Weil Conjectures and Betti Numbers of Moduli Spaces

Total Page:16

File Type:pdf, Size:1020Kb

Weil Conjectures and Betti Numbers of Moduli Spaces Weil conjectures and Betti numbers of moduli spaces Christopher Lazda 1 Lecture 1 Let’s start with an object you’ll hopefully all be reasonably familiar with. X s ³(s) n¡ , s C, Re(s) 1. Æ n 1 2 È ¸ Conjecture (RH). If ³(s) 0 and 0 Re(s) 1, then Re(s) 1 . Æ Ç Ç Æ 2 This has an Euler product expansion Y s 1 ³(s) (1 p¡ )¡ Æ p prime ¡ and we note that {prime numbers} {closed points of Spec(Z)} $ so we can write Y s 1 ³(s) (1 #k(x)¡ )¡ Æ x Spec(Z) ¡ 2j j where k(x) is the residue field at x. Definition. For any scheme X of finite type over Z, (i.e. any “arithmetic scheme") we define Y s 1 ³X (s) (1 #k(x)¡ )¡ Æ x X ¡ 2j j the product being taken over all closed points, and k(x) denotes the residue field. Exercise. Show that in this situation k(x) is always a finite field, so the definition makes sense. Example. Suppose that K/Q is finite, with ring of integers OK . Then taking X Spec(OK ) Æ we get Y s 1 ³Spec (s) (1 Np¡ )¡ (OK ) Æ ¡ p OK ½ which is the usual Dedekind zeta function ³K (s) of K. There is also a Riemann hypothesis 1 for ³K , again stating that zeroes of ³K with 0 Re(s) 1 satisfy Re(s) . Ç Ç Æ 2 1 ¡ ¢ Example. X AF Spec Fp t . Æ p Æ J K n 1 o © ª closed points of A irreducible polynomials over Fp Fp $ Y ds Nd ³ 1 (s) (1 p¡ )¡ AF ) p Æ d 1 ¡ ¸ 1 s where Nd # irreducible polynomials of degree d. Let’s try the following trick: set u p¡ Æ Q d Nd Æ and compute uZ0(u)/Z(u) where Z(u) (1 u )¡ . We get Æ d ¡ d dN ud u log Z(u) X d d du Æ d 1 1 u ¸ ¡ X md dNd u Æ d,m 1 ¸ X X n dNd u Æ n 1 d n ¸ j X pnun Æ n 1 ¸ n n P 1 n since (recall from Galois theory) d n dNd p . Note that p #AF (Fp ) and that we also j Æ Æ p have d p log Z(u) du Æ 1 pu ¡ 1 Z(u) ) Æ 1 pu ¡ 1 ³A1 (s) . ) Fp Æ 1 p1 s ¡ ¡ This trivially satisfies the ‘Riemann Hypothesis’, since it has no zeroes. Lemma. Let q be a prime power, and X a scheme of finite type over Fq (therefore X is a scheme of finite type over Z and has a zeta function). Write Bn #X(Fqn ). Then we have Æ Ã ! X Bn n ³X (s) exp u Æ n 1 n ¸ s where u q¡ Æ Proof. Let Nd be the number of closed points of X of degree d over Fq, i.e. such that the residue field k(x) is Fqd . Then we have the formula X dNd Bn d n Æ j since every closed point of degree d gives rise to exactly d points in X(Fqn ) for d n. Then j exactly as in the calculation we’ve just done we can show Y d Nd ³X (s) (1 u )¡ Æ d 1 ¡ ¸ s Q d Nd where u q¡ and that if we let Z(u) d 1(1 u )¡ then we have an identity of power Æ Æ ¸ ¡ series d X n u log Z(u) Bnu du Æ n 1 ¸ and the lemma follows. 2 nd Exercise. By showing that when X/Fq has dimension d,#X(Fqn ) O(q ) as d , show Æ ! 1 that ³X (s) converges for Re(s) dim X. È So zeta function of schemes over finite fields ‘encode’ the numbers of points over all finite extension fields, in that if you know one, you know the other. It’s in practise often easier to work with the power series à ! X #X(Fqn ) n Z(X, u): exp u Q u . Æ n 1 n 2 J K ¸ Note that while the ³-function ³X (s) doesn’t ‘see’ the base field Fq, the Z-function Z(X, u) s does, since we have set u q¡ . Æ 1.1 Abelian Varieties Now let’s take A/Fq an abelian variety of dimension g, that is a smooth, projective, (geo- metrically) connected group variety over Fq. We’ll let A A F Fq, and F : A A be the Æ £ q ! q-power linear Frobenius morphism, that is if we have some projective embedding A PN ! Fq q q then in homogeneous co-ordinates we have F(x0 : ... : xN ) (x0 : ... : xN ). Æ n Therefore A(Fqn ) is exactly the (closed) fixed points of F , or in other words, if