Formal Groups Laws and Genera*
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Problems About Formal Groups and Cohomology Theories Arizona Winter School 2019
PROBLEMS ABOUT FORMAL GROUPS AND COHOMOLOGY THEORIES ARIZONA WINTER SCHOOL 2019 VESNA STOJANOSKA 1. Formal Group Laws In this document, a formal group law over a commutative ring R is always com- mutative and one-dimensional. Specifically, it is a power series F (x; y) 2 R[[x; y]] satisfying the following axioms: • F (x; 0) = x = F (0; x), • F (x; y) = F (y; x), and • F (x; F (y; z)) = F (F (x; y); z). Sometimes we denote F (x; y) by x +F y. For a non-negative integer n, the n-series of F is defined inductively by [0]F x = 0, and [n + 1]F x = x +F [n]F x. (1) Show that for any formal group law F (x; y) 2 R[[x; y]], x has a formal inverse. In other words, there is a power series i(x) 2 R[[x]] such that F (x; i(x)) = 0. As a consequence, we can define [−n]F x = i([n]F x). (2) Check that the following define formal group laws: (a) F (x; y) = x + y + uxy, where u is any unit in R. Also show that this is isomorphic to the multiplicative formal group law over R. x+y (b) F (x; y) = 1+xy . Hint: Note that if x = tanh(u) and y = tanh(v), then F (x; y) = tanh(x + y). (3) Suppose F; H are formal group laws over a complete local ring R, and we're given a morphism f : F ! H, i.e. f(x) 2 R[[x]] such that f(F (x; y)) = H(f(x); f(y)): Now let C be the category of complete local R-algebras and continuous maps between them; for T 2 C, denote by Spf(T ): C!Set the functor S 7! HomC(T;S). -
Generalized Rudin–Shapiro Sequences
ACTA ARITHMETICA LX.1 (1991) Generalized Rudin–Shapiro sequences by Jean-Paul Allouche (Talence) and Pierre Liardet* (Marseille) 1. Introduction 1.1. The Rudin–Shapiro sequence was introduced independently by these two authors ([21] and [24]) and can be defined by u(n) εn = (−1) , where u(n) counts the number of 11’s in the binary expansion of the integer n (see [5]). This sequence has the following property: X 2iπnθ 1/2 (1) ∀ N ≥ 0, sup εne ≤ CN , θ∈R n<N where one can take C = 2 + 21/2 (see [22] for improvements of this value). The order of magnitude of the left hand term in (1), as N goes to infin- 1/2 ity, is exactly N ; indeed, for each sequence (an) with values ±1 one has 1/2 X 2iπn(·) X 2iπn(·) N = ane ≤ ane , 2 ∞ n<N n<N where k k2 denotes the quadratic norm and k k∞ the supremum norm. Note that for almost every√ sequence (an) of ±1’s the supremum norm of the above sum is bounded by N Log N (see [23]). The inequality (1) has been generalized in [2] (see also [3]): X 2iπxu(n) 0 α(x) (2) sup f(n)e ≤ C N , f∈M2 n<N where M2 is the set of 2-multiplicative sequences with modulus 1. The * Research partially supported by the D.R.E.T. under contract 901636/A000/DRET/ DS/SR 2 J.-P. Allouche and P. Liardet exponent α(x) is explicitly given and satisfies ∀ x 1/2 ≤ α(x) ≤ 1 , ∀ x 6∈ Z α(x) < 1 , ∀ x ∈ Z + 1/2 α(x) = 1/2 . -
Fibonacci, Kronecker and Hilbert NKS 2007
Fibonacci, Kronecker and Hilbert NKS 2007 Klaus Sutner Carnegie Mellon University www.cs.cmu.edu/∼sutner NKS’07 1 Overview • Fibonacci, Kronecker and Hilbert ??? • Logic and Decidability • Additive Cellular Automata • A Knuth Question • Some Questions NKS’07 2 Hilbert NKS’07 3 Entscheidungsproblem The Entscheidungsproblem is solved when one knows a procedure by which one can decide in a finite number of operations whether a given logical expression is generally valid or is satisfiable. The solution of the Entscheidungsproblem is of fundamental importance for the theory of all fields, the theorems of which are at all capable of logical development from finitely many axioms. D. Hilbert, W. Ackermann Grundzuge¨ der theoretischen Logik, 1928 NKS’07 4 Model Checking The Entscheidungsproblem for the 21. Century. Shift to computer science, even commercial applications. Fix some suitable logic L and collection of structures A. Find efficient algorithms to determine