Young's square-root shifted convolution conjecture for Maass forms

Let U(z)U(z) be a Hecke–Maass cusp form with Laplace eigenvalue 1/4+T21/4+T^2, Fourier coefficients λ(n)\lambda(n) and first coefficient ρ(1)\rho(1). For fixed 0<ayb0<a\le y\le b, αR\alpha\in\mathbb{R}, and 1MT1+ε1\le M\le T^{1+\varepsilon}, Young's square-root shifted convolution conjecture.

ρ(1)21mMe(mα)nZλ(n)λ(n+m)KiT(2πny)KiT(2πm+ny)a,b,εT1/2+εM1/2.|\rho(1)|^2\sum_{1\le|m|\le M}e(m\alpha)\sum_{n\in\mathbb{Z}}\lambda(n)\lambda(n+m)K_{iT}(2\pi|n|y)K_{iT}(2\pi|m+n|y)\ll_{a,b,\varepsilon}T^{-1/2+\varepsilon}M^{1/2}.

Equivalently, uniformly in αR\alpha\in\mathbb{R},

1mM01U(x+iy)2e(m(αx))dxa,b,εT1/2+εM1/2.\sum_{1\le|m|\le M}\int_0^1|U(x+iy)|^2e(m(\alpha-x))\,dx\ll_{a,b,\varepsilon}T^{-1/2+\varepsilon}M^{1/2}.

This stronger hypothesis supplies cancellation across the shift mm and would imply the conjectural compact-set sup-norm bound U(z)TεU(z)\ll T^\varepsilon.

Sources & referencesView supporting material

Primary source

Matthew P. Young, “The quantum unique ergodicity conjecture for thin sets”, arXiv:1306.1554 (2013).

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