<p>Let <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42543_2025_111_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {Mp}(2n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>Mp</mtext> <mo stretchy="false">(</mo> <mn>2</mn> <mi>n</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> be the metaplectic group over a local field <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42543_2025_111_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(F \supset \mathbb {Q}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>F</mi> <mo>⊃</mo> <msub> <mi mathvariant="double-struck">Q</mi> <mi>p</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> defined by an additive character of <i>F</i> of conductor <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42543_2025_111_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(4{\mathfrak {o}}_F\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>4</mn> <msub> <mi mathvariant="fraktur">o</mi> <mi>F</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>. Gan–Savin (<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42543_2025_111_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(p \ne 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>≠</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>) and Takeda–Wood (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42543_2025_111_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(p=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>) obtained an equivalence between the Bernstein block of <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42543_2025_111_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {Mp}(2n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>Mp</mtext> <mo stretchy="false">(</mo> <mn>2</mn> <mi>n</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> containing the even (resp. odd) Weil representation and the Iwahori-spherical block of the split <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42543_2025_111_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="81" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {SO}(2n+1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>SO</mtext> <mo stretchy="false">(</mo> <mn>2</mn> <mi>n</mi> <mo>+</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> (resp. its non-split inner form), by giving an isomorphism between Hecke algebras. We revisit this equivalence from an endoscopic perspective. It turns out that the L-parameters of irreducible representations are preserved, whilst the difference between characters of component groups is governed by symplectic local root numbers.</p>

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Spectral Transfer for Metaplectic Groups. II. Hecke Algebra Correspondences

  • Fei Chen,
  • Wen-Wei Li

摘要

Let \(\text {Mp}(2n)\) Mp ( 2 n ) be the metaplectic group over a local field \(F \supset \mathbb {Q}_p\) F Q p defined by an additive character of F of conductor \(4{\mathfrak {o}}_F\) 4 o F . Gan–Savin ( \(p \ne 2\) p 2 ) and Takeda–Wood ( \(p=2\) p = 2 ) obtained an equivalence between the Bernstein block of \(\text {Mp}(2n)\) Mp ( 2 n ) containing the even (resp. odd) Weil representation and the Iwahori-spherical block of the split \(\text {SO}(2n+1)\) SO ( 2 n + 1 ) (resp. its non-split inner form), by giving an isomorphism between Hecke algebras. We revisit this equivalence from an endoscopic perspective. It turns out that the L-parameters of irreducible representations are preserved, whilst the difference between characters of component groups is governed by symplectic local root numbers.