A |= ϕ for any structure A ∈ A and sentence ϕ in L. Variants: fix ϕ, fix A. NKS’07 5 CA as Structures Discrete dynamical systems, minimalist description: Aρ = hC, i where C ⊆ ΣZ is the space of configurations of the system and is the “next configuration” relation induced by the local map ρ. Use standard first order logic (either relational or functional) to describe properties of the system. NKS’07 6 Some Formulae ∀ x ∃ y (y x) ∀ x, y, z (x z ∧ y z ⇒ x = y) ∀ x ∃ y, z (y x ∧ z x ∧ ∀ u (u x ⇒ u = y ∨ u = z)) There is no computability requirement for configurations, in x y both x and y may be complicated. -
Formal Groups, Witt Vectors and Free Probability
Formal Groups, Witt vectors and Free Probability Roland Friedrich and John McKay December 6, 2019 Abstract We establish a link between free probability theory and Witt vectors, via the theory of formal groups. We derive an exponential isomorphism which expresses Voiculescu's free multiplicative convolution as a function of the free additive convolution . Subsequently we continue our previous discussion of the relation between complex cobordism and free probability. We show that the generic nth free cumulant corresponds to the cobordism class of the (n 1)-dimensional complex projective space. This permits us to relate several probability distributions− from random matrix theory to known genera, and to build a dictionary. Finally, we discuss aspects of free probability and the asymptotic representation theory of the symmetric group from a conformal field theoretic perspective and show that every distribution with mean zero is embeddable into the Universal Grassmannian of Sato-Segal-Wilson. MSC 2010: 46L54, 55N22, 57R77, Keywords: Free probability and free operator algebras, formal group laws, Witt vectors, complex cobordism (U- and SU-cobordism), non-crossing partitions, conformal field theory. Contents 1 Introduction 2 2 Free probability and formal group laws4 2.1 Generalised free probability . .4 arXiv:1204.6522v3 [math.OA] 5 Dec 2019 2.2 The Lie group Aut( )....................................5 O 2.3 Formal group laws . .6 2.4 The R- and S-transform . .7 2.5 Free cumulants . 11 3 Witt vectors and Hopf algebras 12 3.1 The affine group schemes . 12 3.2 Witt vectors, λ-rings and necklace algebras . 15 3.3 The induced ring structure . -
Formal Group Rings of Toric Varieties 3
FORMAL GROUP RINGS OF TORIC VARIETIES WANSHUN WONG Abstract. In this paper we use formal group rings to construct an alge- braic model of the T -equivariant oriented cohomology of smooth toric vari- eties. Then we compare our algebraic model with known results of equivariant cohomology of toric varieties to justify our construction. Finally we construct the algebraic counterpart of the pull-back and push-forward homomorphisms of blow-ups. 1. Introduction Let h be an algebraic oriented cohomology theory in the sense of Levine-Morel [14], where examples include the Chow group of algebraic cycles modulo rational equivalence, algebraic K-theory, connective K-theory, elliptic cohomology, and a universal such theory called algebraic cobordism. It is known that to any h one can associate a one-dimensional commutative formal group law F over the coefficient ring R = h(pt), given by c1(L1 ⊗ L2)= F (c1(L1),c1(L2)) for any line bundles L1, L2 on a smooth variety X, where c1 is the first Chern class. Let T be a split algebraic torus which acts on a smooth variety X. An object of interest is the T -equivariant cohomology ring hT (X) of X, and we would like to build an algebraic model for it. More precisely, instead of using geometric methods to compute hT (X), we want to use algebraic methods to construct another ring A (our algebraic model), such that A should be easy to compute and it gives infor- mation about hT (X). Of course the best case is that A and hT (X) are isomorphic. -
Congruences Between the Coefficients of the Tate Curve Via Formal Groups
