<p>Let <i>X</i> be a normal variety of positive dimension over a finite field of characteristic <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(p&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and let <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {C}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">C</mi> </math></EquationSource> </InlineEquation> be either a locally constant constructible Weil <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>ℓ</mi> </msub> </math></EquationSource> </InlineEquation>-sheaf, a locally constant constructible quasi-tame <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq4.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_\mathfrak {u}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi mathvariant="fraktur">u</mi> </msub> </math></EquationSource> </InlineEquation>-sheaf or an overconvergent <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-<i>F</i>-isocrystal on <i>X</i>. We prove the following Tannakian Cebotarev density theorem: let <i>S</i> be a set of closed points of <i>X</i> of upper Dirichlet density 1 (resp. <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq6.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>) and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Φ</mi> </math></EquationSource> </InlineEquation> the union of conjugacy classes of Frobenius elements corresponding to <i>S</i> in the Tannakian group <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="TEX">\(G(\mathcal {C})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mo stretchy="false">(</mo> <mi mathvariant="script">C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> of <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {C}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">C</mi> </math></EquationSource> </InlineEquation>. Then <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Φ</mi> </math></EquationSource> </InlineEquation> is Zariski-dense in (resp. the Zariski-closure of <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Φ</mi> </math></EquationSource> </InlineEquation> contains at least one connected component of) <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="37" /> </InlineMediaObject> <EquationSource Format="TEX">\(G(\mathcal {C})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>G</mi> <mo stretchy="false">(</mo> <mi mathvariant="script">C</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. We use the theory of companions and its by-product, the existence of a weight filtration, to reduce the general statement to the case of locally constant constructible étale <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq3.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>ℓ</mi> </msub> </math></EquationSource> </InlineEquation>-sheaves, where the assertion is an easy consequence of the (classical) Cebotarev density theorem. The reduction step relies on group-theoretic arguments which might be of independent interest. When <i>X</i> is smooth, our strategy can be adapted to reduce the Tannakian Cebotarev density theorem for convergent <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-<i>F</i>-isocrystals satisfying a weak form of the parabolicity conjecture of Crew (resp. for overconvergent <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-<i>F</i>-isocrystals) to the case of direct sums of isoclinic <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-<i>F</i>-isocrystals, which is due to Hartl and Pál. Since the parabolicity conjecture is known for convergent <InlineEquation ID="IEq17"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-<i>F</i>-isocrystals admitting an overconvergent extension by recent work of D’Addezio and is straightforward for convergent <InlineEquation ID="IEq18"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-<i>F</i>-isocrystals admitting a slope filtration, this in particular proves unconditionally the Tannakian Cebotarev density theorem in those two cases. Let us point out that this variant of our strategy for convergent (resp. overconvergent) <InlineEquation ID="IEq19"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="208_2024_2994_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="20" /> </InlineMediaObject> <EquationSource Format="TEX">\(\overline{\mathbb {Q}}_p\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mover> <mi mathvariant="double-struck">Q</mi> <mo>¯</mo> </mover> <mi>p</mi> </msub> </math></EquationSource> </InlineEquation>-<i>F</i>-isocrystals is purely <i>p</i>-adic and “elementary” in the sense that it does not resort to automorphic techniques <i>via</i> the companion conjecture (nor to the “à la Weil II” formalism of Frobenius weights).</p>

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Variations on a Tannakian Cebotarev density theorem

  • Anna Cadoret,
  • Akio Tamagawa

摘要

Let X be a normal variety of positive dimension over a finite field of characteristic \(p>0\) p > 0 and let \(\mathcal {C}\) C be either a locally constant constructible Weil \(\overline{\mathbb {Q}}_\ell \) Q ¯ -sheaf, a locally constant constructible quasi-tame \(\overline{\mathbb {Q}}_\mathfrak {u}\) Q ¯ u -sheaf or an overconvergent \(\overline{\mathbb {Q}}_p\) Q ¯ p -F-isocrystal on X. We prove the following Tannakian Cebotarev density theorem: let S be a set of closed points of X of upper Dirichlet density 1 (resp. \(>0\) > 0 ) and \(\Phi \) Φ the union of conjugacy classes of Frobenius elements corresponding to S in the Tannakian group \(G(\mathcal {C})\) G ( C ) of \(\mathcal {C}\) C . Then \(\Phi \) Φ is Zariski-dense in (resp. the Zariski-closure of \(\Phi \) Φ contains at least one connected component of) \(G(\mathcal {C})\) G ( C ) . We use the theory of companions and its by-product, the existence of a weight filtration, to reduce the general statement to the case of locally constant constructible étale \(\overline{\mathbb {Q}}_\ell \) Q ¯ -sheaves, where the assertion is an easy consequence of the (classical) Cebotarev density theorem. The reduction step relies on group-theoretic arguments which might be of independent interest. When X is smooth, our strategy can be adapted to reduce the Tannakian Cebotarev density theorem for convergent \(\overline{\mathbb {Q}}_p\) Q ¯ p -F-isocrystals satisfying a weak form of the parabolicity conjecture of Crew (resp. for overconvergent \(\overline{\mathbb {Q}}_p\) Q ¯ p -F-isocrystals) to the case of direct sums of isoclinic \(\overline{\mathbb {Q}}_p\) Q ¯ p -F-isocrystals, which is due to Hartl and Pál. Since the parabolicity conjecture is known for convergent \(\overline{\mathbb {Q}}_p\) Q ¯ p -F-isocrystals admitting an overconvergent extension by recent work of D’Addezio and is straightforward for convergent \(\overline{\mathbb {Q}}_p\) Q ¯ p -F-isocrystals admitting a slope filtration, this in particular proves unconditionally the Tannakian Cebotarev density theorem in those two cases. Let us point out that this variant of our strategy for convergent (resp. overconvergent) \(\overline{\mathbb {Q}}_p\) Q ¯ p -F-isocrystals is purely p-adic and “elementary” in the sense that it does not resort to automorphic techniques via the companion conjecture (nor to the “à la Weil II” formalism of Frobenius weights).