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Weil Conjectures Exposition Weil Conjectures Exposition Evgeny Goncharov [email protected],∗ [email protected]† Abstract In this paper we provide a full account of the Weil conjectures including Deligne’s proof of the conjecture about the eigenvalues of the Frobenius endomorphism. Section 1 is an introduction into the subject. Our exposition heavily relies on the Etale Cohomology theory of Grothendieck so I included an overview in Section 2. Once one ver- ifies (or takes for granted) the results therein, proofs of most of the Weil conjectures are straightforward as we show in Section 3. Sections 4-8 constitute the proof of the remaining conjecture. The exposition is mostly similar to that of Deligne in [7] though I tried to provide more details whenever necessary. Following Deligne, I included an overview of Lefschetz theory (that is crucial for the proof) in Section 6. Section 9 contains a (somewhat random and far from complete) account of the conse- quences. Numerous references are mentioned throughout the paper as well as briefly discussed in Subsection 1.4. Contents 1 Preliminaries 2 1.1 StatementoftheWeilconjectures . ....... 2 1.2 A different definition of the zeta function and the Frobenius endomorphism . 3 1.3 Examples and evolution of the results . ..... 4 1.4 References....................................... .. 6 arXiv:1807.10812v2 [math.AG] 26 Jan 2019 2 Overview of Etale cohomology 7 2.1 Basicdefinitions..................................... 7 2.2 Cohomology groups with compact support and l-adiccohomology . 9 2.3 Higher direct images of sheaves, the Leray spectral sequence ............. 11 2.4 Major results in Etale cohomology . .... 11 2.5 Cohomological interpretation of zeta and L-functions . .......... 14 2.6 Poincareduality..................................... 17 3 Proof of the Weil conjectures except for the Riemann hypothesis 19 4 Preliminary reductions 22 ∗Cambridge University, Center for Mathematical Sciences, Wilberforce Road, Cambridge, UK †National Research University Higher School of Economics (NRU HSE), Usacheva 6, Moscow, Russia. 1 5 The Main Lemma 23 6 Overview of Lefschetz theory 29 6.1 LocalLefschetztheory ............................. ..... 29 6.2 GlobalLefschetztheory. .. .. .. ..... 31 6.3 ThetheoremofKajdanandMargulis . .... 35 7 The rationality theorem 37 8 Completion of the proof of the Weil conjectures 41 9 Consequences 43 9.1 ConsequencesinNumbertheory. ..... 43 9.2 Otherconsequences................................ .... 46 1 Preliminaries In this section we formulate the Weil conjectures, state a few examples and outline how the results have evolved over the time. We finish by discussing the references. 1.1 Statement of the Weil conjectures a Let X0 be a nonsingular (= smooth) projective variety over Fq (a field with q p , p-prime, “ a Z 0 elements) of dimension d. We let X be the variety obtained from X0 by extension of P ą scalars of Fq to F¯q and X0 Fqn be the set of points of X0 with coordinates in Fqn . For a set A p q we denote by #A the number of elements in A (so #X0 Fqn is the number of points of X0 with p q coordinates in Fqn ). Definition. We define the zeta function of X0 to be tn Z X , t exp #X F n . 0 0 q n p q“ ˜ně1 p q ¸ ÿ Thus, Z X0, t Q t is a formal power series with rational coefficients. Note that we have p q P rr ss d n t log Z X , t #X F n t dt 0 0 q p q“ ně1 p q ÿ d n so t dt log Z X0, t is the generating function for the sequence #X0 Fq ně1. We nowp stateq the Weil conjectures (the original statementst canp bequ found in Weil’s paper [1] published in 1949): (I) Rationality: Z X0, t is a rational function of t. Moreover, we have p q P1 X0, t P3 X0, t P2d´1 t Z X0, t p q p q¨¨¨ p q p q“ P0 X0, t P2 X0, t P2d X0, t p q p q¨¨¨ p q d where P0 X0, t 1 t, P2d X0, t 1 q t and each Pi X0, t is an integral polynomial. p q“ ´ p q“ ´ p q 2 (II) Functional equation Z X0, t satisfies the functional equation p q ´d ´1 dχ{2 χ Z X0, q t q t Z X0, t , p q“˘ p q i where χ 1 βi for βi deg Pi t . “ ip´ q “ p q (III) Betti numbers If X lifts to a variety X1 in characteristic 0, then βi are the (real) Betti ř numbers of X1 considered as a variety over C. βi (IV) Riemann hypothesis