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 128, Number 3, Pages 677{681 S 0002-9939(99)05133-3 Article electronically published on July 6, 1999 CONGRUENCES BETWEEN THE COEFFICIENTS OF THE TATE CURVE VIA FORMAL GROUPS ANTONIOS BROUMAS (Communicated by David E. Rohrlich) 2 3 Abstract. Let Eq : Y + XY = X + h4X + h6 be the Tate curve with canonical differential, ! = dX=(2Y + X). If the characteristic is p>0, then the Hasse invariant, H, of the pair (Eq;!) should equal one. If p>3, then calculation of H leads to a nontrivial separable relation between the coefficients h4 and h6.Ifp=2orp= 3, Thakur related h4 and h6 via elementary methods and an identity of Ramanujan. Here, we treat uniformly all characteristics via explicit calculation of the formal group law of Eq. Our analysis was motivated by the study of the invariant A which is an infinite Witt vector generalizing the Hasse invariant. 1. Introduction The Tate curve in characteristic either zero or positive is an elliptic curve with canonical Weierstrass model: 2 3 (1) Eq : Y + XY = X + h4X + h6 5S +7S nk where h = 5S and h = 3 5 for S = : 4 − 3 6 − 12 k 1 qn n 1 X≥ − Note that the denominator appearing in the expression of h6 is simply a nota- tional convenience and in fact Eq is defined over Z[[q]]. Hence, since all coefficients are integral, we can specialize to positive characteristic p for any prime p of our choice and obtain Eq defined over Fp[[q]]. In all positive characteristics the Hasse invariant of the pair (Eq;!)for!the canonical invariant differential, ! = dX=(2Y + X), is equal to 1. -
FORMAL SCHEMES and FORMAL GROUPS Contents 1. Introduction 2
FORMAL SCHEMES AND FORMAL GROUPS NEIL P. STRICKLAND Contents 1. Introduction 2 1.1. Notation and conventions 3 1.2. Even periodic ring spectra 3 2. Schemes 3 2.1. Points and sections 6 2.2. Colimits of schemes 8 2.3. Subschemes 9 2.4. Zariski spectra and geometric points 11 2.5. Nilpotents, idempotents and connectivity 12 2.6. Sheaves, modules and vector bundles 13 2.7. Faithful flatness and descent 16 2.8. Schemes of maps 22 2.9. Gradings 24 3. Non-affine schemes 25 4. Formal schemes 28 4.1. (Co)limits of formal schemes 29 4.2. Solid formal schemes 31 4.3. Formal schemes over a given base 33 4.4. Formal subschemes 35 4.5. Idempotents and formal schemes 38 4.6. Sheaves over formal schemes 39 4.7. Formal faithful flatness 40 4.8. Coalgebraic formal schemes 42 4.9. More mapping schemes 46 5. Formal curves 49 5.1. Divisors on formal curves 49 5.2. Weierstrass preparation 53 5.3. Formal differentials 56 5.4. Residues 57 6. Formal groups 59 6.1. Group objects in general categories 59 6.2. Free formal groups 63 6.3. Schemes of homomorphisms 65 6.4. Cartier duality 66 6.5. Torsors 67 7. Ordinary formal groups 69 Date: November 17, 2000. 1 2 NEIL P. STRICKLAND 7.1. Heights 70 7.2. Logarithms 72 7.3. Divisors 72 8. Formal schemes in algebraic topology 73 8.1. Even periodic ring spectra 73 8.2. Schemes associated to spaces 74 8.3. -
The Hirzebruch Genera of Complete Intersections 3
THE HIRZEBRUCH GENERA OF COMPLETE INTERSECTIONS JIANBO WANG, ZHIWANG YU, YUYU WANG Abstract. Following Brooks’s calculation of the Aˆ-genus of complete intersections, a new and more computable formula about the Aˆ-genus and α-invariant will be described as polynomials of multi-degree and dimension. We also give an iterated formula of Aˆ-genus and the necessary and sufficient conditions for the vanishing of Aˆ-genus of complex even dimensional spin complete intersections. Finally, we obtain a general formula about the Hirzebruch genus of complete intersections, and calculate some classical Hirzebruch genera as examples. 