Noncommutative Geometry and Number Theory
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Determining Large Groups and Varieties from Small Subgroups and Subvarieties
Determining large groups and varieties from small subgroups and subvarieties This course will consist of two parts with the common theme of analyzing a geometric object via geometric sub-objects which are `small' in an appropriate sense. In the first half of the course, we will begin by describing the work on H. W. Lenstra, Jr., on finding generators for the unit groups of subrings of number fields. Lenstra discovered that from the point of view of computational complexity, it is advantageous to first consider the units of the ring of S-integers of L for some moderately large finite set of places S. This amounts to allowing denominators which only involve a prescribed finite set of primes. We will de- velop a generalization of Lenstra's method which applies to find generators of small height for the S-integral points of certain algebraic groups G defined over number fields. We will focus on G which are compact forms of GLd for d ≥ 1. In the second half of the course, we will turn to smooth projective surfaces defined by arithmetic lattices. These are Shimura varieties of complex dimension 2. We will try to generate subgroups of finite index in the fundamental groups of these surfaces by the fundamental groups of finite unions of totally geodesic projective curves on them, that is, via immersed Shimura curves. In both settings, the groups we will study are S-arithmetic lattices in a prod- uct of Lie groups over local fields. We will use the structure of our generating sets to consider several open problems about the geometry, group theory, and arithmetic of these lattices. -
Noncommutative Geometry and the Spectral Model of Space-Time
S´eminaire Poincar´eX (2007) 179 – 202 S´eminaire Poincar´e Noncommutative geometry and the spectral model of space-time Alain Connes IHES´ 35, route de Chartres 91440 Bures-sur-Yvette - France Abstract. This is a report on our joint work with A. Chamseddine and M. Marcolli. This essay gives a short introduction to a potential application in physics of a new type of geometry based on spectral considerations which is convenient when dealing with noncommutative spaces i.e. spaces in which the simplifying rule of commutativity is no longer applied to the coordinates. Starting from the phenomenological Lagrangian of gravity coupled with matter one infers, using the spectral action principle, that space-time admits a fine structure which is a subtle mixture of the usual 4-dimensional continuum with a finite discrete structure F . Under the (unrealistic) hypothesis that this structure remains valid (i.e. one does not have any “hyperfine” modification) until the unification scale, one obtains a number of predictions whose approximate validity is a basic test of the approach. 1 Background Our knowledge of space-time can be summarized by the transition from the flat Minkowski metric ds2 = − dt2 + dx2 + dy2 + dz2 (1) to the Lorentzian metric 2 µ ν ds = gµν dx dx (2) of curved space-time with gravitational potential gµν . The basic principle is the Einstein-Hilbert action principle Z 1 √ 4 SE[ gµν ] = r g d x (3) G M where r is the scalar curvature of the space-time manifold M. This action principle only accounts for the gravitational forces and a full account of the forces observed so far requires the addition of new fields, and of corresponding new terms SSM in the action, which constitute the Standard Model so that the total action is of the form, S = SE + SSM . -
Space and Time Dimensions of Algebras With
Space and time dimensions of algebras with applications to Lorentzian noncommutative geometry and quantum electrodynamics Nadir Bizi, Christian Brouder, Fabien Besnard To cite this version: Nadir Bizi, Christian Brouder, Fabien Besnard. Space and time dimensions of algebras with appli- cations to Lorentzian noncommutative geometry and quantum electrodynamics. Journal of Mathe- matical Physics, American Institute of Physics (AIP), 2018, 59 (6), pp.062303. 10.1063/1.4986228. hal-01398231v2 HAL Id: hal-01398231 https://hal.archives-ouvertes.fr/hal-01398231v2 Submitted on 16 May 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Space and time dimensions of algebras with application to Lorentzian noncommutative geometry and quantum electrodynamics Nadir Bizi, Christian Brouder, and Fabien Besnard Citation: Journal of Mathematical Physics 59, 062303 (2018); doi: 10.1063/1.5010424 View online: https://doi.org/10.1063/1.5010424 View Table of Contents: http://aip.scitation.org/toc/jmp/59/6 Published by the American Institute of Physics Articles you may -
