A representation of the exchange relation for affine Toda field theory
Identifieur interne : 002E47 ( Istex/Corpus ); précédent : 002E46; suivant : 002E48A representation of the exchange relation for affine Toda field theory
Auteurs : E. Corrigan ; P. E. DoreySource :
- Physics Letters B [ 0370-2693 ] ; 1991.
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:
DOI: 10.1016/0370-2693(91)91677-N
Links to Exploration step
ISTEX:E23F8C08A8210700367F816B63648C576B8F7EA0Le document en format XML
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Corrigan</name><affiliation><mods:affiliation>Department of Mathematical Sciences, University of Durham, Durham DH1 3LE, UK</mods:affiliation></affiliation></author><author><name sortKey="Dorey, P E" sort="Dorey, P E" uniqKey="Dorey P" first="P. E." last="Dorey">P. E. Dorey</name><affiliation><mods:affiliation>Service de Physique Théorique de Saclay, F-91191 Gif-sur-Yvette Cedex, France</mods:affiliation></affiliation></author></analytic><monogr></monogr><series><title level="j">Physics Letters B</title><title level="j" type="abbrev">PLB</title><idno type="ISSN">0370-2693</idno><imprint><publisher>ELSEVIER</publisher><date type="published" when="1991">1991</date><biblScope unit="volume">273</biblScope><biblScope unit="issue">3</biblScope><biblScope unit="page" from="237">237</biblScope><biblScope unit="page" to="245">245</biblScope></imprint><idno type="ISSN">0370-2693</idno></series></biblStruct></sourceDesc><seriesStmt><idno type="ISSN">0370-2693</idno></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Affine</term><term>Affine toda</term><term>Affine toda couplings</term><term>Affine toda field theories</term><term>Affine toda field theory</term><term>Affine toda theory</term><term>Algebra</term><term>Analytic continuation</term><term>Annihilation part</term><term>Bootstrap</term><term>Cartan matrix</term><term>Commutation relation</term><term>Commutation relations</term><term>Computational purposes</term><term>Conformal</term><term>Conformal field theory</term><term>Conformal nature</term><term>Constant dependence</term><term>Coxeter</term><term>Coxeter element</term><term>Creation operators</term><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><term>Inner products</term><term>Lett</term><term>Minimal part</term><term>Next section</term><term>Nucl</term><term>Operator product</term><term>Opposite sign</term><term>Order poles</term><term>Other words</term><term>Particle type</term><term>Perturbation theory</term><term>Perturbed conformal field theory</term><term>Phys</term><term>Physics letters</term><term>Physics lettersb</term><term>Quantum theory</term><term>Rapidity</term><term>Rapidity dependence</term><term>Rapidity difference</term><term>Root systems</term><term>Same colour</term><term>Similar expression</term><term>Simple roots</term><term>Single particle state</term><term>Single particle states</term><term>Toda</term><term>Vertex operator</term><term>Vertex operators</term><term>Weyl group</term></keywords><keywords scheme="Teeft" xml:lang="en"><term>Affine</term><term>Affine toda</term><term>Affine toda couplings</term><term>Affine toda field theories</term><term>Affine toda field theory</term><term>Affine toda theory</term><term>Algebra</term><term>Analytic continuation</term><term>Annihilation part</term><term>Bootstrap</term><term>Cartan matrix</term><term>Commutation relation</term><term>Commutation relations</term><term>Computational purposes</term><term>Conformal</term><term>Conformal field theory</term><term>Conformal nature</term><term>Constant dependence</term><term>Coxeter</term><term>Coxeter element</term><term>Creation operators</term><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><term>Inner products</term><term>Lett</term><term>Minimal part</term><term>Next section</term><term>Nucl</term><term>Operator product</term><term>Opposite sign</term><term>Order poles</term><term>Other words</term><term>Particle type</term><term>Perturbation theory</term><term>Perturbed conformal field theory</term><term>Phys</term><term>Physics letters</term><term>Physics lettersb</term><term>Quantum theory</term><term>Rapidity</term><term>Rapidity dependence</term><term>Rapidity difference</term><term>Root systems</term><term>Same colour</term><term>Similar expression</term><term>Simple roots</term><term>Single particle state</term><term>Single particle states</term><term>Toda</term><term>Vertex operator</term><term>Vertex operators</term><term>Weyl group</term></keywords></textClass><langUsage><language ident="en">en</language></langUsage></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">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. 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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.