1. Introduction A genus of a multiplicative sequence is a ring homomorphism, from the ring of smooth compact manifolds (up to suitable cobordism) to another ring. A multiplicative se- quence is completely determined by its characteristic power series Q(x). Moreover, ev- ery power series Q(x) determines a multiplicative sequence. Given a power series Q(x), there is an associated Hirzebruch genus, which is also denoted as a ϕQ-genus. For more details, please see Section 2. The focus of this paper is mainly on the description of the Hirzebruch genus of complete intersections with multi-degree and dimension. n+r A complex n-dimensional complete intersection Xn(d1,...,dr) CP is a smooth complex n-dimensional manifold given by a transversal intersection⊂ of r nonsin- gular hypersurfaces in complex projective space. The unordered r-tuple d := (d1,...,dr) is called the multi-degree, which denotes the degrees of the r nonsingular hypersur- faces, and the product d := d1d2 dr is called the total degree. -
Lectures on Lubin-Tate Spaces Arizona Winter School March 2019 (Incomplete Draft)
Lectures on Lubin-Tate spaces Arizona Winter School March 2019 (Incomplete draft) M. J. Hopkins Department of Mathematics, Harvard University, Cambridge, MA 02138 Email address: [email protected] Contents Introduction5 Prerequisites5 Lecture 1. Lubin-Tate spaces7 1.1. Overview7 1.2. Height8 1.3. Deformations of formal groups9 1.4. Formal complex multiplication in local fields 10 1.5. Formal moduli for one-parameter formal Lie groups 13 1.6. Deformations a la Kodaira-Spencer 14 Lecture 2. Toward explicit formulas 17 2.1. Differentials and the log 17 2.2. p-typical coordinates 19 2.3. Hazewinkel's functional equation lemma 20 2.4. The Hazewinkel parameters 22 2.5. Dieudonn´emodules 23 2.6. Dieudonn´emodules and logarithms 25 2.7. Tapis de Cartier 26 2.8. Cleaning things up 29 Lecture 3. Crystals 31 3.1. A further formula 31 3.2. Periods 33 3.3. Crystals 36 3.4. The crystalline period map 46 Lecture 4. The crystalline approximation 49 Lecture 5. Projects 51 5.1. Project: finite subgroups 51 5.2. Project: Action of finite subgroups 52 5.3. Project: Line bundles in height 2 53 Bibliography 61 3 Introduction Lubin-Tate formal groups and their moduli play a surprising number of roles in mathematics, especially in number theory and algebraic topology. In number theory, the formal groups were originally used to construct the local class field theory isomorphism. Many years later a program emerged to use the moduli spaces to realize the local Langlands correspondence. In algebraic topology, thanks to Quillen, 1-dimensional commutative formal groups appear in the Adams-Novikov spectral sequence relating complex cobordism groups to stable homotopy groups, and through the work of Morava and many others, the Lubin-Tate groups lead to the \chromatic" picture of homotopy theory. -
Formal Group Laws
Formal group laws November 25, 2012 The additive formal group Ga plays a fundamental role in the theory. We will see in the first section that up to isomorphism this is the only formal group over a Q-algebra. This is far from true over other rings. The ring of endomorphisms of a formal group over a Q-algebra R is canonically iso- morphic to R. In general things are more complicated, even for the additive formal group. For example, as we will see in Section 3, the endomorphism ring of Ga over rings of characteristic p is quite interesting. It is related to the algebra of Steenrod reduced powers, familiar from algebraic topology. A wish to establish an analogue of Ga affording the full Steenrod algebra at an odd prime leads to the amusing project of working out the \super" analogue of formal groups, in Section 4. The final section is a misfit in this chapter: it is devoted to the relationship between the multiplicative group and gradings. 1 Formal group laws In studying formal groups one often picks a parameter and so obtains by transport of structure a \formal group law": Definition 1.1 A formal group law over R is a formal group over R whose underlying formal scheme is D. The group structure on D = Spf R[[t]] given by a formal group law is defined by an augmented (and hence automatically continuous) R-algebra homomorphism R[[t]] ! R[[t]]⊗^ R[[t]] = R[[u; v]] (where u = t ⊗ 1; v = 1 ⊗ t). This homomorphism is determined by the image of t, which is a formal power 1 series F (u; v) 2 R[[u; v]] such that F (0; v) = v; F (u; 0) = u; F (F (u; v); w) = F (u; F (v; w)); F (u; v) = F (v; u): It is easy to check inductively that there is a power series [−1]F (u) such that F ([−1]F (u); u) = 0 = F (u; [−1]F (u)), so we do not need to assume the existence of an inverse. -
