Three Lectures on Formal Groups 0. Introduction. F
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
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). -
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 . -
Contemporary Mathematics 220
CONTEMPORARY MATHEMATICS 220 Homotopy Theory via Algebraic Geometry and Group Representations Proceedings of a Conference on Homotopy Theory March 23-27, 1997 Northwestern University Mark Mahowald Stewart Priddy Editors http://dx.doi.org/10.1090/conm/220 Selected Titles in This Series 220 Mark Mahowald and Stewart Priddy, Editors, Homotopy theory via algebraic geometry and group representations, 1998 219 Marc Henneaux, Joseph Krasil'shchik, and Alexandre Vinogradov, Editors, Secondary calculus and cohomological physics, 1998 218 Jan Mandel, Charbel Farhat, and Xiao-Chuan Cai, Editors, Domain decomposition methods 10, 1998 217 Eric Carlen, Evans M. Harrell, and Michael Loss, Editors, Advances in differential equations and mathematical physics, 1998 216 Akram Aldroubi and EnBing Lin, Editors, Wavelets, multiwavelets, and their applications, 1998 215 M. G. Nerurkar, D.P. Dokken, and D. B. Ellis, Editors, Topological dynamics and applications, 1998 214 Lewis A. Coburn and Marc A. Rieffel, Editors, Perspectives on quantization, 1998 213 Farhad Jafari, Barbara D. MacCluer, Carl C. Cowen, and A. Duane Porter, Editors, Studies on composition operators, 1998 212 E. Ramirez de Arellano, N. Salinas, M. V. Shapiro, and N. L. Vasilevski, Editors, Operator theory for complex and hypercomplex analysis, 1998 211 J6zef Dodziuk and Linda Keen, Editors, Lipa's legacy: Proceedings from the Bers Colloquium, 1997 210 V. Kumar Murty and Michel Waldschmidt, Editors, Number theory, 1998 209 Steven Cox and Irena Lasiecka, Editors, Optimization methods in partial differential equations, 1997 208 MichelL. Lapidus, Lawrence H. Harper, and Adolfo J. Rumbos, Editors, Harmonic analysis and nonlinear differential equations: A volume in honor of Victor L. Shapiro, 1997 207 Yujiro Kawamata and Vyacheslav V. -
On Beta Elements in the Adams-Novikov Spectral Sequence
Submitted exclusively to the London Mathematical Society doi:10.1112/0000/000000 On β-elements in the Adams-Novikov spectral sequence Hirofumi Nakai and Douglas C. Ravenel Dedicated to Professor Takao Matumoto on his sixtieth birthday Abstract In this paper we detect invariants in the comodule consisting of β-elements over the Hopf algebroid (A(m + 1);G(m + 1)) defined in[Rav02], and we show that some related Ext groups vanish below a certain dimension. The result obtained here will be extensively used in [NR] to extend the range of our knowledge for π∗(T (m)) obtained in[Rav02]. Contents 1. Introduction ................ 1 2. The construction of Bm+1 ............. 5 3. Basic methods for finding comodule primitives ........ 8 4. 0-primitives in Bm+1 .............. 11 5. 1-primitives in Bm+1 .............. 13 6. j-primitives in Bm+1 for j > 1 ........... 16 7. Higher Ext groups for j = 1 ............ 20 Appendix A. Some results on binomial coefficients ........ 21 Appendix B. Quillen operations on β-elements ........ 24 References ................. 26 1. Introduction In this paper we describe some tools needed in the method of infinite descent, which is an approach to finding the E2-term of the Adams-Novikov spectral sequence converging to the stable homotopy groups of spheres. It is the subject of [Rav86, Chapter 7], [Rav04, Chapter 7] and [Rav02]. We begin by reviewing some notation. Fix a prime p. Recall the Brown-Peterson spectrum BP . Its homotopy groups and those of BP ^ BP are known to be polynomial algebras π∗(BP ) = Z(p)[v1; v2 :::] and BP∗(BP ) = BP∗[t1; t2 :::]: In [Rav86, Chapter 6] the second author constructed intermediate spectra 0 ::: S(p) = T (0) / T (1) / T (2) / T (3) / / BP with T (m) is equivalent to BP below the dimension of vm+1. -
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. -
Lecture Notes in Mathematics
