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Keith Glennon

Publications and source records attributed to Keith Glennon.

10 recordsLinked to original sources

Local symmetry and the dependence on extended spacetime

We show that linearised E theory possesses a local symmetry at low levels provided the parameters of the local symmetry obey differential conditions that restrict their dependence on the extended spacetime. In the decomposition of E theory that leads to Siegel theory, also known as Double Field theory, we also find the analogous restrictions on the parameters. They are different to the section conditions which are universally used in this context. We also show that the dilaton equation of Siegel theory is invariant under the local symmetry if the parameters satisfy an analogous non-linear constraint on the parameters. We argue that there is no need to impose conditions on the fields of E theory or Siegel theory.

hep-th

On the Sugawara Current Algebra Proposal for M-Theory

We examine the proposal of [29] that M-theory may admit a Sugawara-type current algebra formulation based on $E_{11} \otimes_s l_1$. Motivated by the role of generalized coordinates in E-theory, we ask whether current algebra relations of this type can be derived in a setting that includes those coordinates systematically. We show that such a construction can indeed be carried out for a rigid $E_{11}$ model in which the generalized coordinates are treated as inert under the rigid symmetry, in contrast with E-theory. We also argue that the bilinear form entering the Schwinger term requires closer scrutiny, since any natural ad-invariant extension of the $E_{11}$ Cartan-Killing form to $E_{11} \otimes_s l_1$ is degenerate.

hep-th

Diagonalization Procedure for Reducible Massless N=1 Supermultiplets

We consider N=1 supersymmetric systems in d=4, 6 and 10 dimensions which consist of reducible bosonic and fermionic massless representations of the Poincare group. We show in detail how to decompose the corresponding Lagrangians into a sum of Lagrangians for irreducible representations of the Poincare group. We also outline a modification of this procedure in the case of an anti-de Sitter background.

hep-th

Bosonic M-Theory From a Kac-Moody Algebra Perspective

We study the existence of a bosonic m-theory extension of the 10D and 26D closed bosonic string in terms of Kac-Moody algebras. We argue that K11 and K27 are symmetries which protect the coefficients of the closed bosonic string in 10 and 26 dimensions. Therefore the Susskind-Horowitz bosonic m-theory obtained by compactification on S1/Z2, which does not produce the correct coefficients, must be replaced by something that preserves K11 and K27. We argue that in 11D, a non-trivial bosonic m-theory should be considered as (the bosonic sector of) m-theory, and in 27D that no obvious bosonic m-theory exists.

hep-th

K27 as a symmetry of closed bosonic strings and branes

We show that the dynamics encoded in the non-linear realisation of the semi-direct product of the very extended algebra K27 with its vector representation contains the low energy effective action of the closed bosonic string.

hep-th

Applications of Kac-Moody Algebras to Gravity and String Theory

It has previously been proposed that the the theory of strings and branes possesses a large symmetry group generated by the Kac-Moody algebra $E_{11}$. It has also previously been proposed that the the theory of gravitation in four dimensions possesses a large symmetry group generated by the Kac-Moody algebra $A_1^{+++}$. These symmetry groups predict the existence of an infinite collection of fields in each theory, including a field that can be interpreted as a dual graviton. In this thesis we will discuss developments related to these approaches to string theory and gravity. We begin by reviewing the method of nonlinear realizations, then introducing the Kac-Moody algebra $A_1^{+++}$, along with its first fundamental representation representation which introduces space-time, to low levels. We will then consider a nonlinear realization involving their semi-direct product, and use the associated Cartan forms to construct dynamics for the low level fields of this nonlinear realization. We will then propose duality relations between fields of the theory at different levels, and propose a nonlinear equation of motion for the dual graviton arising from $A_1^{+++}$. We then consider the analogous results for $E_{11}$, and describe a proposed nonlinear dual graviton equation in the context of string theory. We next discuss irreducible representations of $E_{11}$. We will construct isotropy groups associated to massive and massless particles, branes such as the M2 and M5 branes, and the IIA string. Finally we present an approach for introducing spinorial representations of the Kac-Moody algebra $E_{11}$.

hep-th

The string little algebra

We consider the string, like point particles and branes, to be an irreducible representation of the semi-direct product of the Cartan involution invariant subalgebra of E11 and its vector representation. We show that the subalgebra that preserves the string charges, the string little algebra, is essentially the Borel subalgebra of E9. We also show that the known string physical states carry a representation of parts of this algebra.

hep-th

The massless irreducible representation in E theory and how bosons can appear as spinors

We study in detail the irreducible representation of E theory that corresponds to massless particles. This has little algebra Ic(E9) and contains 128 physical states that belong to the spinor representation of SO(16). These are the degrees of freedom of maximal supergravity in eleven dimensions. This smaller number of the degrees of freedom, compared to what might be expected, is due to an infinite number of duality relations which in turn can be traced to the existence of a subaglebra of Ic(E9) which forms an ideal and annihilates the representation. We explain how these features are inherited into the covariant theory. We also comment on the remarkable similarity between how the bosons and fermions arise in E theory.

hep-th

Gravity, Dual Gravity and A1+++

We construct the non-linear realisation of the semi-direct product of the very extended algebra A1+++ and its vector representation. This theory has an infinite number of fields that depend on a spacetime with an infinite number of coordinates. Discarding all except the lowest level field and coordinates the dynamics is just Einstein's equation for the graviton field. We show that the gravity field is related to the dual graviton field by a duality relation and we also derive the equation of motion for the dual gravity field.

hep-th