we con- sider the isogeny n ©n id F : A A Æ ¡ ! n then A(Fqn ) ker(©n)(Fq). Since id F separable, we therefore have Æ ¡ n #A(Fqn ) deg(id F ). Æ ¡ n To calculate this, we’ll introduce the Tate module of A. Let ` - q be a prime, so that A[` ] is n2g an étale group scheme over Fq of order ` , and n n 2g A[` ](Fq) (Z/` Z) Æ» (non-canonically). The multiplication by ` induces transition maps n n 1 [`]: A[` ](Fq) A[` ¡ ](Fq) ! so we can form the inverse limit n T (A): lim A[` ](Fq), ` Æ Ã¡¡n this is a free Z -module of rank 2g, and every endomorphism à End(A) of A induces an ` 2 endomorphism à of T (A), and hence of V (A): T (A) Z Q . ` ` ` Æ ` ­ ` ` Theorem (See Mumford’s “Abelian Varieties”). For every endomorphism à End(A) there 2 exists a unique polynomial P (t) Z[t] (the characteristic polynomial of Ã) such that for all à 2 integers n we have P (n) deg([n] Ã). Ã Æ ¡ 3 Moreover for any ` - q we have that P (t) det(t à ) Ã Æ ¡ ` is the characteristic polynomial of Ã` acting on V`(A). We’re now going to take à F, the Frobenius endomorphism, this tells us that if we let Æ 2g Y PF (t) (t ! j) Æ i 1 ¡ Æ be the characteristic polynomial of F acting on V (A), and n 1, then ` ¸ 2g Y n PF n (t) (t ! j ) Æ i 1 ¡ Æ n is the characteristic polynomial of F acting on V`(A) and hence we can count the number of Fqn -rational points on A as 2g n Y n #A(Fqn ) deg(id F ) PF n (1) (1 ! j ) Æ ¡ Æ Æ i 1 ¡ Æ X n X n n n n 1 ! ! ! ... ! ...! . Æ ¡ j1 Å j1 j2 ¡ Å j1 j2g j1 j1, j2 Actually, some simple linear algebra tells us that X n n ! ...! j1 jk j1,..., jk n k is exactly the trace of F acting on ¤ V`(A), so we can write 2g X k n k #A(Fqn ) ( 1) Tr(F ¤ V`(A)). Æ k 0 ¡ j Æ Substituting this in to the expression for Z(A, u) gives us k 1 à !( 1) Å 2g n ¡ Y X n k u Z(A, u) exp Tr(F ¤ V`(A) Æ k 0 ¡ n 1 j n Æ ¸ Lemma. Let V be a finite dimensional vector space over a field K, and ' : V V and ! endomorphism. Then à n ! X n u det¡id 'u¢ exp Tr(' ) . ¡ Æ ¡ n 1 n ¸ Proof. Exercise (hint: express both sides in terms of the eigenvalues of '). So we can therefore write the Z-function of A as 2g k 1 Y k ( 1) Å Z(A, u) det(id Fu ¤ V`(A)) ¡ Æ k 0 ¡ j Æ P1(t)...P2g 1(u) ¡ Æ P0(u)...P2g(u) 4 where k Pk(t) det(id Fu ¤ V (A)) Z[u] Æ ¡ j ` 2 Q can be written as (1 ®iku) with ®ik running over things of the form ! j ...! j . i ¡ 1 k 1/2 Theorem (Riemann Hypothesis). Each ! j has norm q . s Exercise. What does this tell us about the zeroes of ³A(s) Z(A, q¡ )? Æ Exercise. We expect a functional equation g 1 Z(A,(q u)¡ ) Z(A, u) Æ can you interpret this in terms of a statement about the ! j? 2 Lectures 2 & 3 James told you about the Weil conjectures, and said that a ‘good’ cohomology theory for varieties over Fq would imply them more or less formally. Let’s look at that in a bit more detail. Weil cohomology theories Definition. Fix an algebraically closed field k and let Vk be the category of smooth, pro- jective, connected varieties over k, that is non-singular, connected varieties cut out by ho- mogenous equations in some PN (k). Let K be a field of characteristic 0. A K-valued Weil cohomology theory is a contravariant functor H¤( ): Vk {graded vector spaces over K} ¡ ! X H¤(X) 7! f : X Y f ¤ : H¤(Y ) H¤(X) ! 7! ! together with a graded commutative product i j i j : H (X) K H (X) H Å (X) [ ­ ! a trace morphism Tr : H2dim X (X) K ! and a cycle class map cl : Cr(X) H2r(X) ! such that: i) Hi(X) is finite dimensional, and zero outside the range [0,2dim X]. ii) (Künneth formula) if we let p1, p2 : X Y X,Y denote the two projections, then the £ ! natural map H¤(X) K H¤(Y ) H¤(X Y ) ­ ! £ ® ¯ ® ¯ : p¤(®) p¤(¯): ­ 7! Æ 1 [ 2 is an isomorphism.
