Compactified D =1 string models
Identifieur interne : 002100 ( Main/Exploration ); précédent : 002099; suivant : 002101Compactified D =1 string models
Auteurs : Z. Yang [États-Unis]Source :
- Physics Letters B [ 0370-2693 ] ; 1990.
English descriptors
- Teeft :
- Angular part, Compactified, Compactified space, Continuum limit, Critical dimension, Critical dimensions, Critical string, Critical strings, Different behaviors, Ground state, Ground state energy, Hagedorn temperature, July, Lett, Liouville, Liouville action, Liouville mode, Liouville string, Liouville theory, Liouviue action, Matrix, Matrix model, Nucl, Partition function, Phase transition, Phase transition point, Phys, Physical picture, Physics letters, Physics lettersb, Random matrix model, Soliton sector, Statistical mechanics, String theory, Theory group, Vortex, World sheet.
Abstract
Abstract: We study compactification and BKT phase transition in the context of the D=1 string. We first present as our motivation a scenario in the critical string. When the radius R of the compactified space is smaller than the critical value Rc, the BKT transition results in the elimination of the compactified coordinate as a dynamical variable and consequently the Liouville mode comes in. Many questions concerning this scenario are answered by considering the compactified D=1 random matrix model, which can be solved in large and small radius limits. The occurrence of a BKT phase transition between them is argued through the compactified D=1 Liouville theory.
Url:
DOI: 10.1016/0370-2693(90)91398-U
Affiliations:
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Le document en format XML
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<front><div type="abstract" xml:lang="en">Abstract: We study compactification and BKT phase transition in the context of the D=1 string. We first present as our motivation a scenario in the critical string. When the radius R of the compactified space is smaller than the critical value Rc, the BKT transition results in the elimination of the compactified coordinate as a dynamical variable and consequently the Liouville mode comes in. Many questions concerning this scenario are answered by considering the compactified D=1 random matrix model, which can be solved in large and small radius limits. The occurrence of a BKT phase transition between them is argued through the compactified D=1 Liouville theory.</div>
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