<p>We compute the first moment of cubic Hecke <i>L</i>-functions over <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {Q}(\sqrt{-3})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">Q</mi> <mo stretchy="false">(</mo> <msqrt> <mrow> <mo>-</mo> <mn>3</mn> </mrow> </msqrt> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> evaluated at any <i>s</i> inside the critical strip. The first moment for <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(s&lt;\frac{1}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>&lt;</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation> is particularly interesting, and we show there is a phase transition at <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(s=\frac{1}{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>=</mo> <mfrac> <mn>1</mn> <mn>3</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. This extends the analogue result of David and Meisner (Trans Am Math Soc 378:5125–5157. <a href="https://doi.org/10.1090/tran/9428">https://doi.org/10.1090/tran/9428</a>, 2025) for the first moment over function fields. As in their work, the computation of the moment at <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(s=\frac{1}{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>=</mo> <mfrac> <mn>1</mn> <mn>3</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation> relies on a cancellation between two terms which are a priori not related: a main term of the principal sum which comes from cubes, and the contribution from infinitely many residues of Dirichlet series of cubic Gauss sums to the dual sum. The cancellation also improves the error term and exhibits a secondary term for all <i>s</i>. In particular, at <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(s=\frac{1}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>=</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, we prove the existence of a secondary term of size <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(Q^{5/6}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>Q</mi> <mrow> <mn>5</mn> <mo stretchy="false">/</mo> <mn>6</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>, where the size of the family is <i>Q</i>. We conjecture that a similar behaviour would hold for higher order Hecke <i>L</i>-functions attached to <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ℓ</mi> </math></EquationSource> </InlineEquation>th order residue symbols, refining a function field conjecture of David and Meisner. The proof follows the steps of writing <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(L(s,\chi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo>,</mo> <mi>χ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> as two finite sums with the approximate functional equation. Two main ingredients are then exploited: the bound on the second moment of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(L(1/2+it,\chi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>L</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> <mo>+</mo> <mi>i</mi> <mi>t</mi> <mo>,</mo> <mi>χ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> that follows from Heath–Brown’s cubic large sieve, and the deep work of Kubota and Patterson which connects the Dirichlet series of cubic Gauss sums to metaplectic forms, and gives a formula for its residues in terms of the Fourier coefficients of metaplectic theta functions.</p>

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Hecke L-functions away from the central line

  • Mohammad H. Hamdar

摘要

We compute the first moment of cubic Hecke L-functions over \(\mathbb {Q}(\sqrt{-3})\) Q ( - 3 ) evaluated at any s inside the critical strip. The first moment for \(s<\frac{1}{2}\) s < 1 2 is particularly interesting, and we show there is a phase transition at \(s=\frac{1}{3}\) s = 1 3 . This extends the analogue result of David and Meisner (Trans Am Math Soc 378:5125–5157. https://doi.org/10.1090/tran/9428, 2025) for the first moment over function fields. As in their work, the computation of the moment at \(s=\frac{1}{3}\) s = 1 3 relies on a cancellation between two terms which are a priori not related: a main term of the principal sum which comes from cubes, and the contribution from infinitely many residues of Dirichlet series of cubic Gauss sums to the dual sum. The cancellation also improves the error term and exhibits a secondary term for all s. In particular, at \(s=\frac{1}{2}\) s = 1 2 , we prove the existence of a secondary term of size \(Q^{5/6}\) Q 5 / 6 , where the size of the family is Q. We conjecture that a similar behaviour would hold for higher order Hecke L-functions attached to \(\ell \) th order residue symbols, refining a function field conjecture of David and Meisner. The proof follows the steps of writing \(L(s,\chi )\) L ( s , χ ) as two finite sums with the approximate functional equation. Two main ingredients are then exploited: the bound on the second moment of \(L(1/2+it,\chi )\) L ( 1 / 2 + i t , χ ) that follows from Heath–Brown’s cubic large sieve, and the deep work of Kubota and Patterson which connects the Dirichlet series of cubic Gauss sums to metaplectic forms, and gives a formula for its residues in terms of the Fourier coefficients of metaplectic theta functions.