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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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Lenguaje: | eng |
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1993
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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. |
id | cern-246611 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1993 |
record_format | invenio |
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 |