Recommended publications
  • What Is the Motivation Behind the Theory of Motives?
    What is the motivation behind the Theory of Motives? Barry Mazur How much of the algebraic topology of a connected simplicial complex X is captured by its one-dimensional cohomology? Specifically, how much do you know about X when you know H1(X, Z) alone? For a (nearly tautological) answer put GX := the compact, connected abelian Lie group (i.e., product of circles) which is the Pontrjagin dual of the free abelian group H1(X, Z). Now H1(GX, Z) is canonically isomorphic to H1(X, Z) = Hom(GX, R/Z) and there is a canonical homotopy class of mappings X −→ GX which induces the identity mapping on H1. The answer: we know whatever information can be read off from GX; and are ignorant of anything that gets lost in the projection X → GX. The theory of Eilenberg-Maclane spaces offers us a somewhat analogous analysis of what we know and don’t know about X, when we equip ourselves with n-dimensional cohomology, for any specific n, with specific coefficients. If we repeat our rhetorical question in the context of algebraic geometry, where the structure is somewhat richer, can we hope for a similar discussion? In algebraic topology, the standard cohomology functor is uniquely characterized by the basic Eilenberg-Steenrod axioms in terms of a simple normalization (the value of the functor on a single point). In contrast, in algebraic geometry we have a more intricate set- up to deal with: for one thing, we don’t even have a cohomology theory with coefficients in Z for varieties over a field k unless we provide a homomorphism k → C, so that we can form the topological space of complex points on our variety, and compute the cohomology groups of that topological space.
    [Show full text]
  • DENINGER COHOMOLOGY THEORIES Readers Who Know What the Standard Conjectures Are Should Skip to Section 0.6. 0.1. Schemes. We
    DENINGER COHOMOLOGY THEORIES TAYLOR DUPUY Abstract. A brief explanation of Denninger's cohomological formalism which gives a conditional proof Riemann Hypothesis. These notes are based on a talk given in the University of New Mexico Geometry Seminar in Spring 2012. The notes are in the same spirit of Osserman and Ile's surveys of the Weil conjectures [Oss08] [Ile04]. Readers who know what the standard conjectures are should skip to section 0.6. 0.1. Schemes. We will use the following notation: CRing = Category of Commutative Rings with Unit; SchZ = Category of Schemes over Z; 2 Recall that there is a contravariant functor which assigns to every ring a space (scheme) CRing Sch A Spec A 2 Where Spec(A) = f primes ideals of A not including A where the closed sets are generated by the sets of the form V (f) = fP 2 Spec(A) : f(P) = 0g; f 2 A: By \f(P ) = 000 we means f ≡ 0 mod P . If X = Spec(A) we let jXj := closed points of X = maximal ideals of A i.e. x 2 jXj if and only if fxg = fxg. The overline here denote the closure of the set in the topology and a singleton in Spec(A) being closed is equivalent to x being a maximal ideal. 1 Another word for a closed point is a geometric point. If a point is not closed it is called generic, and the set of generic points are in one-to-one correspondence with closed subspaces where the associated closed subspace associated to a generic point x is fxg.
