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The exact mass-gap of the supersymmetric O(N) sigma model
A formula for the mass-gap of the supersymmetric O(N) sigma model (N>4) in two dimensions is derived: m/\Lambda_{\overline{\rm MS}}=2^{2\Delta}\sin(\pi\Delta)/(\pi\Delta), where \Delta=1/(N-2) and m is the mass of the fundamental vector particle in the theory. This result is obtained by comparing...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1994
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Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(94)01477-T http://cds.cern.ch/record/269235 |
_version_ | 1780886961937973248 |
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author | Evans, Jonathan M. Hollowood, Timothy J. |
author_facet | Evans, Jonathan M. Hollowood, Timothy J. |
author_sort | Evans, Jonathan M. |
collection | CERN |
description | A formula for the mass-gap of the supersymmetric O(N) sigma model (N>4) in two dimensions is derived: m/\Lambda_{\overline{\rm MS}}=2^{2\Delta}\sin(\pi\Delta)/(\pi\Delta), where \Delta=1/(N-2) and m is the mass of the fundamental vector particle in the theory. This result is obtained by comparing two expressions for the free-energy density in the presence of a coupling to a conserved charge; one expression is computed from the exact S-matrix of Shankar and Witten via the the thermodynamic Bethe ansatz and the other is computed using conventional perturbation theory. These calculations provide a stringent test of the S-matrix, showing that it correctly reproduces the universal part of the beta-function and resolving the problem of CDD ambiguities. |
id | cern-269235 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1994 |
record_format | invenio |
spelling | cern-2692352023-03-14T16:36:01Zdoi:10.1016/0370-2693(94)01477-Thttp://cds.cern.ch/record/269235engEvans, Jonathan M.Hollowood, Timothy J.The exact mass-gap of the supersymmetric O(N) sigma modelGeneral Theoretical PhysicsA formula for the mass-gap of the supersymmetric O(N) sigma model (N>4) in two dimensions is derived: m/\Lambda_{\overline{\rm MS}}=2^{2\Delta}\sin(\pi\Delta)/(\pi\Delta), where \Delta=1/(N-2) and m is the mass of the fundamental vector particle in the theory. This result is obtained by comparing two expressions for the free-energy density in the presence of a coupling to a conserved charge; one expression is computed from the exact S-matrix of Shankar and Witten via the the thermodynamic Bethe ansatz and the other is computed using conventional perturbation theory. These calculations provide a stringent test of the S-matrix, showing that it correctly reproduces the universal part of the beta-function and resolving the problem of CDD ambiguities.A formula for the mass-gap of the supersymmetric O($N$) sigma model ($N>4$) in two dimensions is derived: $m/\Lambda_{\overline{\rm MS}}=2~{2\Delta}\sin(\pi\Delta)/(\pi\Delta)$, where $\Delta=1/(N-2)$ and $m$ is the mass of the fundamental vector particle in the theory. This result is obtained by comparing two expressions for the free-energy density in the presence of a coupling to a conserved charge; one expression is computed from the exact S-matrix of Shankar and Witten via the the thermodynamic Bethe ansatz and the other is computed using conventional perturbation theory. These calculations provide a stringent test of the S-matrix, showing that it correctly reproduces the universal part of the beta-function and resolving the problem of CDD ambiguities.A formula for the mass-gap of the supersymmetric O( N ) sigma model ( N > 4) in two dimensions is derived: m Λ MS =2 2Δ sin (πΔ) (πΔ) , where Δ = 1 (N−2) and m is the mass of the fundamental vector particle in the theory. This result is obtained by comparing two expressions for the free-energy density in the presence of a coupling to a conserved charge; one expression is computed from the exact S-matrix of Shankar and Witten via the thermodynamic Bethe ansatz and the other is computed using conventional perturbation theory. These calculations a provide a stringent test of the S-maxtrix, showing that it correctly reproduces the universal part of the beta-functional and resolving the problem of CDD ambiguities.hep-th/9409141CERN-TH-7425-94SWAT-93-94-39CERN-TH-7425-94SWAT-39oai:cds.cern.ch:2692351994-09-23 |
spellingShingle | General Theoretical Physics Evans, Jonathan M. Hollowood, Timothy J. The exact mass-gap of the supersymmetric O(N) sigma model |
title | The exact mass-gap of the supersymmetric O(N) sigma model |
title_full | The exact mass-gap of the supersymmetric O(N) sigma model |
title_fullStr | The exact mass-gap of the supersymmetric O(N) sigma model |
title_full_unstemmed | The exact mass-gap of the supersymmetric O(N) sigma model |
title_short | The exact mass-gap of the supersymmetric O(N) sigma model |
title_sort | exact mass-gap of the supersymmetric o(n) sigma model |
topic | General Theoretical Physics |
url | https://dx.doi.org/10.1016/0370-2693(94)01477-T http://cds.cern.ch/record/269235 |
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