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A representation of the exchange relation for affine Toda field theory

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A representation of the exchange relation for affine Toda field theory

Auteurs : E. Corrigan [Royaume-Uni] ; P. E. Dorey [France]

Source :

Physics Letters B [ 0370-2693 ] ; 1991.

RBID : ISTEX:E23F8C08A8210700367F816B63648C576B8F7EA0

English descriptors

KwdEn :
- Affine, Affine toda, Affine toda couplings, Affine toda field theories, Affine toda field theory, Affine toda theory, Algebra, Analytic continuation, Annihilation part, Bootstrap, Cartan matrix, Commutation relation, Commutation relations, Computational purposes, Conformal, Conformal field theory, Conformal nature, Constant dependence, Coxeter, Coxeter element, Creation operators, Creation part, December, Eigenvalue, Euclidean section, Exchange relation, Exponent, Fock, Fock space operators, Fundamental weights, Inner products, Lett, Minimal part, Next section, Nucl, Operator product, Opposite sign, Order poles, Other words, Particle type, Perturbation theory, Perturbed conformal field theory, Phys, Physics letters, Physics lettersb, Quantum theory, Rapidity, Rapidity dependence, Rapidity difference, Root systems, Same colour, Similar expression, Simple roots, Single particle state, Single particle states, Toda, Vertex operator, Vertex operators, Weyl group.
Teeft :
- Affine, Affine toda, Affine toda couplings, Affine toda field theories, Affine toda field theory, Affine toda theory, Algebra, Analytic continuation, Annihilation part, Bootstrap, Cartan matrix, Commutation relation, Commutation relations, Computational purposes, Conformal, Conformal field theory, Conformal nature, Constant dependence, Coxeter, Coxeter element, Creation operators, Creation part, December, Eigenvalue, Euclidean section, Exchange relation, Exponent, Fock, Fock space operators, Fundamental weights, Inner products, Lett, Minimal part, Next section, Nucl, Operator product, Opposite sign, Order poles, Other words, Particle type, Perturbation theory, Perturbed conformal field theory, Phys, Physics letters, Physics lettersb, Quantum theory, Rapidity, Rapidity dependence, Rapidity difference, Root systems, Same colour, Similar expression, Simple roots, Single particle state, Single particle states, Toda, Vertex operator, Vertex operators, Weyl group.

Abstract

Abstract: Vertex operators are constructed providing representations of the exchange relations containing either the S-matrix of a real coupling (simply-laced) affine Toda field theory, or its minimal counterpart. One feature of the construction is that the bootstrap relations for the S-matrices follow automatically from those for the conserved quantities, via an algebraic interpretation of the fusing of two particles to form a single bound state.

Url:

https://api.istex.fr/document/E23F8C08A8210700367F816B63648C576B8F7EA0/fulltext/pdf

DOI: 10.1016/0370-2693(91)91677-N

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Le document en format XML

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<term>Next section</term>
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<term>Order poles</term>
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<term>Physics letters</term>
<term>Physics lettersb</term>
<term>Quantum theory</term>
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<term>Cartan matrix</term>
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<term>Conformal field theory</term>
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<term>Constant dependence</term>
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<term>Creation part</term>
<term>December</term>
<term>Eigenvalue</term>
<term>Euclidean section</term>
<term>Exchange relation</term>
<term>Exponent</term>
<term>Fock</term>
<term>Fock space operators</term>
<term>Fundamental weights</term>
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<term>Minimal part</term>
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<term>Operator product</term>
<term>Opposite sign</term>
<term>Order poles</term>
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<term>Perturbation theory</term>
<term>Perturbed conformal field theory</term>
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<term>Physics letters</term>
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<term>Rapidity dependence</term>
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A representation of the exchange relation for affine Toda field theory

A representation of the exchange relation for affine Toda field theory

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Abstract

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