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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...

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Detalles Bibliográficos
Autores principales: Peterman, A., Zichichi, A.
Lenguaje:eng
Publicado: 1994
Materias:
Acceso en línea:https://dx.doi.org/10.1007/BF02781563
http://cds.cern.ch/record/252571
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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.
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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
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