The Bernstein-Gelfand Tensor Product Functor and the Weight-2 Eisenstein Series

preprint2022arXivOpen access

Abstract

The Bernstein-Gelfand tensor product functors are endofunctors of the category of Harish-Chandra modules provided by tensor products with finite dimensional modules. We provide an automorphic analogue of these tensor product functors, implemented by vector-valued automorphic representations that are trivial at all finite places. They naturally explain the role of vector-valued modular forms in recent work by Bringmann-Kudla on Harish-Chandra modules associated with harmonic weak Maaß forms. We give a detailed account of the image sym1⊗ϖ(E2)\mathrm{sym}^1 \otimes \varpi(E_2) of the automorphic representation ϖ(E2)\varpi(E_2) generated by the Eisenstein series of weight 22 under one of those tensor product functors. This builds upon work by Roy-Schmidt-Yi, who recently determined the structure of ϖ(E2)\varpi(E_2). They found that ϖ(E2)\varpi(E_2) does not decompose as a restricted tensor product over all places of Q\mathbb{Q}, while we discover that sym1⊗ϖ(E2)\mathrm{sym}^1 \otimes \varpi(E_2) has a direct summand that does. This summand corresponds to a holomorphic and modular, vector-valued analogue of E2E_2. The complement in sym1⊗ϖ(E2)\mathrm{sym}^1 \otimes \varpi(E_2) arises from one of the vector-valued examples in the work of Bringmann-Kudla. Our approach allows us to determine its structure at the finite places.

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