    [Show full text]
  • A Note on Grothendieck's Standard Conjectures of Type C and D
    A NOTE ON GROTHENDIECK’S STANDARD CONJECTURES OF TYPE C+ AND D GONC¸ALO TABUADA Abstract. Grothendieck conjectured in the sixties that the even K¨unneth projector (with respect to a Weil cohomology theory) is algebraic and that the homological equivalence relation on algebraic cycles coincides with the numer- ical equivalence relation. In this note we extend these celebrated conjectures from smooth projective schemes to the broad setting of smooth proper dg cat- egories. As an application, we prove that Grothendieck’s original conjectures are invariant under homological projective duality. This leads to a proof of Grothendieck’s conjectures in the case of intersections of quadrics, linear sec- tions of determinantal varieties, and intersections of bilinear divisors. Along the way, we prove also the case of quadric fibrations. 1. Introduction and statement of results Let k be a base field of characteristic zero. Given a smooth projective k-scheme ∗ i ∗ ∗ th X and a Weil cohomology theory H , let us denote by πX : H (X) → H (X) the i ∗ K¨unneth projector, by Z (X)Q the Q-vector space of algebraic cycles on X, and by ∗ ∗ Z (X)Q/∼hom and Z (X)Q/∼num the quotients with respect to the homological and numerical equivalence relations, respectively. Following Grothendieck [4] (see also Kleiman [6, 7]), the standard conjecture1 of type C+, denote by C+(X), asserts that + 2i the even K¨unneth projector πX := Pi πX is algebraic, and the standard conjecture ∗ ∗ of type D, denoted by D(X), asserts that Z (X)Q/∼hom = Z (X)Q/∼num.
    [Show full text]
  • Arxiv:1710.02344V3 [Math.AG] 12 Jun 2019 Mirror Symmetry, Mixed Motives, and Ζ(3)
    Mirror symmetry, mixed motives, and ζ(3) Minhyong Kim1 and Wenzhe Yang2 1Mathematical Institute, University of Oxford 2Stanford Institute for Theoretical Physics June 14, 2019 Abstract In this paper, we present an application of mirror symmetry to arithmetic geometry. The main result is the computation of the period of a mixed Hodge structure, which lends evidence to its expected motivic origin. More precisely, given a mirror pair (M,W ) of Calabi-Yau threefolds, the prepotential of the complexified K¨ahler moduli space of M admits an expansion with a constant term that is frequently of the form −3 χ(M) ζ(3)/(2πi)3 + r, where r ∈ Q and χ(M) is the Euler characteristic of M. We focus on the mirror pairs for which the deformation space of the mirror threefold W forms part of a one-parameter algebraic family Wϕ defined over Q and the large complex structure limit is a rational point. Assuming a version of the mirror conjecture, we compute the limit mixed Hodge 3 structure on H (Wϕ) at the large complex structure limit. It turns out to have a direct summand expressible as an extension of Q(−3) by Q(0) whose isomorphism class can be computed in terms of the prepotential of M, and hence, involves ζ(3). By way arXiv:1710.02344v3 [math.AG] 12 Jun 2019 of Ayoub’s works on the motivic nearby cycle functor, this reveals in precise form a connection between mirror symmetry and a variant of the Hodge conjecture for mixed Tate motives. 0. Introduction Over 50 years of research on motives has continued to enrich virtually all areas of number theory and algebraic geometry with a wide-ranging supply of unifying themes as well as deep formulas.
    [Show full text]
  • Introduction to Motives
    Introduction to motives Sujatha Ramdorai and Jorge Plazas With an appendix by Matilde Marcolli Abstract. This article is based on the lectures of the same tittle given by the first author during the instructional workshop of the program \number theory and physics" at ESI Vienna during March 2009. An account of the topics treated during the lectures can be found in [24] where the categorical aspects of the theory are stressed. Although naturally overlapping, these two independent articles serve as complements to each other. In the present article we focus on the construction of the category of pure motives starting from the category of smooth projective varieties. The necessary preliminary material is discussed. Early accounts of the theory were given in Manin [21] and Kleiman [19], the material presented here reflects to some extent their treatment of the main aspects of the theory. We also survey the theory of endomotives developed in [5], this provides a link between the theory of motives and tools from quantum statistical mechanics which play an important role in results connecting number theory and noncommutative geometry. An extended appendix (by Matilde Marcolli) further elaborates these ideas and reviews the role of motives in noncommutative geometry. Introduction Various cohomology theories play a central role in algebraic geometry, these co- homology theories share common properties and can in some cases be related by specific comparison morphisms. A cohomology theory with coefficients in a ring R is given by a contra-variant functor H from the category of algebraic varieties over a field k to the category of graded R-algebras (or more generally to a R-linear tensor category).
