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Where are the mirror manifolds?

The recent classification of Landau--Ginzburg potentials and their abelian symmetries focuses attention on a number of models with large positive Euler number for which no mirror partner is known. All of these models are related to Calabi--Yau manifolds in weighted $\IP_4$, with a characteristic str...

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Autor principal: Kreuzer, Maximilian
Lenguaje:eng
Publicado: 1993
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(93)91318-H
http://cds.cern.ch/record/246611
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author Kreuzer, Maximilian
author_facet Kreuzer, Maximilian
author_sort Kreuzer, Maximilian
collection CERN
description The recent classification of Landau--Ginzburg potentials and their abelian symmetries focuses attention on a number of models with large positive Euler number for which no mirror partner is known. All of these models are related to Calabi--Yau manifolds in weighted $\IP_4$, with a characteristic structure of the defining polynomials. A closer look at these potentials suggests a series of non-linear transformations, which relate the models to configurations for which a construction of the mirror is known, though only at certain points in moduli space. A special case of these transformations generalizes the $\ZZ_2$ orbifold representation of the $D$ invariant, implying a hidden symmetry in tensor products of minimal models.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1993
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spelling cern-2466112023-03-14T16:34:38Zdoi:10.1016/0370-2693(93)91318-Hhttp://cds.cern.ch/record/246611engKreuzer, MaximilianWhere are the mirror manifolds?Particle Physics - TheoryThe recent classification of Landau--Ginzburg potentials and their abelian symmetries focuses attention on a number of models with large positive Euler number for which no mirror partner is known. All of these models are related to Calabi--Yau manifolds in weighted $\IP_4$, with a characteristic structure of the defining polynomials. A closer look at these potentials suggests a series of non-linear transformations, which relate the models to configurations for which a construction of the mirror is known, though only at certain points in moduli space. A special case of these transformations generalizes the $\ZZ_2$ orbifold representation of the $D$ invariant, implying a hidden symmetry in tensor products of minimal models.The recent classification of Landau--Ginzburg potentials and their abelian symmetries focuses attention on a number of models with large positive Euler number for which no mirror partner is known. All of these models are related to Calabi--Yau manifolds in weighted $\IP_4$, with a characteristic structure of the defining polynomials. A closer look at these potentials suggests a series of non-linear transformations, which relate the models to configurations for which a construction of the mirror is known, though only at certain points in moduli space. A special case of these transformations generalizes the $\ZZ_2$ orbifold representation of the $D$ invariant, implying a hidden symmetry in tensor products of minimal models.The recent classification of Landau--Ginzburg potentials and their abelian symmetries focuses attention on a number of models with large positive Euler number for which no mirror partner is known. All of these models are related to Calabi--Yau manifolds in weighted $\IP_4$, with a characteristic structure of the defining polynomials. A closer look at these potentials suggests a series of non-linear transformations, which relate the models to configurations for which a construction of the mirror is known, though only at certain points in moduli space. A special case of these transformations generalizes the $\ZZ_2$ orbifold representation of the $D$ invariant, implying a hidden symmetry in tensor products of minimal models.The recent classification of Landau-Ginzburg potentials and their abelian symmetries focuses attention on a number of models with large positive Euler number for which no mirror partner is known. All of these models are related to Calabi-Yau manifolds in weighted P 4 , with a characteristic structure of the defining polynomials. A closer look at these potentials suggests a series of non-linear transformations, which relate the model to configurations for which a construction of the mirror is known, though only at certain points in moduli space. A special case of these transformations generalizes the Z 2 orbifold representation of the D invariant, implying a hidden symmetry in tensor products of minimal models.hep-th/9303015CERN-TH-6802-93CERN-TH-6802-93oai:cds.cern.ch:2466111993
spellingShingle Particle Physics - Theory
Kreuzer, Maximilian
Where are the mirror manifolds?
title Where are the mirror manifolds?
title_full Where are the mirror manifolds?
title_fullStr Where are the mirror manifolds?
title_full_unstemmed Where are the mirror manifolds?
title_short Where are the mirror manifolds?
title_sort where are the mirror manifolds?
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0370-2693(93)91318-H
http://cds.cern.ch/record/246611
work_keys_str_mv AT kreuzermaximilian wherearethemirrormanifolds