<p>We prove strong hybrid subconvex bounds simultaneously in the <i>q</i> and <i>t</i> aspects for <i>L</i>-functions of selfdual <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({{\,\textrm{GL}\,}}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> cusp forms twisted by primitive Dirichlet characters. We additionally prove analogous hybrid subconvex bounds for central values of certain <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({{\,\textrm{GL}\,}}_3 \times {{\,\textrm{GL}\,}}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>3</mn> </msub> <mo>×</mo> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> Rankin–Selberg <i>L</i>-functions. The subconvex bounds that we obtain are strong in the sense that, modulo current knowledge on estimates for the second moment of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({{\,\textrm{GL}\,}}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>3</mn> </msub> </math></EquationSource> </InlineEquation> <i>L</i>-functions, they are the natural limit of the first moment method pioneered by Li and by Blomer. The method of proof relies on an explicit <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({{\,\textrm{GL}\,}}_3 \times {{\,\textrm{GL}\,}}_2 \leftrightsquigarrow \leftrightsquigarrow {{\,\textrm{GL}\,}}_4 \times {{\,\textrm{GL}\,}}_1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>3</mn> </msub> <mo>×</mo> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>2</mn> </msub> <mo>↭</mo> <mo>↭</mo> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>4</mn> </msub> <mo>×</mo> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>1</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> spectral reciprocity formula, which relates a <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({{\,\textrm{GL}\,}}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> moment of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({{\,\textrm{GL}\,}}_3 \times {{\,\textrm{GL}\,}}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>3</mn> </msub> <mo>×</mo> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> Rankin–Selberg <i>L</i>-functions to a <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\({{\,\textrm{GL}\,}}_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> moment of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\({{\,\textrm{GL}\,}}_4 \times {{\,\textrm{GL}\,}}_1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>4</mn> </msub> <mo>×</mo> <msub> <mrow> <mspace width="0.166667em" /> <mtext>GL</mtext> <mspace width="0.166667em" /> </mrow> <mn>1</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> Rankin–Selberg <i>L</i>-functions. A key additional input is a Lindelöf-on-average upper bound for the second moment of Dirichlet <i>L</i>-functions restricted to a coset, which is of independent interest.</p>

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Strong hybrid subconvexity for twisted selfdual \({\text {GL}}_3\) L-functions

  • Soumendra Ganguly,
  • Peter Humphries,
  • Yongxiao Lin,
  • Ramon Nunes

摘要

We prove strong hybrid subconvex bounds simultaneously in the q and t aspects for L-functions of selfdual \({{\,\textrm{GL}\,}}_3\) GL 3 cusp forms twisted by primitive Dirichlet characters. We additionally prove analogous hybrid subconvex bounds for central values of certain \({{\,\textrm{GL}\,}}_3 \times {{\,\textrm{GL}\,}}_2\) GL 3 × GL 2 Rankin–Selberg L-functions. The subconvex bounds that we obtain are strong in the sense that, modulo current knowledge on estimates for the second moment of \({{\,\textrm{GL}\,}}_3\) GL 3 L-functions, they are the natural limit of the first moment method pioneered by Li and by Blomer. The method of proof relies on an explicit \({{\,\textrm{GL}\,}}_3 \times {{\,\textrm{GL}\,}}_2 \leftrightsquigarrow \leftrightsquigarrow {{\,\textrm{GL}\,}}_4 \times {{\,\textrm{GL}\,}}_1\) GL 3 × GL 2 GL 4 × GL 1 spectral reciprocity formula, which relates a \({{\,\textrm{GL}\,}}_2\) GL 2 moment of \({{\,\textrm{GL}\,}}_3 \times {{\,\textrm{GL}\,}}_2\) GL 3 × GL 2 Rankin–Selberg L-functions to a \({{\,\textrm{GL}\,}}_1\) GL 1 moment of \({{\,\textrm{GL}\,}}_4 \times {{\,\textrm{GL}\,}}_1\) GL 4 × GL 1 Rankin–Selberg L-functions. A key additional input is a Lindelöf-on-average upper bound for the second moment of Dirichlet L-functions restricted to a coset, which is of independent interest.