    [Show full text]
  • G Aperf–Modules and De Rham Cohomology
    perf Ga –modules and de Rham Cohomology Shubhodip Mondal Abstract We prove that algebraic de Rham cohomology as a functor defined on smooth Fp–algebras is formally perf ´etale in a precise sense. To prove this, we define and study the notion of a pointed Ga –module and its perf refinement which we call a quasi-ideal in Ga following Drinfeld. Our results show that given de Rham cohomology, one obtains the theory of crystalline cohomology as its unique functorial deformation. Contents 1 Introduction 2 1.1 Overviewoftheresults............................... ......... 2 1.2 Motivationsandrelatedwork . ......... 5 1.3 Acknowledgements .................................. ........ 6 2 Modules over ring schemes 7 2.1 Ga–modules............................................ .. 7 Gperf 2.2 a –modules............................................ 8 2.3 TheHodgemap...................................... ...... 11 2.4 Cartierduality ...................................... ...... 12 G Gperf 2.5 Deformations of some a and a –modules ........................... 14 G Gperf 3 Construction of functors using a and a –modules 18 3.1 Tensoring a module with a module scheme. ......... 18 3.2 Unwinding pointed Ga–modules. .................................. 19 Gperf 3.3 Unwinding pointed a –modulesI. ................................ 23 Gperf 3.4 Unwinding pointed a –modulesII................................. 26 3.5 Hodgefiltration..................................... ....... 31 4 Review of de Rham and Crystalline cohomology 33 5 Formal ´etaleness of de Rham cohomology 35 arXiv:2101.03146v1 [math.AG] 8 Jan 2021 5.1 First proof using deformation theory of u∗W [F ]. ......................... 35 5.2 Second proof using deformation theory of W [F ]. ......................... 36 1 1 Introduction 1.1 Overview of the results Let X be a scheme over a field k. Grothendieck defined the algebraic de Rham cohomology of X to be the ∗ hypercohomology of the algebraic de Rham complex ΩX [Gro66].
    [Show full text]
  • Motives: an Introductory Survey for Physicists
    MOTIVES: AN INTRODUCTORY SURVEY FOR PHYSICISTS ABHIJNAN REJ (WITH AN APPENDIX BY MATILDE MARCOLLI) Abstract. We survey certain accessible aspects of Grothendieck's theory of motives in arith- metic algebraic geometry for mathematical physicists, focussing on areas that have recently found applications in quantum field theory. An appendix (by Matilde Marcolli) sketches further connections between motivic theory and theoretical physics. post hoc, ergo ante hoc { Umberto Eco, Interpretation and overinterpretation Contents 1. Introduction 1 2. The Grothendieck ring 2 3. The Tannakian formalism 6 4. Weil cohomology 12 5. Classical motives 15 6. Mixed motives 18 7. Motivic measures and zeta functions 22 8. Appendix: Motivic ideas in physics (by M.Marcolli) 24 References 29 1. Introduction This survey paper is based on lectures given by the author at Boston University, the Max Planck Institute in Bonn, at Durham university and at the Indian Statistical Institute and the SN Bose National Center for the Basic Sciences in Kolkata and the Indian Institute of Technology in Mumbai. The purpose of these introductory notes are to familiarize an audience of physicists with some of the algebraic and algebro-geometric background upon which Grothendieck's theory of motives of algebraic varieties relies. There have been many recent developments in the interactions between high energy physics and motives, mostly within the framework of perturbative quantum field theory and the evaluation of Feynman diagrams as periods of algebraic varieties, though motives are beginning to play an important role in other branched of theoretical physics, such as string theory, especially through the recent interactions with the Langlands program, and through the theory of BPS states.
