<p>Based on our previous work on an arithmetic analogue of Christol’s theorem, this paper studies in more detail the structure of the <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Λ</mi> </math></EquationSource> </InlineEquation>-ring <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq2.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="156" /> </InlineMediaObject> <EquationSource Format="TEX">\(E_K = K \otimes W_{O_K}^a(O_{\bar{K}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mi>K</mi> </msub> <mo>=</mo> <mi>K</mi> <mo>⊗</mo> <msubsup> <mi>W</mi> <mrow> <msub> <mi>O</mi> <mi>K</mi> </msub> </mrow> <mi>a</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>O</mi> <mover accent="true"> <mrow> <mi>K</mi> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> of algebraic Witt vectors for number fields <i>K</i>. First developing general results concerning <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(E_K\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>E</mi> <mi>K</mi> </msub> </math></EquationSource> </InlineEquation>, we apply them to the case when <i>K</i> is an imaginary quadratic field. The main results include the “<i>modularity theorem</i>” for algebraic Witt vectors, which claims that certain deformation families <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq4.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="143" /> </InlineMediaObject> <EquationSource Format="TEX">\(f: M_2(\widehat{\mathbb {Z}}) \times \mathfrak {H}\rightarrow \mathbb {C}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>:</mo> <msub> <mi>M</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mover accent="true"> <mi mathvariant="double-struck">Z</mi> <mo stretchy="false">^</mo> </mover> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <mi mathvariant="fraktur">H</mi> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">C</mi> </mrow> </math></EquationSource> </InlineEquation> of modular functions of finite level always define algebraic Witt vectors <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\widehat{f}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mi>f</mi> <mo stretchy="false">^</mo> </mover> </math></EquationSource> </InlineEquation> by their special values, and conversely, every algebraic Witt vector <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\xi \in E_K\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ξ</mi> <mo>∈</mo> <msub> <mi>E</mi> <mi>K</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> is realized in this way, that is, <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq7.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(\xi = \widehat{f}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ξ</mi> <mo>=</mo> <mover accent="true"> <mi>f</mi> <mo stretchy="false">^</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> for some deformation family <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq4.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="143" /> </InlineMediaObject> <EquationSource Format="TEX">\(f: M_2(\widehat{\mathbb {Z}}) \times \mathfrak {H}\rightarrow \mathbb {C}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>:</mo> <msub> <mi>M</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mover accent="true"> <mi mathvariant="double-struck">Z</mi> <mo stretchy="false">^</mo> </mover> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <mi mathvariant="fraktur">H</mi> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">C</mi> </mrow> </math></EquationSource> </InlineEquation>. This gives a rather explicit description of the <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Λ</mi> </math></EquationSource> </InlineEquation>-ring <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(E_K\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>E</mi> <mi>K</mi> </msub> </math></EquationSource> </InlineEquation> for imaginary quadratic fields <i>K</i>, which is stated as the identity <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq11.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="76" /> </InlineMediaObject> <EquationSource Format="TEX">\(E_K = M_K\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mi>K</mi> </msub> <mo>=</mo> <msub> <mi>M</mi> <mi>K</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> between the <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Λ</mi> </math></EquationSource> </InlineEquation>-ring <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="26" /> </InlineMediaObject> <EquationSource Format="TEX">\(E_K\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>E</mi> <mi>K</mi> </msub> </math></EquationSource> </InlineEquation> and the <i>K</i>-algebra <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq14.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="TEX">\(M_K\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>M</mi> <mi>K</mi> </msub> </math></EquationSource> </InlineEquation> of <i>modular vectors</i> <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40687_2025_525_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\widehat{f}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mi>f</mi> <mo stretchy="false">^</mo> </mover> </math></EquationSource> </InlineEquation>.</p>

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Semi-galois categories III: Witt vectors by deformations of modular functions

  • Takeo Uramoto

摘要

Based on our previous work on an arithmetic analogue of Christol’s theorem, this paper studies in more detail the structure of the \(\Lambda \) Λ -ring \(E_K = K \otimes W_{O_K}^a(O_{\bar{K}})\) E K = K W O K a ( O K ¯ ) of algebraic Witt vectors for number fields K. First developing general results concerning \(E_K\) E K , we apply them to the case when K is an imaginary quadratic field. The main results include the “modularity theorem” for algebraic Witt vectors, which claims that certain deformation families \(f: M_2(\widehat{\mathbb {Z}}) \times \mathfrak {H}\rightarrow \mathbb {C}\) f : M 2 ( Z ^ ) × H C of modular functions of finite level always define algebraic Witt vectors \(\widehat{f}\) f ^ by their special values, and conversely, every algebraic Witt vector \(\xi \in E_K\) ξ E K is realized in this way, that is, \(\xi = \widehat{f}\) ξ = f ^ for some deformation family \(f: M_2(\widehat{\mathbb {Z}}) \times \mathfrak {H}\rightarrow \mathbb {C}\) f : M 2 ( Z ^ ) × H C . This gives a rather explicit description of the \(\Lambda \) Λ -ring \(E_K\) E K for imaginary quadratic fields K, which is stated as the identity \(E_K = M_K\) E K = M K between the \(\Lambda \) Λ -ring \(E_K\) E K and the K-algebra \(M_K\) M K of modular vectors \(\widehat{f}\) f ^ .