Noncommutative Geometry and Flavour Mixing
Noncommutative geometry and flavour mixing prepared by Jose´ M. Gracia-Bond´ıa Department of Theoretical Physics Universidad de Zaragoza, 50009 Zaragoza, Spain October 22, 2013 1 Introduction: the universality problem “The origin of the quark and lepton masses is shrouded in mystery” [1]. Some thirty years ago, attempts to solve the enigma based on textures of the quark mass matrices, purposedly reflecting mass hierarchies and “nearest-neighbour” interactions, were very popular. Now, in the late eighties, Branco, Lavoura and Mota [2] showed that, within the SM, the zero pattern 0a b 01 @c 0 dA; (1) 0 e 0 a central ingredient of Fritzsch’s well-known Ansatz for the mass matrices, is devoid of any particular physical meaning. (The top quark is above on top.) Although perhaps this was not immediately clear at the time, paper [2] marked a water- shed in the theory of flavour mixing. In algebraic terms, it establishes that the linear subspace of matrices of the form (1) is universal for the group action of unitaries effecting chiral basis transformations, that respect the charged-current term of the Lagrangian. That is, any mass matrix can be transformed to that form without modifying the corresponding CKM matrix. To put matters in perspective, consider the unitary group acting by similarity on three-by- three matrices. The classical triangularization theorem by Schur ensures that the zero patterns 0a 0 01 0a b c1 @b c 0A; @0 d eA (2) d e f 0 0 f are universal in this sense. However, proof that the zero pattern 0a b 01 @0 c dA e 0 f 1 is universal was published [3] just three years ago! (Any off-diagonal n(n−1)=2 zero pattern with zeroes at some (i j) and no zeroes at the matching ( ji), is universal in this sense, for complex n × n matrices.) Fast-forwarding to the present time, notwithstanding steady experimental progress [4] and a huge amount of theoretical work by many authors, we cannot be sure of being any closer to solving the “Meroitic” problem [5] of divining the spectrum behind the known data. -
Noncommutative Stacks
Noncommutative Stacks Introduction One of the purposes of this work is to introduce a noncommutative analogue of Artin’s and Deligne-Mumford algebraic stacks in the most natural and sufficiently general way. We start with quasi-coherent modules on fibered categories, then define stacks and prestacks. We define formally smooth, formally unramified, and formally ´etale cartesian functors. This provides us with enough tools to extend to stacks the glueing formalism we developed in [KR3] for presheaves and sheaves of sets. Quasi-coherent presheaves and sheaves on a fibered category. Quasi-coherent sheaves on geometric (i.e. locally ringed topological) spaces were in- troduced in fifties. The notion of quasi-coherent modules was extended in an obvious way to ringed sites and toposes at the moment the latter appeared (in SGA), but it was not used much in this generality. Recently, the subject was revisited by D. Orlov in his work on quasi-coherent sheaves in commutative an noncommutative geometry [Or] and by G. Laumon an L. Moret-Bailly in their book on algebraic stacks [LM-B]. Slightly generalizing [R4], we associate with any functor F (regarded as a category over a category) the category of ’quasi-coherent presheaves’ on F (otherwise called ’quasi- coherent presheaves of modules’ or simply ’quasi-coherent modules’) and study some basic properties of this correspondence in the case when the functor defines a fibered category. Imitating [Gir], we define the quasi-topology of 1-descent (or simply ’descent’) and the quasi-topology of 2-descent (or ’effective descent’) on the base of a fibered category (i.e. -
Noncommutative Geometry, the Spectral Standpoint Arxiv
