<p>In the setting of a Drinfeld module <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq1.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="16" /> </InlineMediaObject> <EquationSource Format="TEX">\(\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ϕ</mi> </math></EquationSource> </InlineEquation> over a curve <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="40" /> </InlineMediaObject> <EquationSource Format="TEX">\(X/\mathbb {F}_q\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>X</mi> <mo stretchy="false">/</mo> <msub> <mi mathvariant="double-struck">F</mi> <mi>q</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>, we use a functorial point of view to define <i>Anderson eigenvectors</i>, a generalization of the so-called “special functions” introduced by Anglès, Ngo Dac and Tavares Ribeiro, and prove the existence of a universal object <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega _\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ω</mi> <mi>ϕ</mi> </msub> </math></EquationSource> </InlineEquation>. We adopt an analogous approach with the adjoint Drinfeld module <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\phi ^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>ϕ</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation> to define <i>dual Anderson eigenvectors</i>. The universal object of this functor, denoted by <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\zeta _\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ζ</mi> <mi>ϕ</mi> </msub> </math></EquationSource> </InlineEquation>, is a generalization of Pellarin zeta functions, can be expressed as an Eisenstein-like series over the period lattice, and its coordinates are analytic functions from <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="106" /> </InlineMediaObject> <EquationSource Format="TEX">\(X({\mathbb {C}_\infty })\setminus \{\infty \}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>X</mi> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="double-struck">C</mi> <mi>∞</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mo lspace="0.15em" rspace="0.15em" stretchy="false">\</mo> <mrow> <mo stretchy="false">{</mo> <mi>∞</mi> <mo stretchy="false">}</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {C}_\infty }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">C</mi> <mi>∞</mi> </msub> </math></EquationSource> </InlineEquation>. For all integers <i>i</i>, we define dot products <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq8.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(\zeta _\phi \cdot \omega _\phi ^{(i)}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ζ</mi> <mi>ϕ</mi> </msub> <mo>·</mo> <msubsup> <mi>ω</mi> <mi>ϕ</mi> <mrow> <mo stretchy="false">(</mo> <mi>i</mi> <mo stretchy="false">)</mo> </mrow> </msubsup> </mrow> </math></EquationSource> </InlineEquation> as certain meromorphic differential forms over <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\(X_{\mathbb {C}_\infty }\setminus \{\infty \}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>X</mi> <msub> <mi mathvariant="double-struck">C</mi> <mi>∞</mi> </msub> </msub> <mo lspace="0.15em" rspace="0.15em" stretchy="false">\</mo> <mrow> <mo stretchy="false">{</mo> <mi>∞</mi> <mo stretchy="false">}</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and prove they are actually rational. This amounts to a generalization of Pellarin’s identity for the Carlitz module and is linked to the pairing of the <i>A</i>-motive and the dual <i>A</i>-motive defined by Hartl and Juschka. Finally, we develop an algorithm to compute the forms <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq8.gif" Format="GIF" Height="27" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(\zeta _\phi \cdot \omega _\phi ^{(i)}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ζ</mi> <mi>ϕ</mi> </msub> <mo>·</mo> <msubsup> <mi>ω</mi> <mi>ϕ</mi> <mrow> <mo stretchy="false">(</mo> <mi>i</mi> <mo stretchy="false">)</mo> </mrow> </msubsup> </mrow> </math></EquationSource> </InlineEquation> when <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_506_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(X=\mathbb {P}^1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>X</mi> <mo>=</mo> <msup> <mrow> <mi mathvariant="double-struck">P</mi> </mrow> <mn>1</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> and prove a conjecture of Gazda and Maurischat about the invertibility of special functions for Drinfeld modules of rank 1.</p>

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A duality result about special functions for Drinfeld modules of arbitrary rank

  • Giacomo Hermes Ferraro

摘要

In the setting of a Drinfeld module \(\phi \) ϕ over a curve \(X/\mathbb {F}_q\) X / F q , we use a functorial point of view to define Anderson eigenvectors, a generalization of the so-called “special functions” introduced by Anglès, Ngo Dac and Tavares Ribeiro, and prove the existence of a universal object \(\omega _\phi \) ω ϕ . We adopt an analogous approach with the adjoint Drinfeld module \(\phi ^*\) ϕ to define dual Anderson eigenvectors. The universal object of this functor, denoted by \(\zeta _\phi \) ζ ϕ , is a generalization of Pellarin zeta functions, can be expressed as an Eisenstein-like series over the period lattice, and its coordinates are analytic functions from \(X({\mathbb {C}_\infty })\setminus \{\infty \}\) X ( C ) \ { } to \({\mathbb {C}_\infty }\) C . For all integers i, we define dot products \(\zeta _\phi \cdot \omega _\phi ^{(i)}\) ζ ϕ · ω ϕ ( i ) as certain meromorphic differential forms over \(X_{\mathbb {C}_\infty }\setminus \{\infty \}\) X C \ { } and prove they are actually rational. This amounts to a generalization of Pellarin’s identity for the Carlitz module and is linked to the pairing of the A-motive and the dual A-motive defined by Hartl and Juschka. Finally, we develop an algorithm to compute the forms \(\zeta _\phi \cdot \omega _\phi ^{(i)}\) ζ ϕ · ω ϕ ( i ) when \(X=\mathbb {P}^1\) X = P 1 and prove a conjecture of Gazda and Maurischat about the invertibility of special functions for Drinfeld modules of rank 1.