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A search for exact superstring vacua
We investigate $2d$ sigma-models with a $2+N$ dimensional Minkowski signature target space metric and Killing symmetry, specifically supersymmetrized, and see under which conditions they might lead to corresponding exact string vacua. It appears that the issue relies heavily on the properties of the...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1994
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Acceso en línea: | https://dx.doi.org/10.1007/BF02781563 http://cds.cern.ch/record/252571 |
_version_ | 1780885624115429376 |
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author | Peterman, A. Zichichi, A. |
author_facet | Peterman, A. Zichichi, A. |
author_sort | Peterman, A. |
collection | CERN |
description | We investigate $2d$ sigma-models with a $2+N$ dimensional Minkowski signature target space metric and Killing symmetry, specifically supersymmetrized, and see under which conditions they might lead to corresponding exact string vacua. It appears that the issue relies heavily on the properties of the vector $M_{\mu}$, a reparametrization term, which needs to possess a definite form for the Weyl invariance to be satisfied. We give, in the $n = 1$ supersymmetric case, two non-renormalization theorems from which we can relate the $u$ component of $M_{\mu}$ to the $\beta^G_{uu}$ function. We work out this $(u,u)$ component of the $\beta^G$ function and find a non-vanishing contribution at four loops. Therefore, it turns out that at order $\alpha^{\prime 4}$, there are in general non-vanishing contributions to $M_u$ that prevent us from deducing superstring vacua in closed form. |
id | cern-252571 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1994 |
record_format | invenio |
spelling | cern-2525712020-07-23T02:47:52Zdoi:10.1007/BF02781563http://cds.cern.ch/record/252571engPeterman, A.Zichichi, A.A search for exact superstring vacuaGeneral Theoretical PhysicsWe investigate $2d$ sigma-models with a $2+N$ dimensional Minkowski signature target space metric and Killing symmetry, specifically supersymmetrized, and see under which conditions they might lead to corresponding exact string vacua. It appears that the issue relies heavily on the properties of the vector $M_{\mu}$, a reparametrization term, which needs to possess a definite form for the Weyl invariance to be satisfied. We give, in the $n = 1$ supersymmetric case, two non-renormalization theorems from which we can relate the $u$ component of $M_{\mu}$ to the $\beta^G_{uu}$ function. We work out this $(u,u)$ component of the $\beta^G$ function and find a non-vanishing contribution at four loops. Therefore, it turns out that at order $\alpha^{\prime 4}$, there are in general non-vanishing contributions to $M_u$ that prevent us from deducing superstring vacua in closed form.We investigate $2d$ sigma-models with a $2+N$ dimensional Minkowski signature target space metric and Killing symmetry, specifically supersymmetrized, and see under which conditions they might lead to corresponding exact string vacua. It appears that the issue relies heavily on the properties of the vector $M_{\mu}$, a reparametrization term, which needs to possess a definite form for the Weyl invariance to be satisfied. We give, in the $n = 1$ supersymmetric case, two non-renormalization theorems from which we can relate the $u$ component of $M_{\mu}$ to the $\beta~G_{uu}$ function. We work out this $(u,u)$ component of the $\beta~G$ function and find a non-vanishing contribution at four loops. Therefore, it turns out that at order $\alpha~{\prime 4}$, there are in general non-vanishing contributions to $M_u$ that prevent us from deducing superstring vacua in closed form.We investigate 2d σ-models with a (2 +N)-dimensional Minkowski signature target space metric and Killing symmetry, specifically supersymmetrized, and see under which conditions they might lead to corresponding exact string vacua. It appears that the issue relies heavily on the properties of the vectorMμ, a reparametrization term, which needs to possess a definite form for the Weyl invariance to be satisfied. We give, in then = 1 supersymmetric case, two non-renormalization theorems from which we can relate theu component ofMμ to the βuuG function. We work out this(u, u) component of the ΒG function and find a non-vanishing contribution at four loops. Therefore, it turns out that at order α′4, there are in general non-vanishing contributions toMu that prevent us from deducing superstring vacua in closed form.hep-th/9308108CERN-TH-6946-93CERN-LAA-93-23CERN-LAA-93-23CERN-TH-6946-93oai:cds.cern.ch:2525711994 |
spellingShingle | General Theoretical Physics Peterman, A. Zichichi, A. A search for exact superstring vacua |
title | A search for exact superstring vacua |
title_full | A search for exact superstring vacua |
title_fullStr | A search for exact superstring vacua |
title_full_unstemmed | A search for exact superstring vacua |
title_short | A search for exact superstring vacua |
title_sort | search for exact superstring vacua |
topic | General Theoretical Physics |
url | https://dx.doi.org/10.1007/BF02781563 http://cds.cern.ch/record/252571 |
work_keys_str_mv | AT petermana asearchforexactsuperstringvacua AT zichichia asearchforexactsuperstringvacua AT petermana searchforexactsuperstringvacua AT zichichia searchforexactsuperstringvacua |