Homogeneity and Prime Models in Trosion-Free Hyperbolic Groups
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Homogeneity and Algebraic Closure in Free Groups
Homogeneity and algebraic closure in free groups Abderezak Ould Houcine Universit´ede Mons, Universit´eLyon 1 Equations and First-order properties in Groups Montr´eal, 15 october 2010 Contents 1 Homogeneity & prime models Definitions Existential homogeneity & prime models Homogeneity 2 Algebraic & definable closure Definitions Constructibility over the algebraic closure A counterexample Homogeneity and algebraic closure in free groups Homogeneity & prime models Contents 1 Homogeneity & prime models Definitions Existential homogeneity & prime models Homogeneity 2 Algebraic & definable closure Definitions Constructibility over the algebraic closure A counterexample Homogeneity and algebraic closure in free groups Homogeneity & prime models Definitions Homogeneity & existential homogeneity Homogeneity and algebraic closure in free groups Homogeneity & prime models Definitions Homogeneity & existential homogeneity Let M be a countable model. Homogeneity and algebraic closure in free groups Homogeneity & prime models Definitions Homogeneity & existential homogeneity Let M be a countable model. Let ¯a ∈ Mn. Homogeneity and algebraic closure in free groups Homogeneity & prime models Definitions Homogeneity & existential homogeneity Let M be a countable model. Let ¯a ∈ Mn. The type of ¯a is defined by Homogeneity and algebraic closure in free groups Homogeneity & prime models Definitions Homogeneity & existential homogeneity Let M be a countable model. Let ¯a ∈ Mn. The type of ¯a is defined by tpM(¯a)= {ψ(¯x)|M |= ψ(¯a)}. Homogeneity and algebraic closure in free groups Homogeneity & prime models Definitions Homogeneity & existential homogeneity Let M be a countable model. Let ¯a ∈ Mn. The type of ¯a is defined by tpM(¯a)= {ψ(¯x)|M |= ψ(¯a)}. M is homogeneous Homogeneity and algebraic closure in free groups Homogeneity & prime models Definitions Homogeneity & existential homogeneity Let M be a countable model. -
Arxiv:1911.10534V3 [Math.AT] 17 Apr 2020 Statement
THE ANDO-HOPKINS-REZK ORIENTATION IS SURJECTIVE SANATH DEVALAPURKAR Abstract. We show that the map π∗MString ! π∗tmf induced by the Ando-Hopkins-Rezk orientation is surjective. This proves an unpublished claim of Hopkins and Mahowald. We do so by constructing an E1-ring B and a map B ! MString such that the composite B ! MString ! tmf is surjective on homotopy. Applications to differential topology, and in particular to Hirzebruch's prize question, are discussed. 1. Introduction The goal of this paper is to show the following result. Theorem 1.1. The map π∗MString ! π∗tmf induced by the Ando-Hopkins-Rezk orientation is surjective. This integral result was originally stated as [Hop02, Theorem 6.25], but, to the best of our knowledge, no proof has appeared in the literature. In [HM02], Hopkins and Mahowald give a proof sketch of Theorem 1.1 for elements of π∗tmf of Adams-Novikov filtration 0. The analogue of Theorem 1.1 for bo (namely, the statement that the map π∗MSpin ! π∗bo induced by the Atiyah-Bott-Shapiro orientation is surjective) is classical [Mil63]. In Section2, we present (as a warmup) a proof of this surjectivity result for bo via a technique which generalizes to prove Theorem 1.1. We construct an E1-ring A with an E1-map A ! MSpin. The E1-ring A is a particular E1-Thom spectrum whose mod 2 homology is given by the polynomial subalgebra 4 F2[ζ1 ] of the mod 2 dual Steenrod algebra. The Atiyah-Bott-Shapiro orientation MSpin ! bo is an E1-map, and so the composite A ! MSpin ! bo is an E1-map. -
The Center and the Commutator Subgroup in Hopfian Groups