</p></abstract></profileDesc><revisionDesc><change when="1991-10-03">Modified</change><change when="1991">Published</change></revisionDesc></teiHeader></istex:fulltextTEI><json:item><extension>txt</extension><original>false</original><mimetype>text/plain</mimetype><uri>https://api.istex.fr/document/E23F8C08A8210700367F816B63648C576B8F7EA0/fulltext/txt</uri></json:item></fulltext><metadata><istex:metadataXml wicri:clean="Elsevier, elements deleted: tail"><istex:xmlDeclaration>version="1.0" encoding="utf-8"</istex:xmlDeclaration><istex:docType PUBLIC="-//ES//DTD journal article DTD version 4.5.2//EN//XML" URI="art452.dtd" name="istex:docType"></istex:docType><istex:document><converted-article version="4.5.2" docsubtype="fla"><item-info><jid>PLB</jid><aid>9191677N</aid><ce:pii>0370-2693(91)91677-N</ce:pii><ce:doi>10.1016/0370-2693(91)91677-N</ce:doi><ce:copyright type="unknown" year="1991"></ce:copyright></item-info><head><ce:title>A representation of the exchange relation for affine Toda field theory</ce:title><ce:author-group><ce:author><ce:given-name>E.</ce:given-name><ce:surname>Corrigan</ce:surname></ce:author><ce:affiliation><ce:textfn>Department of Mathematical Sciences, University of Durham, Durham DH1 3LE, UK</ce:textfn></ce:affiliation></ce:author-group><ce:author-group><ce:author><ce:given-name>P.E.</ce:given-name><ce:surname>Dorey</ce:surname></ce:author><ce:affiliation><ce:textfn>Service de Physique Théorique de Saclay<ce:cross-ref refid="FN1"><ce:sup>1</ce:sup></ce:cross-ref><ce:footnote id="FN1"><ce:label>1</ce:label><ce:note-para>Laboratoire de la Direction des Sciences de la Matière du Commissariat à l'Energie Atomique.</ce:note-para></ce:footnote>, F-91191 Gif-sur-Yvette Cedex, France</ce:textfn></ce:affiliation></ce:author-group><ce:date-received day="26" month="7" year="1991"></ce:date-received><ce:date-revised day="3" month="10" year="1991"></ce:date-revised><ce:abstract><ce:section-title>Abstract</ce:section-title><ce:abstract-sec><ce:simple-para>Vertex operators are constructed providing representations of the exchange relations containing either the <ce:italic>S</ce:italic>-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 <ce:italic>S</ce:italic>-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.</ce:simple-para></ce:abstract-sec></ce:abstract></head></converted-article></istex:document></istex:metadataXml><mods version="3.6"><titleInfo><title>A representation of the exchange relation for affine Toda field theory</title></titleInfo><titleInfo type="alternative" contentType="CDATA"><title>A representation of the exchange relation for affine Toda field theory</title></titleInfo><name type="personal"><namePart type="given">E.</namePart><namePart type="family">Corrigan</namePart><affiliation>Department of Mathematical Sciences, University of Durham, Durham DH1 3LE, UK</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">P.E.</namePart><namePart type="family">Dorey</namePart><affiliation>Service de Physique Théorique de Saclay, F-91191 Gif-sur-Yvette Cedex, France</affiliation><role><roleTerm type="text">author</roleTerm></role></name><typeOfResource>text</typeOfResource><genre type="research-article" displayLabel="Full-length article" authority="ISTEX" authorityURI="https://content-type.data.istex.fr" valueURI="https://content-type.data.istex.fr/ark:/67375/XTP-1JC4F85T-7">research-article</genre><originInfo><publisher>ELSEVIER</publisher><dateIssued encoding="w3cdtf">1991</dateIssued><dateModified encoding="w3cdtf">1991-10-03</dateModified><copyrightDate encoding="w3cdtf">1991</copyrightDate></originInfo><language><languageTerm type="code" authority="iso639-2b">eng</languageTerm><languageTerm type="code" authority="rfc3066">en</languageTerm></language><abstract lang="en">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.</abstract><relatedItem type="host"><titleInfo><title>Physics Letters B</title></titleInfo><titleInfo type="abbreviated"><title>PLB</title></titleInfo><genre type="journal" authority="ISTEX" authorityURI="https://publication-type.data.istex.fr" valueURI="https://publication-type.data.istex.fr/ark:/67375/JMC-0GLKJH51-B">journal</genre><originInfo><publisher>ELSEVIER</publisher><dateIssued encoding="w3cdtf">19911219</dateIssued></originInfo><identifier type="ISSN">0370-2693</identifier><identifier type="PII">S0370-2693(00)X1100-8</identifier><part><date>19911219</date><detail type="volume"><number>273</number><caption>vol.</caption></detail><detail type="issue"><number>3</number><caption>no.</caption></detail><extent unit="issue-pages"><start>193</start><end>366</end></extent><extent unit="pages"><start>237</start><end>245</end></extent></part></relatedItem><identifier type="istex">E23F8C08A8210700367F816B63648C576B8F7EA0</identifier><identifier type="ark">ark:/67375/6H6-RH2SK8SH-C</identifier><identifier type="DOI">10.1016/0370-2693(91)91677-N</identifier><identifier type="PII">0370-2693(91)91677-N</identifier><recordInfo><recordContentSource authority="ISTEX" authorityURI="https://loaded-corpus.data.istex.fr" valueURI="https://loaded-corpus.data.istex.fr/ark:/67375/XBH-HKKZVM7B-M">elsevier</recordContentSource></recordInfo></mods><json:item><extension>json</extension><original>false</original><mimetype>application/json</mimetype><uri>https://api.istex.fr/document/E23F8C08A8210700367F816B63648C576B8F7EA0/metadata/json</uri></json:item></metadata></istex></record>Pour manipuler ce document sous Unix (Dilib)
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