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On field redefinitions and exact solutions in string theory
String backgrounds associated with gauged $G/H$ WZNW models in general depend non-trivially on $\alpha'$. We note, however, that there exists a local covariant $\a'$-dependent field redefinition that relates the exact metric-dilaton background corresponding to the $SL(2,R)/U(1)$ model to i...
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Lenguaje: | eng |
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1993
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Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(93)91372-T http://cds.cern.ch/record/252574 |
_version_ | 1780885624558977024 |
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author | Tseytlin, Arkady A. |
author_facet | Tseytlin, Arkady A. |
author_sort | Tseytlin, Arkady A. |
collection | CERN |
description | String backgrounds associated with gauged $G/H$ WZNW models in general depend non-trivially on $\alpha'$. We note, however, that there exists a local covariant $\a'$-dependent field redefinition that relates the exact metric-dilaton background corresponding to the $SL(2,R)/U(1)$ model to its leading-order form ($D=2$ black hole). As a consequence, there exists a `scheme' in which the string effective equations have the latter as an exact solution. However, the corresponding equation for the tachyon (which, like other Weyl anomaly coefficients, has scheme-dependent form) still contains corrections of all orders in $\alpha'$. As a result, the `probes' (the tachyons) still feel the $\alpha'$-corrected background. The field redefinitions we discuss contain the dilaton terms in the metric transformation law. We comment on exact forms of the duality transformation in different `schemes'. |
id | cern-252574 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1993 |
record_format | invenio |
spelling | cern-2525742023-03-14T18:52:30Zdoi:10.1016/0370-2693(93)91372-Thttp://cds.cern.ch/record/252574engTseytlin, Arkady A.On field redefinitions and exact solutions in string theoryParticle Physics - TheoryGeneral Theoretical PhysicsString backgrounds associated with gauged $G/H$ WZNW models in general depend non-trivially on $\alpha'$. We note, however, that there exists a local covariant $\a'$-dependent field redefinition that relates the exact metric-dilaton background corresponding to the $SL(2,R)/U(1)$ model to its leading-order form ($D=2$ black hole). As a consequence, there exists a `scheme' in which the string effective equations have the latter as an exact solution. However, the corresponding equation for the tachyon (which, like other Weyl anomaly coefficients, has scheme-dependent form) still contains corrections of all orders in $\alpha'$. As a result, the `probes' (the tachyons) still feel the $\alpha'$-corrected background. The field redefinitions we discuss contain the dilaton terms in the metric transformation law. We comment on exact forms of the duality transformation in different `schemes'.String backgrounds associated with gauged $G/H$ WZNW models in general depend non-trivially on $\alpha'$. We note, however, that there exists a local covariant $\a'$-dependent field redefinition that relates the exact metric-dilaton background corresponding to the $SL(2,R)/U(1)$ model to its leading-order form ($D=2$ black hole). As a consequence, there exists a `scheme' in which the string effective equations have the latter as an exact solution. The field redefinitions we discuss contain the dilaton terms in the metric transformation law. We also comment on exact forms of duality transformation in different `schemes'.String backgrounds associated with gauged $G/H$ WZNW models in general depend non-trivially on $\alpha'$. We note, however, that there exists a local covariant $\a'$-dependent field redefinition that relates the exact metric-dilaton background corresponding to the $SL(2,R)/U(1)$ model to its leading-order form ($D=2$ black hole). As a consequence, there exists a `scheme' in which the string effective equations have the latter as an exact solution. The field redefinitions we discuss contain the dilaton terms in the metric transformation law. We also comment on exact forms of duality transformation in different `schemes'.String backgrounds associated with gauged $G/H$ WZNW models in general depend non-trivially on $\alpha'$. We note, however, that there exists a local covariant $\a'$-dependent field redefinition that relates the exact metric-dilaton background corresponding to the $SL(2,R)/U(1)$ model to its leading-order form ($D=2$ black hole). As a consequence, there exists a `scheme' in which the string effective equations have the latter as an exact solution. The field redefinitions we discuss contain the dilaton terms in the metric transformation law. We also comment on exact forms of duality transformation in different `schemes'.String backgrounds associated with gauged $G/H$ WZNW models in general depend non-trivially on $\alpha'$. We note, however, that there exists a local covariant $\a'$-dependent field redefinition that relates the exact metric-dilaton background corresponding to the $SL(2,R)/U(1)$ model to its leading-order form ($D=2$ black hole). As a consequence, there exists a `scheme' in which the string effective equations have the latter as an exact solution. The field redefinitions we discuss contain the dilaton terms in the metric transformation law. We also comment on exact forms of duality transformation in different `schemes'.String backgrounds associated with gauged G/H WZNW models in general depend nontrivially on α′. We note, however that there exists a local covariant α′ -dependent field redefinition that relates the exact metric-dilaton background corresponding to the SL(2, R )/U(1) model to its leading-order form ( D =2 black hole). As a consequence, there exists a “scheme” in which the string effective equations have the latter as an exact solution. However, the corresponding dquation for the tachyon (which, like other Weyl anomaly equations, has scheme-dependent form) still contains corrections of all orders in α′. As a result, the string “probes” still feel the α′ -corrected background. The field redefinitions we discuss contain the dilaton terms in the metric transformation law. We also comment on exact forms of the duality transformation in different “schemes”.hep-th/9308042CERN-TH-6970-93CERN-TH-6970-93oai:cds.cern.ch:2525741993 |
spellingShingle | Particle Physics - Theory General Theoretical Physics Tseytlin, Arkady A. On field redefinitions and exact solutions in string theory |
title | On field redefinitions and exact solutions in string theory |
title_full | On field redefinitions and exact solutions in string theory |
title_fullStr | On field redefinitions and exact solutions in string theory |
title_full_unstemmed | On field redefinitions and exact solutions in string theory |
title_short | On field redefinitions and exact solutions in string theory |
title_sort | on field redefinitions and exact solutions in string theory |
topic | Particle Physics - Theory General Theoretical Physics |
url | https://dx.doi.org/10.1016/0370-2693(93)91372-T http://cds.cern.ch/record/252574 |
work_keys_str_mv | AT tseytlinarkadya onfieldredefinitionsandexactsolutionsinstringtheory |