The center and the commutator subgroup in hopfian groups 1~. I-hRSHON Polytechnic Institute of Brooklyn, Brooklyn, :N.Y., U.S.A. 1. Abstract We continue our investigation of the direct product of hopfian groups. Through- out this paper A will designate a hopfian group and B will designate (unless we specify otherwise) a group with finitely many normal subgroups. For the most part we will investigate the role of Z(A), the center of A (and to a lesser degree also the role of the commutator subgroup of A) in relation to the hopficity of A • B. Sections 2.1 and 2.2 contain some general results independent of any restric- tions on A. We show here (a) If A X B is not hopfian for some B, there exists a finite abelian group iv such that if k is any positive integer a homomorphism 0k of A • onto A can be found such that Ok has more than k elements in its kernel. (b) If A is fixed, a necessary and sufficient condition that A • be hopfian for all B is that if 0 is a surjective endomorphism of A • B then there exists a subgroup B. of B such that AOB-=AOxB.O. In Section 3.1 we use (a) to establish our main result which is (e) If all of the primary components of the torsion subgroup of Z(A) obey the minimal condition for subgroups, then A • is hopfian, In Section 3.3 we obtain some results for some finite groups B. For example we show here (d) If IB[ -~ p'q~.., q? where p, ql q, are the distinct prime divisors of ]B[ and ff 0 <e<3, 0~e~2 and Z(A) has finitely many elements of order p~ then A • is hopfian. -
Our Mathematical Universe: I. How the Monster Group Dictates All of Physics
October, 2011 PROGRESS IN PHYSICS Volume 4 Our Mathematical Universe: I. How the Monster Group Dictates All of Physics Franklin Potter Sciencegems.com, 8642 Marvale Drive, Huntington Beach, CA 92646. E-mail: [email protected] A 4th family b’ quark would confirm that our physical Universe is mathematical and is discrete at the Planck scale. I explain how the Fischer-Greiss Monster Group dic- tates the Standard Model of leptons and quarks in discrete 4-D internal symmetry space and, combined with discrete 4-D spacetime, uniquely produces the finite group Weyl E8 x Weyl E8 = “Weyl” SO(9,1). The Monster’s j-invariant function determines mass ratios of the particles in finite binary rotational subgroups of the Standard Model gauge group, dictates Mobius¨ transformations that lead to the conservation laws, and connects interactions to triality, the Leech lattice, and Golay-24 information coding. 1 Introduction 5. Both 4-D spacetime and 4-D internal symmetry space are discrete at the Planck scale, and both spaces can The ultimate idea that our physical Universe is mathematical be telescoped upwards mathematically by icosians to at the fundamental scale has been conjectured for many cen- 8-D spaces that uniquely combine into 10-D discrete turies. In the past, our marginal understanding of the origin spacetime with discrete Weyl E x Weyl E symmetry of the physical rules of the Universe has been peppered with 8 8 (not the E x E Lie group of superstrings/M-theory). huge gaps, but today our increased understanding of funda- 8 8 mental particles promises to eliminate most of those gaps to 6. -
§2. Elliptic Curves: J-Invariant (Jan 31, Feb 4,7,9,11,14) After
24 JENIA TEVELEV §2. Elliptic curves: j-invariant (Jan 31, Feb 4,7,9,11,14) After the projective line P1, the easiest algebraic curve to understand is an elliptic curve (Riemann surface of genus 1). Let M = isom. classes of elliptic curves . 1 { } We are going to assign to each elliptic curve a number, called its j-invariant and prove that 1 M1 = Aj . 1 1 So as a space M1 A is not very interesting. However, understanding A ! as a moduli space of elliptic curves leads to some breath-taking mathemat- ics. More generally, we introduce M = isom. classes of smooth projective curves of genus g g { } and M = isom. classes of curves C of genus g with points p , . , p C . g,n { 1 n ∈ } We will return to these moduli spaces later in the course. But first let us recall some basic facts about algebraic curves = compact Riemann surfaces. We refer to [G] and [Mi] for a rigorous and detailed exposition. §2.1. Algebraic functions, algebraic curves, and Riemann surfaces. The theory of algebraic curves has roots in analysis of Abelian integrals. An easiest example is the elliptic integral: in 1655 Wallis began to study the arc length of an ellipse (X/a)2 + (Y/b)2 = 1. The equation for the ellipse can be solved for Y : Y = (b/a) (a2 X2), − and this can easily be differentiated !to find bX Y ! = − . a√a2 X2 − 2 This is squared and put into the integral 1 + (Y !) dX for the arc length. Now the substitution x = X/a results in " ! 1 e2x2 s = a − dx, 1 x2 # $ − between the limits 0 and X/a, where e = 1 (b/a)2 is the eccentricity. -