Three Lectures on Formal Groups 0. Introduction. F
Canadian Mathematical Society Conference Proceedings Volume 5 {1986} Three Lectures on Formal Groups Michie/ Hazewinkel CWI. Amsterdam Abstract and Preface. This paper is the written version of a series of three lectures given in Windsor at the occasion of the Cana dian Mathematical Society's summer school in Lie algebras and related topics in July 1984. They were antended as in introduction to the subject for an algebraically oriented audience with special emphasis on the kind of phenomena that appear when dealing with commutative formal groups over rings (rather than fields). Proofs and more details of most everything can be found in [9]. I am (and was) most grateful for the oppor tunity to speak on this topic and heartily thank the organising committee, notably Bob Moody. and the local organizers, the two friendly giants Dan Britten and Frank Lemire. for the opportunity. The phenomena are extraordinary rich in the commutative case-privately I suspect (with admittedly little grounds) especially in the commutative case - and much work remains to be done to get even a first idea of what the noncomrnutative theory has in store. These written notes follow the original lectures in structure but contain rather more. The contents are: 0) Introduction; I) Two classes of examples of formal groups from other parts of mathematics; 2) Generalities and bialgebras: 3) The Lie algebra of a formal group. Characteristic zero formal Lie theory: 4) The commuta tivity theorem; 5) Logarithms; 6) The functional equation lemma. Examples of formal groups: 7) Universal formal groups. Generalities: 8) p-typical formal groups; 9) A universal p-typical formal group and a formal group universal over Z1pi-algebras; 10) Construction of a universal formal group; 11) Application to algebraic topology; 12) Atkin-Swinnerton Dyer congruences for elliptic curves; 13) Witt vectors: 14) Curves. -
TMF for Number Theorists
TMF for number theorists Paul VanKoughnett September 14, 2014 1 What is stable homotopy theory? k Stable homotopy theory starts with a question: what are the homotopy groups of spheres? We define πn+kS to be the group of homotopy classes of maps Sn+k ! Sk. We can suspend a sphere by placing it as the `equator' of a sphere one dimension higher. This construction is actually functorial, so we get maps k k+1 Σ: πn+kS ! πn+k+1S : The `stable' in `stable homotopy theory' means stabilization with respect to this suspension operation. Thus, we define k πnS = colimk πn+kS ; and make these stable homotopy groups of spheres π∗S the focus of our energy. One of the earliest theorems of this subject, the Freudenthal suspension theorem, implies that this colimit is always attained at a finite stage: k πnS = πn+kS for k ≥ n + 2: So if you'd like, we're studying the homotopy groups of sufficiently high-dimensional spheres. One can, and should, ask why, and I could give you a number of answers. One answer is that the original problem of calculating all the homotopy groups of spheres is so intractable that we might as well replace it with a slightly less intractable one. A second answer is that the stable stuff has a lot more structure than n+k k the unstable stuff: for example, π∗S is a graded ring, since we can compose two maps α : S ! S and β : Sm+j ! Sj only after suspending them: k Σm+j α Σ β Sn+k+m+j /Sk+m+j /Sk+j: A third answer is that, for whatever reason, the reduction has been extraordinarily fruitful.