Irreducible representations of E theory

DOI10.1142/S0217751X19501331zbMath1471.83024arXiv1905.07324OpenAlexW3100924311MaRDI QIDQ5010174

Peter C. West

Publication date: 24 August 2021

Published in: International Journal of Modern Physics A (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/1905.07324

zbMATH Keywords

supergravityduality symmetriesstringsbranes

Mathematics Subject Classification ID

String and superstring theories in gravitational theory (83E30) Supergravity (83E50) Infinite-dimensional groups and algebras motivated by physics, including Virasoro, Kac-Moody, (W)-algebras and other current algebras and their representations (81R10) String and superstring theories; other extended objects (e.g., branes) in quantum field theory (81T30) Classes of solutions; algebraically special solutions, metrics with symmetries for problems in general relativity and gravitational theory (83C20) Kaluza-Klein and other higher-dimensional theories (83E15) Structure and representation of the Lorentz group (22E43) Correspondence, duality, holography (AdS/CFT, gauge/gravity, etc.) (81T35)

Related Items (1)

Higher dualisations of linearised gravity and the \(A_1^{+++}\) algebra

Cites Work

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• A remark on the scattering of BPS monopoles.
• Tensor gauge fields in arbitrary representations of \(\operatorname{GL}(D,\mathbb R)\). Duality and Poincaré lemma
• M-theory and \(U\)-duality on \(T^d\) with gauge backgrounds
• \(E_{11}\) must be a symmetry of strings and branes
• An E11 invariant gauge fixing
• Mixed-symmetry multiplets and higher-spin curvatures

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