For 1 i 2d 1, Pi t 1 αi,jt , where αi,j are ď ď ´ p q “ j“1p ´ q algebraic integers of absolute value qi{2. ś Although Weil does not explicitly say so, it is clear that the conjectures are partially suggested by topological statements (in particular, (I) is suggested by the Lefschetz fixed-point formula and (II) is suggested by Poincare duality). Note that χ in (II) is the Euler characteristic of X (which can be defined as the self-intersection number of the diagonal with itself in X X) and (III) ˆ suggests the existence of a cohomological theory such that βi are the Betti numbers (dimensions of the cohomology groups) of X in that theory. If such a theory also had an analog of the Lefschetz fixed-point formula and of Poincare duality (together with a theorem relating the Betti numbers of X and X1), then proofs of most of the conjectures (except for the Riemann hypothesis) would be straightforward. A search for such a theory (a ”Weil cohomology” theory) eventually resulted in the invention of Etale Cohomology (and l-adic cohomology) by Artin, Verdier and Grothendieck. In terms of this l-adic cohomology, the ”moral” of (I)-(IV) is that topological properties of X0 determine the diophantine shape of its zeta function. 1.2 A different definition of the zeta function and the Frobenius en- domorphism To explain the connection between (IV) above and the original Riemann hypothesis (for the Rie- mann zeta function) we need to make an alternative definition of the zeta function (it is also the definition used by Deligne in [7]): Definition. Let Y be a scheme of finite type over Spec Z , Y the set of closed points of Y and for y Y denote by N y the number of elements in the residuep q | field| k y of Y at y. The Hasse-Weil zetaP | function| of Y isp q p q ´s ´1 ζY s 1 N y p q“ p ´ p q q yP|Y | ź (this product absolutely converges for Re s dim Y ). p qą Note that for Y Spec Z , ζY s is the Riemann zeta function (we will elaborate more on this in the last few paragraphs“ p ofq thisp paper).q We can regard a variety X0 as a scheme of finite type over Z via X0 Spec Fq ã Spec Z Ñ p q Ñ p q (where the second map is defined by Z Z pZ ã Fq). For x X0 let deg x k x : Fq . We have N x qdegpxq so it makes sense toÑ introduce{ Ñ a new variableP t q´sandp letq“r p q s p q“ “ degpxq ´1 Z X0, t 1 t . p q“ p ´ q xP|X | ź0 3 This product converges for t small enough and we have | | ´s ζX s Z X0, q . 0 p q“ p q Given that this definition of Z X0, t coincides with the one given in Subsection 1.1, the Rie- p q mann hypothesis for X0 states that ζX0 s has its poles on the lines Re s 0, 1, , dim X0 and 1 3 dimpX0q´1 p q“ ¨ ¨ ¨ zeroes on the lines Re s 2 , 2 , , 2 , so the analogy with the original Riemann hypothesis becomes clear. p q“ ¨ ¨ ¨ Let me now introduce the Frobenius endomorphism1 F (that will play a central role in our exposition) and explore the connection between the fixed points of X under F n, n 1 and the 2 q ě varieties X0 Fqn . Define the Frobenius endomorphism as F : X X, x x . By this we p q Ñ Ñ mean that on every open affine U (defined by some U0) F acts by taking the q-th power of all the coordinates (there exists a unique such F ). We have F ´1 U U and deg F qdim X . Identify p q “ “ the set X of closed points of X with X0 F¯q (those are the points Hom Spec F¯q ,X0 of X0 | | p q Fq p p q q with coefficients in F¯q). Let ϕ Gal F¯q Fq be the substitution of Frobenius. The action of F on P p { q X identifies with the action of ϕ on X0 F¯q . Under this equivalence: | | F p q (a) The set X of closed points of X fixed under F is identified with the set X0 Fq X0 F¯q q p qĂ p q of points of X defined over Fq (just because for x F¯q one has x Fq x x). (b) Similarly, the set XF n of closed points of XPfixed under theP n-thô iteration“ of F is identified with X0 Fqn . p q (c) The set X of closed points of X is identified with the set X F of the orbits of F (or ϕ) | | | | on X . The degree deg x of x X0 is the number of elements in the corresponding orbit. |(d)| From (b) and (c)p weq seeP that | | F n #X #X0 Fqn deg x (1) “ p q“ p q degpxq|n ÿ (for x X0 and deg x n, x defines deg x points with coordinates in Fqn all conjugate over Fq).
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