Lecture Notes in Mathematics For information about Vols. 1-1145 please contact your bookseller Vol. 1173: H. DeHs, M. Knebusch, Locally Semialgebraic Spaces. XVI, or Springer-Verlag. 329 pages. 1g95, Vol. 1146: 5eminaire d'Aigebre Paul Dubreil et Marie-Paula Malliavin. Vol. 1174: Categories in Continuum Physics, Buffalo 1982. Seminar. Proceedings, 1g63-1984. Edite par M.-P. Malliavin. IV, 420 pages. Edited by F.W. Lawvere and S.H. Schanuel. V, t26 pages. t986. 1985. Vol. 1175: K. Mathiak, Valuations of Skew Fields and Projective Vol. 1147: M. Wschebor, Surfaces Aleatoires. VII, 11t pages. 1985. Hjelmslev Spaces. VII, 116 pages. 1986. Vol. 1t48: Mark A. Kon, Probability Distributions in Quantum Statistical Vol. 1176: R.R. Bruner, J.P. May, J.E. McClure, M. Steinberger, Mechanics. V, 12t pages. 1985. Hoo Ring Spectra and their Applications. VII, 388 pages. 1988. Vol. 1149: Universal Algebra and Lattice Theory. Proceedings, 1984. Vol. 1t77: Representation Theory I. Finite Dimensional Algebras. Edited by S. D. Comer. VI, 282 pages. 1985. Proceedings, t984. Edited by V. Dlab, P. Gabriel and G. Michler. XV, 340 pages. 1g86. Vol. 1150: B. Kawohl, Rearrangements and Convexity of Level Sets in Vol. 1178: Representation Theory II. Groups and Orders. Proceed PDE. V, 136 pages. 1985. ings, 1984. Edited by V. Dlab, P. Gabriel and G. Michler. XV, 370 Vol 1151: Ordinary and Partial Differential Equations. Proceedings, pages. 1986. 1984. Edited by B.D. Sleeman and R.J. Jarvis. XIV, 357 pages. 1985. Vol. 1179: Shi J .-Y. The Kazhdan-Lusztig Cells in Certain Affine Weyl Vol. 1152: H. Widom, Asymptotic Expansions for Pseudodifferential Groups. -
ON BEYOND HATCHER! in the Fall Semester of 2012, Constantin
ON BEYOND HATCHER! ERIC PETERSON In the Fall semester of 2012, Constantin Teleman encouraged me to run a short seminar which would teach attendees about advanced algebraic topology. UC-Berkeley runs a pair of graduate courses in algebraic topology which more or less go through Allen Hatcher’s Algebraic Topology, but there is a long road from there to the forefront of the field. Getting students research-ready inside of four seminar talks is an impossible task, of course, and so instead my goal is to sketch a picture of some of the major components of the field, so that students know enough of the flavor of the subject to at least identify whether they’re intrigued by its questions and its methods, and then further to know where to look to learn more. To reinforce the impression that there’s a lot going on in algebraic topology, each day will be very distinctly flavored from the others, and no day will require absolutely understanding any day that came before it. In the same vein, few things will be completely proven, but I hope to at least define the topological things under discussion. Some knowledge from related fields (algebraic geometry, primarily) will be assumed without hesitation. Each of these talks is meant to last roughly 50 minutes. The reader should additionally be warned that, due to my limited worldliness, these notes are bent sharply toward what I consider interesting. This means that they are highly algebraic, and they make no mention of exciting geometric things in stable homotopy theory — like string topology, for one example of many. -
Realising Unstable Modules As the Cohomology of Spaces and Mapping Spaces
Realising unstable modules as the cohomology of spaces and mapping spaces G´eraldGaudens and Lionel Schwartz UMR 7539 CNRS, Universit´eParis 13 LIA CNRS Formath Vietnam Abstract This report discuss the question whether or not a given unstable module is the mod-p cohomology of a space. One first discuss shortly the Hopf invariant 1 problem and the Kervaire invariant 1 problem and give their relations to homotopy theory and geometric topology. Then one describes some more qualitative results, emphasizing the use of the space map(BZ=p; X) and of the structure of the category of unstable modules. 1 Introduction Let p be a prime number, in all the sequel H∗X will denote the the mod p singular cohomology of the topological space X. All spaces X will be supposed p-complete and connected. The singular mod-p cohomology is endowed with various structures: • it is a graded Fp-algebra, commutative in the graded sense, • it is naturally a module over the algebra of stable cohomology operations which is known as the mod p Steenrod algebra and denoted by Ap. The Steenrod algebra is generated by element Sqi of degree i > 0 if p = 2, β and P i of degree 1 and 2i(p − 1) > 0 if p > 2. These elements satisfy the Adem relations. In the mod-2 case the relations write [a=2] X b − t − 1 SqaSqb = Sqa+b−tSqt a − 2t 0 There are two types of relations for p > 2 [a=p] X (p − 1)(b − t) − 1 P aP b = (−1)a+t P a+b−tP t a − pt 0 1 for a; b > 0, and [a=p] [(a−1)=p] X (p − 1)(b − t) X (p − 1)(b − t) − 1 P aβP b = (−1)a+t βP a+b−tP t+ (−1)a+t−1 P a+b−tβP t a − pt a − pt − 1 0 0 for a; b > 0. -
Arxiv:1909.13379V2 [Math.AT] 10 Jul 2021 6