Noncommutative Geometry, the spectral standpoint Alain Connes October 24, 2019 In memory of John Roe, and in recognition of his pioneering achievements in coarse geometry and index theory. Abstract We update our Year 2000 account of Noncommutative Geometry in [68]. There, we de- scribed the following basic features of the subject: I The natural “time evolution" that makes noncommutative spaces dynamical from their measure theory. I The new calculus which is based on operators in Hilbert space, the Dixmier trace and the Wodzicki residue. I The spectral geometric paradigm which extends the Riemannian paradigm to the non- commutative world and gives a new tool to understand the forces of nature as pure gravity on a more involved geometric structure mixture of continuum with the discrete. I The key examples such as duals of discrete groups, leaf spaces of foliations and de- formations of ordinary spaces, which showed, very early on, that the relevance of this new paradigm was going far beyond the framework of Riemannian geometry. Here, we shall report1 on the following highlights from among the many discoveries made since 2000: 1. The interplay of the geometry with the modular theory for noncommutative tori. 2. Great advances on the Baum-Connes conjecture, on coarse geometry and on higher in- dex theory. 3. The geometrization of the pseudo-differential calculi using smooth groupoids. 4. The development of Hopf cyclic cohomology. 5. The increasing role of topological cyclic homology in number theory, and of the lambda arXiv:1910.10407v1 [math.QA] 23 Oct 2019 operations in archimedean cohomology. 6. The understanding of the renormalization group as a motivic Galois group. -
On the Generalized Non-Commutative Sphere and Their K-Theory
Global Journal of Pure and Applied Mathematics. ISSN 0973-1768 Volume 12, Number 2 (2016), pp. 1325-1335 © Research India Publications http://www.ripublication.com On the generalized non-commutative sphere and their K-theory Saleh Omran Taif University, Faculty of Science, Taif , KSA South valley university, Faculty of science, Math. Dep. Qena , Egypt. Abstract In the work we follow the work of J.Cuntz, he associate a universal C* - algebra to every locally finite flag simplicial complex. In this article we define * nc a universal C -algebra S3 , associated to the 3 -dimensional noncommutative sphere. We analyze the topological information of the noncommutative sphere by using it’s skeleton filtration Ik )( . We examine the nc K -theory of the quotient 3 /IS k , and I k for such kk 7, . Keywords: Universal C* -algebra , Noncommutative sphere, K -theory of C* -algebra. 2000 AMS : 19 K 46. 1. Introduction Noncommutative 3 -sphere play an important role in the non commutative geometry which introduced by Allain Connes [4] .In noncommutative geometry, the set of points in the space are replaced by the set of continuous functions on the space. In fact noncommutative geometry change our point of view from the topological space itself to the functions on the space ( The algebra of functions on the space). Indeed, the main idea was noticed first by Gelfand-Niemark [8] they were give an important theorem which state that: any commutative C* -algebra is isomorphic of the continuous functions of a compact space, namely the space of characters of the algebra. More generally any C* -algebra ( commutative or not) is isomorphic to a closed subalgebra of the algebra of bounded operators on a Hilbert space. -
What Is Noncommutative Geometry ? How a Geometry Can Be Commutative and Why Mine Is Not
What is Noncommutative Geometry ? How a geometry can be commutative and why mine is not Alessandro Rubin Junior Math Days 2019/20 SISSA - Scuola Internazionale Superiore di Studi Avanzati This means that the algebra C∞(M) contains enough information to codify the whole geometry of the manifold: 1. Vector fields: linear derivations of C∞(M) 2. Differential 1-forms: C∞(M)-linear forms on vector fields 3. ... Question Do we really need a manifold’s points to study it ? Do we really use the commutativity of the algebra C∞(M) to define the aforementioned objects ? Doing Geometry Without a Geometric Space Theorem Two smooth manifolds M, N are diffeomorphic if and only if their algebras of smooth functions C∞(M) and C∞(N) are isomorphic. 1/41 Question Do we really need a manifold’s points to study it ? Do we really use the commutativity of the algebra C∞(M) to define the aforementioned objects ? Doing Geometry Without a Geometric Space Theorem Two smooth manifolds M, N are diffeomorphic if and only if their algebras of smooth functions C∞(M) and C∞(N) are isomorphic. This means that the algebra C∞(M) contains enough information to codify the whole geometry of the manifold: 1. Vector fields: linear derivations of C∞(M) 2. Differential 1-forms: C∞(M)-linear forms on vector fields 3. ... 1/41 Do we really use the commutativity of the algebra C∞(M) to define the aforementioned objects ? Doing Geometry Without a Geometric Space Theorem Two smooth manifolds M, N are diffeomorphic if and only if their algebras of smooth functions C∞(M) and C∞(N) are isomorphic. -
