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p-ADIC HODGE THEORY

机译:p-ADIC杂散理论

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p-adic Hodge theory is an analogue of Hodge theory for an algebraic variety overa p-adic field. Hodge theory describes the singular cohomology in terms of the deRham cohomology and the space of harmonic forms for a complex or real manifold.The singular cohomology of a manifold is defined by using its topological proper-ties and we don't have its naive analogue over a p-adic field. Motivated by theWeil conjecture on the congruence zeta function of an algebraic variety over a finitefield, A. Grothendieck defined an analogue of the singular cohomology: the kalecohomology for an algebraic variety over a field (and more generally for a scheme)by introducing the notion of kale topology. [29]. Since then, kale cohomology hasbeen an indispensable tool for research in number theory and arithmetic geometry.On the other hand, the de Rham cohomology of the analytic manifold X" associ-ated to a non-singular algebraic variety X defined over the complex number field iscanonically isomorphic to the de Rham cohomology defined by using the sheaves ofalgebraic differential forms on X, and the latter can be defined for a non-singularalgebraic variety over an arbitrary field. p-adic Hodge theory aims at describingthe p-adic kale cohomology HeT(X 0Q2, Qp, Qp) of an algebraic variety X over thep-adic field Qp (or more generally its finite extension), which is a finite-dimensionalQp-vector space, in terms of the (algebraic) de Rham cohomology. Here Qp de-notes an algebraic closure of Qp, and the p-adic kale cohomology is endowed witha natural action of the Galois group Gal (Qp/Qp). We take this Galois action intoconsideration in p-adic Hodge theory. A finite-dimensional Qp-vector space witha continuous and linear action of the Galois group Gal (Qp/Qp) is called a p-adicrepresentation of Gal (Qp/Qp) and it is one of the main objects of study in p-adicHodge theory. However, in this article, we restrict ourselves to treating only theparts related to cohomologies.
机译:p-adic Hodge理论是p-adic场上代数变体的Hodge理论的类似物。 Hodge理论用deRham同调和复或实流形的调和形式空间描述了奇异同调。流形的奇异同调是使用其拓扑性质来定义的,我们在其上没有其天真的相似性p-adic场。受Weil猜想的启发,A。Grothendieck对有限域上的代数变体的全同zeta函数进行了定义,它定义了奇异同调的一个类似物:通过引入的概念,一个场上的代数变体的kalecohomology(更普遍地是一种方案)羽衣甘蓝拓扑。 [29]。从那时起,羽衣甘蓝同调已成为研究数论和算术几何学必不可少的工具。另一方面,解析流形X“的de Rham同调与在复数域上定义的非奇异代数X关联通过使用X上的代数微分形式的束定义的de Rham同态同构同构,并且后者可以为任意场上的非奇异代数变体定义。p-adic Hodge理论旨在描述p-adic羽衣甘蓝同调HeT(在p-adic场Qp(或更一般地,它的有限扩展)上的代数变种X的X 0Q2,Qp,Qp),这是有限的Qp向量空间,用(代数)de Rham同调性表示。表示Qp的代数闭合,并且p-adic羽衣甘蓝同调具有Galois族Gal(Qp / Qp)的自然作用,我们将此p -adic Hodge理论中的Galois作用考虑在内。 -向量空间Galois群Gal(Qp / Qp)的连续和线性作用称为Gal(pp-Qp)的p-增量表示,它是p-adicHodge理论研究的主要对象之一。但是,在本文中,我们仅限于仅处理与同调相关的部分。

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