Multiplicative Invariants and the Finite Co-Hopfian Property
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by UCL Discovery MULTIPLICATIVE INVARIANTS AND THE FINITE CO-HOPFIAN PROPERTY J. J. A. M. HUMPHREYS AND F. E. A. JOHNSON Abstract. A group is said to be finitely co-Hopfian when it contains no proper subgroup of finite index isomorphic to itself. It is known that irreducible lattices in semisimple Lie groups are finitely co-Hopfian. However, it is not clear, and does not appear to be known, whether this property is preserved under direct product. We consider a strengthening of the finite co-Hopfian condition, namely the existence of a non-zero multiplicative invariant, and show that, under mild restrictions, this property is closed with respect to finite direct products. Since it is also closed with respect to commensurability, it follows that lattices in linear semisimple groups of general type are finitely co-Hopfian. §0. Introduction. A group G is finitely co-Hopfian when it contains no proper subgroup of finite index isomorphic to itself. This condition has a natural geometric significance; if M is a smooth closed connected manifold whose fundamental group π1.M/ is finitely co-Hopfian, then any smooth mapping h V M ! M of maximal rank is automatically a diffeomorphism (cf. [8]). From an algebraic viewpoint, this condition is a weakening of a more familiar notion; recall that a group is said to be co-Hopfian when it contains no proper subgroup (of whatever index, finite or infinite) isomorphic to itself. Co-Hopfian groups are finitely co-Hopfian, but the converse is false, shown by the case of finitely generated non-abelian free groups, which are finitely co-Hopfian but not co-Hopfian. -
K3 Surfaces, N= 4 Dyons, and the Mathieu Group
K3 Surfaces, =4 Dyons, N and the Mathieu Group M24 Miranda C. N. Cheng Department of Physics, Harvard University, Cambridge, MA 02138, USA Abstract A close relationship between K3 surfaces and the Mathieu groups has been established in the last century. Furthermore, it has been observed recently that the elliptic genus of K3 has a natural inter- pretation in terms of the dimensions of representations of the largest Mathieu group M24. In this paper we first give further evidence for this possibility by studying the elliptic genus of K3 surfaces twisted by some simple symplectic automorphisms. These partition functions with insertions of elements of M24 (the McKay-Thompson series) give further information about the relevant representation. We then point out that this new “moonshine” for the largest Mathieu group is con- nected to an earlier observation on a moonshine of M24 through the 1/4-BPS spectrum of K3 T 2-compactified type II string theory. This insight on the symmetry× of the theory sheds new light on the gener- alised Kac-Moody algebra structure appearing in the spectrum, and leads to predictions for new elliptic genera of K3, perturbative spec- arXiv:1005.5415v2 [hep-th] 3 Jun 2010 trum of the toroidally compactified heterotic string, and the index for the 1/4-BPS dyons in the d = 4, = 4 string theory, twisted by elements of the group of stringy K3N isometries. 1 1 Introduction and Summary Recently there have been two new observations relating K3 surfaces and the largest Mathieu group M24. They seem to suggest that the sporadic group M24 naturally acts on the spectrum of K3-compactified string theory. -
Mathematische Zeitschrift