THE TELESCOPE CONJECTURE AT HEIGHT 2 AND THE TMF RESOLUTION A. BEAUDRY, M. BEHRENS, P. BHATTACHARYA, D. CULVER, AND Z. XU Abstract. Mahowald proved the height 1 telescope conjecture at the prime 2 as an application of his seminal work on bo-resolutions. In this paper we study the height 2 telescope conjecture at the prime 2 through the lens of tmf-resolutions. To this end we compute the structure of the tmf-resolution for a specific type 2 complex Z. We find that, analogous to the height 1 case, the E1-page of the tmf-resolution possesses a decomposition into a v2- periodic summand, and an Eilenberg-MacLane summand which consists of bounded v2-torsion. However, unlike the height 1 case, the E2-page of the tmf-resolution exhibits unbounded v2-torsion. We compare this to the work of Mahowald-Ravenel-Shick, and discuss how the validity of the telescope con- jecture is connected to the fate of this unbounded v2-torsion: either the un- bounded v2-torsion kills itself off in the spectral sequence, and the telescope conjecture is true, or it persists to form v2-parabolas and the telescope conjec- ture is false. We also study how to use the tmf-resolution to effectively give low dimensional computations of the homotopy groups of Z. These computations allow us to prove a conjecture of the second author and Egger: the E(2)-local Adams-Novikov spectral sequence for Z collapses. Contents 1. Introduction2 2. Background 11 3. The good/evil decomposition of the E1-term 15 4. Morava stabilizer groups and algebras 20 5. -
RESEARCH STATEMENT My Research Lies in the Area of Stable Homotopy Theory. This Is the Part of Homotopy Theory Which Studies
RESEARCH STATEMENT D. CULVER 1. INTRODUCTION My research lies in the area of stable homotopy theory. This is the part of homotopy theory which studies invariants of spaces that are stable under the suspension functor. My research primarily focuses on studying pat- terns that arise in the stable homotopy groups of finite complexes, with a particular emphasis on spheres. I am especially interested in computing infinite periodic families in the stable homotopy groups of spheres. Most of my research can be described as studying these families by using Adams type spectral sequences based on interesting ring spectra. The primary case of interest is the ring spectrum tmf of topological modular forms. I have also become interested in studying the analogous problems in motivic and equi- variant homotopy theory. In addition, I am computing invariants of ring spectra such as topological Hochschild homology, topological cyclic homology, and algebraic K-theory. 2. BACKGROUND A natural tool for approaching the stable homotopy groups of spheres is the classical Adams spectral sequences (ASS). This is a spectral sequence of the form Exts,t , 0 , A (Fp Fp ) = πt s S Zp ∗ ) − ⊗ where p is a prime number. This spectral sequence is particularly good for computing the stable homotopy groups in a finite range, but obscures infinite patterns in the stable homotopy groups of spheres. However, given any ring spectrum E 1, one can always construct an ASS based on E. Under suitable conditions, this spectral sequence takes the form 0 ExtE E (E , E ) = π LE S . ∗ ∗ ∗ ∗ 0 ) Here E E = π (E E) and LE S is a certain localization of the sphere. -
A Combinatorial Model for the Known Bousfield Classes
A combinatorial model for the known Bousfield classes N. P. STRICKLAND We give a combinatorial construction of an ordered semiring A, and show that it can be identified with a certain subquotient of the semiring of p•local Bousfield classes, containing almost all of the classes that have previously been named and studied. This is a convenient way to encapsulate most of the known results about Bousfield classes. 1 Introduction Fix a prime p, and let L denote the set of Bousfield classes in the p•local stable category (which can be regarded as an ordered semiring in a natural way). This note is an attempt to organise many of the known results about the structure of L in a more coherent way. One of the main open questions about L is Ravenel’s Telescope Conjecture (TC). The statement will be recalled in Remark 4.2. Many people suspect that TC is false, but this has still not been proven. We will define an ordered semiring L which is, in a certain sense, the largest quotient of L in which TC becomes true. We will then define (in an explicit, combinatorial way) another ordered semiring A and a function φ: A→L arXiv:1608.08533v2 [math.AT] 8 Jul 2018 such that the composite φ π A −→L −→ L is an injective homomorphism of ordered semirings. (However, φ itself is probably not a semiring homomorphism, unless TC holds.) For almost all elements x ∈L that have been named and studied, we have π(x) ∈ πφ(A). Thus, A is a good model for the known part of L.