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Quartic Gauge Couplings from $K$3 Geometry

We show how certain F^4 couplings in eight dimensions can be computed using the mirror map and K3 data. They perfectly match with the corresponding heterotic one-loop couplings, and therefore this amounts to a successful test of the conjectured duality between the heterotic string on T^2 and F-theor...

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Detalles Bibliográficos
Autores principales: Lerche, W., Stieberger, S., Warner, N.P.
Lenguaje:eng
Publicado: 1998
Materias:
Acceso en línea:https://dx.doi.org/10.4310/ATMP.1999.v3.n5.a8
http://cds.cern.ch/record/372458
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author Lerche, W.
Stieberger, S.
Warner, N.P.
author_facet Lerche, W.
Stieberger, S.
Warner, N.P.
author_sort Lerche, W.
collection CERN
description We show how certain F^4 couplings in eight dimensions can be computed using the mirror map and K3 data. They perfectly match with the corresponding heterotic one-loop couplings, and therefore this amounts to a successful test of the conjectured duality between the heterotic string on T^2 and F-theory on K3. The underlying quantum geometry appears to be a 5-fold, consisting of a hyperk"ahler 4-fold fibered over a IP^1 base. The natural candidate for this fiber is the symmetric product Sym^2(K3). We are lead to this structure by analyzing the implications of higher powers of E_2 in the relevant Borcherds counting functions, and in particular the appropriate generalizations of the Picard-Fuchs equations for the K3.
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spelling cern-3724582023-03-14T17:10:48Zdoi:10.4310/ATMP.1999.v3.n5.a8http://cds.cern.ch/record/372458engLerche, W.Stieberger, S.Warner, N.P.Quartic Gauge Couplings from $K$3 GeometryParticle Physics - TheoryWe show how certain F^4 couplings in eight dimensions can be computed using the mirror map and K3 data. They perfectly match with the corresponding heterotic one-loop couplings, and therefore this amounts to a successful test of the conjectured duality between the heterotic string on T^2 and F-theory on K3. The underlying quantum geometry appears to be a 5-fold, consisting of a hyperk"ahler 4-fold fibered over a IP^1 base. The natural candidate for this fiber is the symmetric product Sym^2(K3). We are lead to this structure by analyzing the implications of higher powers of E_2 in the relevant Borcherds counting functions, and in particular the appropriate generalizations of the Picard-Fuchs equations for the K3.hep-th/9811228CERN-TH-98-378CERN-TH-98-378oai:cds.cern.ch:3724581998-11-27
spellingShingle Particle Physics - Theory
Lerche, W.
Stieberger, S.
Warner, N.P.
Quartic Gauge Couplings from $K$3 Geometry
title Quartic Gauge Couplings from $K$3 Geometry
title_full Quartic Gauge Couplings from $K$3 Geometry
title_fullStr Quartic Gauge Couplings from $K$3 Geometry
title_full_unstemmed Quartic Gauge Couplings from $K$3 Geometry
title_short Quartic Gauge Couplings from $K$3 Geometry
title_sort quartic gauge couplings from $k$3 geometry
topic Particle Physics - Theory
url https://dx.doi.org/10.4310/ATMP.1999.v3.n5.a8
http://cds.cern.ch/record/372458
work_keys_str_mv AT lerchew quarticgaugecouplingsfromk3geometry
AT stiebergers quarticgaugecouplingsfromk3geometry
AT warnernp quarticgaugecouplingsfromk3geometry