    [Show full text]
  • Remarks on the Lefschetz Standard Conjecture and Hyperkähler Varieties
    Remarks on the Lefschetz standard conjecture and hyperk¨ahlervarieties Fran¸coisCharles DMA Ecole´ Normale Sup´erieure 45, rue d'Ulm 75230 Paris Cedex 05 FRANCE [email protected] Abstract. We study the Lefschetz standard conjecture on a smooth complex projective variety X. In degree 2, we reduce it to a local statement concerning local deformations of vector bundles on X. When X is hyperk¨ahler,we show that the existence of nontrivial deformations of stable hyperholomorphic bundles implies the Lefschetz standard conjecture in codimension 2. 1 Introduction In the fundamental paper [9] of 1968, Grothendieck states a series of conjectures concerning the existence of certain algebraic cycles on smooth projective algebraic varieties over an algebraically closed ground fields. Those are known as the standard conjectures. In par- ticular, given such a variety X of dimension n, the Lefschetz standard conjecture predicts the existence of self-correspondences on X that give an inverse to the operations Hk(X) ! H2n−k(X) given by the cup-product n − k times with a hyperplane section for all k ≤ n. Here H∗(X) stands for any Weil cohomology theory on X, e.g. singular cohomology if X is defined over C, or l-adic ´etalecohomology in characteristic different from l. If we can invert the morphism Hk(X) ! H2n−k(X) using self-correspondences on X, we say that the Lefschetz conjecture holds in degree k. Let us now, and for the rest of the paper, work over C. The Lefschetz standard con- jecture then implies the other ones and has strong theoretical consequences.
    [Show full text]
  • WEIL COHOMOLOGY THEORIES 0FFG Contents 1. Introduction 1 2
    WEIL COHOMOLOGY THEORIES 0FFG Contents 1. Introduction 1 2. Conventions and notation 2 3. Correspondences 3 4. Chow motives 7 5. Chow groups of motives 12 6. Projective space bundle formula 13 7. Classical Weil cohomology theories 14 8. Cycles over non-closed fields 22 9. Weil cohomology theories, I 25 10. Further properties 34 11. Weil cohomology theories, II 38 12. Chern classes 41 13. Exterior powers and K-groups 46 14. Weil cohomology theories, III 47 15. Other chapters 58 References 59 1. Introduction 0FFH In this chapter we discuss Weil cohomology theories for smooth projective schemes over a base field. Briefly, for us such a cohomology theory H∗ is one which has Künneth, Poincaré duality, and cycle classes (with suitable compatibilities). We warn the reader that there is no universal agreement in the literature as to what constitutes a “Weil cohomology theory”. Before reading this chapter the reader should take a look at Categories, Section 42 and Homology, Section 17 where we define (symmetric) monoidal categories and we develop just enough basic language concerning these categories for the needs of this chapter. Equipped with this language we construct in Section 3 the symmetric monoidal graded category whose objects are smooth projective schemes and whose morphisms are correspondences. In Section 4 we add images of projectors and invert the Lefschetz motive in order to obtain the symmetric monoidal Karoubian category Mk of Chow motives. This category comes equipped with a contravariant functor h : {smooth projective schemes over k} −→ Mk As we will see below, a key property of a Weil cohomology theory is that it factors over h.
    [Show full text]
  • Supersymmetric Flux Compactifications and Calabi-Yau
    Supersymmetric Flux Compactifications and Calabi-Yau Modularity Shamit Kachru, Richard Nally, and Wenzhe Yang Stanford Institute for Theoretical Physics, Stanford University, Stanford, CA, 94305 March 31, 2020 Abstract Flux compactification of IIB string theory associates special points in Calabi-Yau moduli space to choices of (pairs of) integral three-form fluxes. In this paper, we propose that super- symmetric flux vacua are modular. That is, to a supersymmetric flux vacuum arising in a variety defined over Q, we associate a two-dimensional Galois representation that we conjecture to be modular. We provide numerical evidence for our conjecture by examining flux vacua arising on the octic hypersurface in P4(1, 1, 2, 2, 2). arXiv:2001.06022v2 [hep-th] 30 Mar 2020 1 Contents 1 Introduction 2 2 The Modularity of Calabi-Yau Varieties 4 2.1 ModularityForEllipticCurves . ......... 5 2.2 Modularity For Calabi-Yau Threefolds . ........... 6 2.3 ζ-FunctionsandTheWeilConjectures . ...... 8 3 Supersymmetric Flux Compactifications 11 4 Modularity From Supersymmetric Flux Compactifications 15 5 An Example: The Octic in P(1, 1, 2, 2, 2) 17 6 Conclusion 19 A ζ-Functions and the Greene-Plesser Mirror 21 B Weil Cohomology Theories, Motives, and the Hodge Conjecture 22 B.1 TheAbsoluteGaloisGroup . ...... 22 B.2 Classical Weil Cohomology Theories . .......... 23 B.3 L-functions ......................................... 26 B.4 AUniversalCohomologyTheory . ....... 27 B.5 Algebraic Cycles and Adequate Equivalence Relations . ............... 28 B.6 PureMotives ..................................... 29 B.7 The Hodge Conjecture and Motivic Splits . .......... 32 C Modularity of the Octic at Rational Points 33 C.1 φ = 1/2 ........................................... 34 C.2 φ = 3/5 ..........................................
