Completing the eclectic flavor scheme of the ℤ2 orbifold

Abstract We present a detailed analysis of the eclectic flavor structure of the two-dimensional ℤ2 orbifold with its two unconstrained moduli T and U as well as SL(2, ℤ) T × SL(2, ℤ) U modular symmetry. This provides a thorough understanding of mirror symmetry as well as the R-symmetries that appear...

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Main Authors: Alexander Baur, Moritz Kade, Hans Peter Nilles, Saúl Ramos-Sánchez, Patrick K. S. Vaudrevange
Format: Article
Language:English
Published: SpringerOpen 2021-06-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP06(2021)110
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spelling doaj-1061574bd97f4cef9e0ef2356ce773b52021-06-20T11:06:57ZengSpringerOpenJournal of High Energy Physics1029-84792021-06-012021614510.1007/JHEP06(2021)110Completing the eclectic flavor scheme of the ℤ2 orbifoldAlexander Baur0Moritz Kade1Hans Peter Nilles2Saúl Ramos-Sánchez3Patrick K. S. Vaudrevange4Physik Department T75, Technische Universität MünchenPhysik Department T75, Technische Universität MünchenBethe Center for Theoretical Physics and Physikalisches Institut der Universität BonnInstituto de Física, Universidad Nacional Autónoma de MéxicoPhysik Department T75, Technische Universität MünchenAbstract We present a detailed analysis of the eclectic flavor structure of the two-dimensional ℤ2 orbifold with its two unconstrained moduli T and U as well as SL(2, ℤ) T × SL(2, ℤ) U modular symmetry. This provides a thorough understanding of mirror symmetry as well as the R-symmetries that appear as a consequence of the automorphy factors of modular transformations. It leads to a complete picture of local flavor unification in the (T, U) modulus landscape. In view of applications towards the flavor structure of particle physics models, we are led to top-down constructions with high predictive power. The first reason is the very limited availability of flavor representations of twisted matter fields as well as their (fixed) modular weights. This is followed by severe restrictions from traditional and (finite) modular flavor symmetries, mirror symmetry, CP $$ \mathcal{CP} $$ and R-symmetries on the superpotential and Kähler potential of the theory.https://doi.org/10.1007/JHEP06(2021)110Compactification and String ModelsDiscrete SymmetriesField Theories in Higher DimensionsSuperstrings and Heterotic Strings
collection DOAJ
language English
format Article
sources DOAJ
author Alexander Baur
Moritz Kade
Hans Peter Nilles
Saúl Ramos-Sánchez
Patrick K. S. Vaudrevange
spellingShingle Alexander Baur
Moritz Kade
Hans Peter Nilles
Saúl Ramos-Sánchez
Patrick K. S. Vaudrevange
Completing the eclectic flavor scheme of the ℤ2 orbifold
Journal of High Energy Physics
Compactification and String Models
Discrete Symmetries
Field Theories in Higher Dimensions
Superstrings and Heterotic Strings
author_facet Alexander Baur
Moritz Kade
Hans Peter Nilles
Saúl Ramos-Sánchez
Patrick K. S. Vaudrevange
author_sort Alexander Baur
title Completing the eclectic flavor scheme of the ℤ2 orbifold
title_short Completing the eclectic flavor scheme of the ℤ2 orbifold
title_full Completing the eclectic flavor scheme of the ℤ2 orbifold
title_fullStr Completing the eclectic flavor scheme of the ℤ2 orbifold
title_full_unstemmed Completing the eclectic flavor scheme of the ℤ2 orbifold
title_sort completing the eclectic flavor scheme of the ℤ2 orbifold
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-06-01
description Abstract We present a detailed analysis of the eclectic flavor structure of the two-dimensional ℤ2 orbifold with its two unconstrained moduli T and U as well as SL(2, ℤ) T × SL(2, ℤ) U modular symmetry. This provides a thorough understanding of mirror symmetry as well as the R-symmetries that appear as a consequence of the automorphy factors of modular transformations. It leads to a complete picture of local flavor unification in the (T, U) modulus landscape. In view of applications towards the flavor structure of particle physics models, we are led to top-down constructions with high predictive power. The first reason is the very limited availability of flavor representations of twisted matter fields as well as their (fixed) modular weights. This is followed by severe restrictions from traditional and (finite) modular flavor symmetries, mirror symmetry, CP $$ \mathcal{CP} $$ and R-symmetries on the superpotential and Kähler potential of the theory.
topic Compactification and String Models
Discrete Symmetries
Field Theories in Higher Dimensions
Superstrings and Heterotic Strings
url https://doi.org/10.1007/JHEP06(2021)110
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