Math. Z. (2015) 279:811–848 DOI 10.1007/s00209-014-1395-2 Mathematische Zeitschrift Random walks on free solvable groups Laurent Saloff-Coste · Tianyi Zheng Received: 30 October 2013 / Accepted: 5 August 2014 / Published online: 4 November 2014 © Springer-Verlag Berlin Heidelberg 2014 Abstract For any finitely generated group G,letn → G (n) be the function that describes the rough asymptotic behavior of the probability of return to the identity element at time 2n of a symmetric simple random walk on G (this is an invariant of quasi-isometry). We determine this function when G is the free solvable group Sd,r of derived length d on r generators and some related groups. Mathematics Subject Classification 20F69 · 60J10 1 Introduction 1.1 The random walk group invariant G Let G be a finitely generated group. Given a probability measure μ on G, the random walk driven by μ (started at the identity element e of G)istheG-valued random process = ξ ...ξ (ξ )∞ Xn 1 n where i 1 is a sequence of independent identically distributed G-valued μ ∗ v( ) = ( )v( −1 ) random variables with law .Ifu g h u h h g denotes the convolution of two μ (n) functions u and v on G then the probability that Xn = g is given by Pe (Xn = g) = μ (g) where μ(n) is the n-fold convolution of μ. Given a symmetric set of generators S, the word-length |g| of g ∈ G is the minimal length of a word representing g in the elements of S. The associated volume growth function, r → VG,S(r), counts the number of elements of G with |g|≤r. -
Moonshines for L2(11) and M12
Moonshines for L2(11) and M12 Suresh Govindarajan Department of Physics Indian Institute of Technology Madras (Work done with my student Sutapa Samanta) Talk at the Workshop on Modular Forms and Black Holes @NISER, Bhubaneswar on January 13. 2017 Plan Introduction Some finite group theory Moonshine BKM Lie superalgebras Introduction Classification of Finite Simple Groups Every finite simple group is isomorphic to one of the following groups: (Source: Wikipedia) I A cyclic group with prime order; I An alternating group of degree at least 5; I A simple group of Lie type, including both I the classical Lie groups, namely the groups of projective special linear, unitary, symplectic, or orthogonal transformations over a finite field; I the exceptional and twisted groups of Lie type (including the Tits group which is not strictly a group of Lie type). I The 26 sporadic simple groups. The classification was completed in 2004 when Aschbacher and Smith filled the last gap (`the quasi-thin case') in the proof. Fun Reading: Symmetry and the Monster by Mark Ronan The sporadic simple groups I the Mathieu groups: M11, M12, M22, M23, M24; (found in 1861) I the Janko groups: J1, J2, J3, J4; (others 1965-1980) I the Conway groups; Co1, Co2, Co3; 0 I the Fischer groups; Fi22. Fi23, Fi24; I the Higman-Sims group; HS I the McLaughlin group: McL I the Held group: He; I the Rudvalis group Ru; I the Suzuki sporadic group: Suz; 0 I the O'Nan group: O N; I Harada-Norton group: HN; I the Lyons group: Ly; I the Thompson group: Th; I the baby Monster group: B and Sources: Wikipedia and Mark Ronan I the Fischer-Griess Monster group: M Monstrous Moonshine Conjectures I The j-function has the followed q-series: (q = exp(2πiτ)) j(τ)−744 = q−1+[196883+1] q+[21296876+196883+1] q2+··· I McKay observed that 196883 and 21296876 are the dimensions of the two smallest irreps of the Monster group. -
Arxiv:1307.5522V5 [Math.AG] 25 Oct 2013 Rnho Mathematics
JORDAN GROUPS AND AUTOMORPHISM GROUPS OF ALGEBRAIC VARIETIES ∗ VLADIMIR L. POPOV Steklov Mathematical Institute, Russian Academy of Sciences Gubkina 8, Moscow 119991, Russia and National Research University Higher School of Economics 20, Myasnitskaya Ulitsa, Moscow 101000, Russia [email protected] Abstract. The first section of this paper is focused on Jordan groups in abstract setting, the second on that in the settings of automorphisms groups and groups of birational self-maps of algebraic varieties. The ap- pendix contains formulations of some open problems and the relevant comments. MSC 2010: 20E07, 14E07 Key words: Jordan, Cremona, automorphism, birational map This is the expanded version of my talk, based on [Po10, Sect. 2], at the workshop Groups of Automorphisms in Birational and Affine Geometry, October 29–November 3, 2012, Levico Terme, Italy. The appendix is the expanded