    [Show full text]
  • Witt Vectors As a Polynomial Functor
    Witt vectors as a polynomial functor D. Kaledin∗ To Sasha Beilinson, on his birthday. Contents 1 Preliminaries. 6 1.1 Smallcategories. ......................... 6 1.2 Tracemaps............................. 7 1.3 Mackeyfunctors. ......................... 9 1.4 Fixedpointsandproducts. 11 1.5 The functor Q. .......................... 13 1.6 Cyclicgroups............................ 16 2 Witt vectors. 18 2.1 Preliminaries on cyclic groups. 18 2.2 Polynomial Witt vectors. 20 2.3 Restrictionmaps... .. .. .. .. .. .. 22 3 Basic properties. 25 3.1 Exact sequences and filtrations. 25 3.2 FrobeniusandVerschiebung. 28 3.3 Multiplication. .......................... 32 arXiv:1602.04254v3 [math.AG] 12 Oct 2017 3.4 Explicitdescriptions.. 35 4 Trace functors. 39 4.1 Definitionsandexamples. 39 4.2 Constructions. .......................... 42 4.3 Extensions. ............................ 44 ∗Partially supported by a subsidy granted to the HSE by the Government of the Russian Federation for the implementation of the Global Competitiveness Program. 1 Introduction. Recall that to any commutative ring A, one canonically associates the ring W (A) of p-typical Witt vectors of A (a reader not familiar with the subject can find a great overview for example in [I, Section 0.1]). Witt vectors are functorial in A, and W (A) is the inverse limit of rings Wm(A) of m-truncated p-typical Witt vectors numbered by integers m ≥ 1. We have W1(A) =∼ A, and for any m, Wm+1(A) is an extension of A by Wm(A). If A is annihilated by a prime p and perfect — that is, the Frobenius m endomorphism F : A → A is bijective — then one has Wm(A) =∼ W (A)/p , and in particular, A =∼ W (A)/p.
    [Show full text]
  • Weil Cohomology Theories This Is an Old Note on Weil Cohomology
    Weil cohomology theories This is an old note on Weil cohomology theories written for a graduate student seminar in the Fall of 2007 organized by Johan de Jong. It later became a chapter of the Stacks project. We strongly urge the reader to read this online at https://stacks.math.columbia.edu/tag/0FFG instead of reading the old material below. In particular, we do not vouch for the correctness of what follows. Fix an algebraically closed field C. All varieties will be varieties over C. See the end of this note for some remarks on what to change to get a Weil cohomology theory over a nonalgebraically closed field. A Weil cohomology theory H∗ with coefficients in the characteristic zero field K is given by the following set of data (notation explained below): (D1) For every nonsingular projective algebraic variety X a graded commutative algebra H∗(X) over ∗ n K. The grading is indexed by integers: H (X) = ⊕n2ZH (X) is a direct sum decomposition of K-vector spaces. The multiplication H∗(X) × H∗(X) ! H∗(X), (α; β) 7! α [ β is called the cup product. It is K-bilinear. Graded commutative means that α [ β = (−1)deg(α) deg(β)β [ α for homogenous elements. (D2) For every morphism of nonsingular projective varieties f : X ! Y a pullback map f ∗ : H∗(Y ) ! H∗(X) which is a K-algebra map preserving the grading. (D3) A 1-dimensional K-vector space K(1), which gives rise to Tate twists as follows. For a K-vector ⊗n ⊗−n space V we define V (n) = V ⊗K K(1) .
    [Show full text]