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research article

Local monodromy of Drinfeld modules

Mornev, M.  
December 3, 2024
Compositio Mathematica

Compared with algebraic varieties the local monodromy of Drinfeld modules appears to be hopelessly complex: the image of the wild inertia subgroup under Tate module representations is infinite save for the case of potential good reduction. Nonetheless, we show that Tate modules of Drinfeld modules are ramified in a limited way: the image of a sufficiently deep ramification subgroup is trivial. This leads to a new invariant, the local conductor of a Drinfeld module. We establish an upper bound on the conductor in terms of the volume of the period lattice. As an intermediate step we develop a theory of normed lattices in function field arithmetic including the notion of volume. We relate normed lattices to vector bundles on projective curves. With the aid of Castelnuovo-Mumford regularity this implies a volume bound on norms of lattice generators, and the conductor inequality follows. Last but not least we describe the image of inertia for Drinfeld modules with period lattices of rank 1. Just as in the theory of local -adic pound Galois representations this image is commensurable with a commutative unipotent algebraic subgroup. However, in the case of Drinfeld modules such a subgroup can be a product of several copies of G(a) .

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Type
research article
DOI
10.1112/S0010437X24007450
Web of Science ID

WOS:001369171800001

Author(s)
Mornev, M.  

École Polytechnique Fédérale de Lausanne

Date Issued

2024-12-03

Publisher

CAMBRIDGE UNIV PRESS

Published in
Compositio Mathematica
Issue

11

Subjects

Drinfeld modules

•

Galois representations

•

Science & Technology

•

Physical Sciences

Editorial or Peer reviewed

REVIEWED

Written at

EPFL

EPFL units
TN  
FunderFunding(s)Grant NumberGrant URL

Swiss National Science Foundation (SNSF)

PZ00P2 202119

ETH Zurich Postdoctoral Fellowship

Available on Infoscience
January 27, 2025
Use this identifier to reference this record
https://infoscience.epfl.ch/handle/20.500.14299/245438
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