version of my notes on open problems posted on the site of this workshop [Po122]. Below k is an algebraically closed field of characteristic zero. Variety means algebraic variety over k in the sense of Serre (so algebraic group means algebraic group over k). We use without explanation standard nota- arXiv:1307.5522v5 [math.AG] 25 Oct 2013 tion and conventions of [Bo91] and [Sp98]. In particular, k(X) denotes the field of rational functions of an irreducible variety X. Bir(X) denotes the group of birational self-maps of an irreducible variety X. Recall that if X is the affine n-dimensional space An, then Bir(X) is called the Cremona group over k of rank n; we denote it by Crn (cf. -
Final Report (PDF)
GROUPS AND GEOMETRIES Inna Capdeboscq (Warwick, UK) Martin Liebeck (Imperial College London, UK) Bernhard Muhlherr¨ (Giessen, Germany) May 3 – 8, 2015 1 Overview of the field, and recent developments As groups are just the mathematical way to investigate symmetries, it is not surprising that a significant number of problems from various areas of mathematics can be translated into specialized problems about permutation groups, linear groups, algebraic groups, and so on. In order to go about solving these problems a good understanding of the finite and algebraic groups, especially the simple ones, is necessary. Examples of this procedure can be found in questions arising from algebraic geometry, in applications to the study of algebraic curves, in communication theory, in arithmetic groups, model theory, computational algebra and random walks in Markov theory. Hence it is important to improve our understanding of groups in order to be able to answer the questions raised by all these areas of application. The research areas covered at the meeting fall into three main inter-related topics. 1.1 Fusion systems and finite simple groups The subject of fusion systems has its origins in representation theory, but it has recently become a fast growing area within group theory. The notion was originally introduced in the work of L. Puig in the late 1970s; Puig later formalized this concept and provided a category-theoretical definition of fusion systems. He was drawn to create this new tool in part because of his interest in the work of Alperin and Broue,´ and modular representation theory was its first berth. It was then used in the field of homotopy theory to derive results about the p-completed classifying spaces of finite groups. -
The Independence of the Notions of Hopfian and Co-Hopfian Abelian P-Groups
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 143, Number 8, August 2015, Pages 3331–3341 http://dx.doi.org/10.1090/proc/12413 Article electronically published on April 23, 2015 THE INDEPENDENCE OF THE NOTIONS OF HOPFIAN AND CO-HOPFIAN ABELIAN P-GROUPS GABOR´ BRAUN AND LUTZ STRUNGMANN¨ (Communicated by Birge Huisgen-Zimmermann) Abstract. Hopfian and co-Hopfian Abelian groups have recently become of great interest in the study of algebraic and adjoint entropy. Here we prove that the existence of the following three types of infinite abelian p-groups of ℵ size less than 2 0 is independent of ZFC: (a) both Hopfian and co-Hopfian, (b) Hopfian but not co-Hopfian, (c) co-Hopfian but not Hopfian. All three ℵ types of groups of size 2 0 exist in ZFC. 1. Introduction A very simple result from linear algebra states that an endomorphism of a finite dimensional vector space is injective if and only if it is surjective and hence an isomorphism. However, an infinite dimensional vector space never has this property, as the standard shift endomorphisms show. Reinhold Baer [B] was the first to investigate these properties for Abelian groups rather than vector spaces. While he used the terminology Q-group and S-group, researchers now use the notions of Hopfian group and co-Hopfian group. These groups have arisen recently in the study of algebraic entropy and its dual, adjoint entropy; see e.g., [DGSZ, GG], which are the motivations for our work. Recall that an (Abelian) group G is Hopfian if every epimorphism G → G is an automorphism.