<p>Let <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math> <mi>K</mi> </math></EquationSource> <EquationSource Format="TEX">$K$</EquationSource> </InlineEquation> be a finite extension of <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="bold">Q</mi> <mi>p</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">$\mathbf {Q}_{p}$</EquationSource> </InlineEquation>, and <InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> <EquationSource Format="TEX">$\rho $</EquationSource> </InlineEquation> be an <InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math> <mi>n</mi> </math></EquationSource> <EquationSource Format="TEX">$n$</EquationSource> </InlineEquation>-dimensional (non-critical generic) crystabelline representation of the absolute Galois group of <InlineEquation ID="IEq7"> <EquationSource Format="MATHML"><math> <mi>K</mi> </math></EquationSource> <EquationSource Format="TEX">$K$</EquationSource> </InlineEquation> of regular Hodge-Tate weights. We associate to <InlineEquation ID="IEq8"> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> <EquationSource Format="TEX">$\rho $</EquationSource> </InlineEquation> an explicit locally <InlineEquation ID="IEq9"> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="bold">Q</mi> <mi>p</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">$\mathbf {Q}_{p}$</EquationSource> </InlineEquation>-analytic representation <InlineEquation ID="IEq10"> <EquationSource Format="MATHML"><math> <msub> <mi>π</mi> <mn>1</mn> </msub> <mo stretchy="false">(</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\pi _{1}(\rho )$</EquationSource> </InlineEquation> of <InlineEquation ID="IEq11"> <EquationSource Format="MATHML"><math> <msub> <mo>GL</mo> <mi>n</mi> </msub> <mo stretchy="false">(</mo> <mi>K</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\operatorname{\mathrm {G}L}_{n}(K)$</EquationSource> </InlineEquation>, which encodes some <InlineEquation ID="IEq12"> <EquationSource Format="MATHML"><math> <mi>p</mi> </math></EquationSource> <EquationSource Format="TEX">$p$</EquationSource> </InlineEquation>-adic Hodge parameters of <InlineEquation ID="IEq13"> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> <EquationSource Format="TEX">$\rho $</EquationSource> </InlineEquation>. When <InlineEquation ID="IEq14"> <EquationSource Format="MATHML"><math> <mi>K</mi> <mo>=</mo> <msub> <mi mathvariant="bold">Q</mi> <mi>p</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">$K=\mathbf {Q}_{p}$</EquationSource> </InlineEquation>, it encodes the full information hence reciprocally determines <InlineEquation ID="IEq15"> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> <EquationSource Format="TEX">$\rho $</EquationSource> </InlineEquation>. When <InlineEquation ID="IEq16"> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> <EquationSource Format="TEX">$\rho $</EquationSource> </InlineEquation> is associated to <InlineEquation ID="IEq17"> <EquationSource Format="MATHML"><math> <mi>p</mi> </math></EquationSource> <EquationSource Format="TEX">$p$</EquationSource> </InlineEquation>-adic automorphic representations, we show under mild hypotheses that <InlineEquation ID="IEq18"> <EquationSource Format="MATHML"><math> <msub> <mi>π</mi> <mn>1</mn> </msub> <mo stretchy="false">(</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\pi _{1}(\rho )$</EquationSource> </InlineEquation> is a subrepresentation of the <InlineEquation ID="IEq19"> <EquationSource Format="MATHML"><math> <msub> <mo>GL</mo> <mi>n</mi> </msub> <mo stretchy="false">(</mo> <mi>K</mi> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\operatorname{\mathrm {G}L}_{n}(K)$</EquationSource> </InlineEquation>-representation globally associated to <InlineEquation ID="IEq20"> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> <EquationSource Format="TEX">$\rho $</EquationSource> </InlineEquation>.</p>

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\(p\)-Adic Hodge parameters in the crystabelline representations of \(\operatorname{\mathrm {G}L}_{n}\)

  • Yiwen Ding

摘要

Let K $K$ be a finite extension of Q p $\mathbf {Q}_{p}$ , and ρ $\rho $ be an n $n$ -dimensional (non-critical generic) crystabelline representation of the absolute Galois group of K $K$ of regular Hodge-Tate weights. We associate to ρ $\rho $ an explicit locally Q p $\mathbf {Q}_{p}$ -analytic representation π 1 ( ρ ) $\pi _{1}(\rho )$ of GL n ( K ) $\operatorname{\mathrm {G}L}_{n}(K)$ , which encodes some p $p$ -adic Hodge parameters of ρ $\rho $ . When K = Q p $K=\mathbf {Q}_{p}$ , it encodes the full information hence reciprocally determines ρ $\rho $ . When ρ $\rho $ is associated to p $p$ -adic automorphic representations, we show under mild hypotheses that π 1 ( ρ ) $\pi _{1}(\rho )$ is a subrepresentation of the GL n ( K ) $\operatorname{\mathrm {G}L}_{n}(K)$ -representation globally associated to ρ $\rho $ .