gell-Mann to identify the 48 spin 1/2 fermions of N=8 supergravity that remain after complete breaking of N=8 supersymmetry with the 3x16…

High Energy Physics - Theory · Physics 2018-09-12 Krzysztof A. Meissner , Hermann Nicolai

We study the supersymmetric quantum dynamics of the cosmological models obtained by reducing $D=5$ supergravity to one timelike dimension. This consistent truncation has fourteen bosonic degrees of freedom, while the quantization of the…

High Energy Physics - Theory · Physics 2022-06-29 Thibault Damour , Philippe Spindel

We study spin structures on affine Kac-Moody symmetric spaces and obtain sufficient conditions for their existence.\ As a by product of this, we obtain a spin-c representation of certain Kac-Moody quadratic subgroups of type E.

Mathematical Physics · Physics 2020-09-17 Amir Farahmand Parsa

We investigate some of the motivations and consequences of the conjecture that the Kac-Moody algebra E11 is the symmetry algebra of M-theory, and we develop methods to aid the further investigation of this idea. The definitions required to…

High Energy Physics - Theory · Physics 2007-11-26 Paul P. Cook

Let G be a split real Kac-Moody group of arbitrary type and let K be its maximal compact subgroup, i.e. the subgroup of elements fixed by a Cartan-Chevalley involution of G. We construct non-trivial spin covers of K, thus confirming a…

Group Theory · Mathematics 2015-02-26 David Ghatei , Max Horn , Ralf Köhl , Sebastian Weiß

We re-examine previously found cosmological solutions to eleven-dimensional supergravity in the light of the E_{10}-approach to M-theory. We focus on the solutions with non zero electric field determined by geometric configurations (n_m,…

High Energy Physics - Theory · Physics 2009-11-11 Marc Henneaux , Mauricio Leston , Daniel Persson , Philippe Spindel

I begin with some memories of Abdus Salam who was my PhD supervisor. After reviewing the theory of non-linear realisations and Kac-Moody algebras, I explain how to construct the non-linear realisation based on the Kac-Moody algebra E11 and…

High Energy Physics - Theory · Physics 2016-10-12 Peter West

In view of the newly conjectured Kac-Moody symmetries of supergravity theories placed in eleven and ten dimensions, the relation between these symmetry groups and possible compactifications are examined. In particular, we identify the…

High Energy Physics - Theory · Physics 2009-11-10 Igor Schnakenburg , Andre Miemiec

We show that (massive) D=10 type IIA supergravity possesses a hidden rigid SO(9,9) symmetry and a hidden local SO(9) x SO(9) symmetry upon dimensional reduction to one (time-like) dimension. We explicitly construct the associated locally…

High Energy Physics - Theory · Physics 2009-11-10 Axel Kleinschmidt , Hermann Nicolai

The Lorentzian Kac-Moody algebra E11, obtained by doubly overextending the compact E8, is decomposed into representations of its canonical hyperbolic E10 subalgebra. Whereas the appearing representations at levels 0 and 1 are known on…

High Energy Physics - Theory · Physics 2010-04-05 Axel Kleinschmidt