CHARACTERS of ALGEBRAIC GROUPS OVER NUMBER FIELDS Bachir Bekka, Camille Francini
CHARACTERS OF ALGEBRAIC GROUPS OVER NUMBER FIELDS Bachir Bekka, Camille Francini To cite this version: Bachir Bekka, Camille Francini. CHARACTERS OF ALGEBRAIC GROUPS OVER NUMBER FIELDS. 2020. hal-02483439 HAL Id: hal-02483439 https://hal.archives-ouvertes.fr/hal-02483439 Preprint submitted on 18 Feb 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. CHARACTERS OF ALGEBRAIC GROUPS OVER NUMBER FIELDS BACHIR BEKKA AND CAMILLE FRANCINI Abstract. Let k be a number field, G an algebraic group defined over k, and G(k) the group of k-rational points in G: We deter- mine the set of functions on G(k) which are of positive type and conjugation invariant, under the assumption that G(k) is gener- ated by its unipotent elements. An essential step in the proof is the classification of the G(k)-invariant ergodic probability measures on an adelic solenoid naturally associated to G(k); this last result is deduced from Ratner's measure rigidity theorem for homogeneous spaces of S-adic Lie groups. 1. Introduction Let k be a field and G an algebraic group defined over k. When k is a local field (that is, a non discrete locally compact field), the group G = G(k) of k-rational points in G is a locally compact group for the topology induced by k. -
Non-Vanishing of L-Functions, the Ramanujan Conjecture, and Families of Hecke Characters
NON-VANISHING OF L-FUNCTIONS, THE RAMANUJAN CONJECTURE, AND FAMILIES OF HECKE CHARACTERS VALENTIN BLOMER AND FARRELL BRUMLEY Abstract. We prove a non-vanishing result for families of GLn × GLn Rankin-Selberg L-functions in the critical strip, as one factor runs over twists by Hecke characters. As an application, we simplify the proof, due to Luo, Rudnick, and Sarnak, of the best known bounds towards the Generalized Ramanujan Conjecture at the infinite places for cusp forms on GLn. A key ingredient is the regularization of the units in residue classes by the use of an Arakelov ray class group. 1. Introduction In this paper we prove a non-vanishing result for Rankin-Selberg L-functions for cusp forms on GLn when one factor ranges over twists by infinite order Hecke characters and give applications to bounds towards the Ramunujan conjecture. 1.1. Infinite order Hecke characters. Before stating our precise results, we enunciate two ways, one automorphic, the other arithmetic, in which infinite order Hecke characters have been put to use to solve problems in number theory whose formulation is naturally posed over number fields. The first is the principle that a cusp form (for the group GL2 at least) should always be taken together with its twists by mod 1 Grossencharacters. This philosophy has been attributed to Sarnak and has its origins in the hybrid mean value estimate of [31]. A striking justification is the recent article by Booker and Krishnamurthy [5] where it is shown that for an irreducible two dimensional complex representation ρ of the Weil-Deligne group, if the Artin-Weil L-function L(s; ρ !) is entire for all mod 1 Grossencharacters ! then ρ is automorphic. -
Quantum Information Hidden in Quantum Fields
Preprints (www.preprints.org) | NOT PEER-REVIEWED | Posted: 21 July 2020 Peer-reviewed version available at Quantum Reports 2020, 2, 33; doi:10.3390/quantum2030033 Article Quantum Information Hidden in Quantum Fields Paola Zizzi Department of Brain and Behavioural Sciences, University of Pavia, Piazza Botta, 11, 27100 Pavia, Italy; [email protected]; Phone: +39 3475300467 Abstract: We investigate a possible reduction mechanism from (bosonic) Quantum Field Theory (QFT) to Quantum Mechanics (QM), in a way that could explain the apparent loss of degrees of freedom of the original theory in terms of quantum information in the reduced one. This reduction mechanism consists mainly in performing an ansatz on the boson field operator, which takes into account quantum foam and non-commutative geometry. Through the reduction mechanism, QFT reveals its hidden internal structure, which is a quantum network of maximally entangled multipartite states. In the end, a new approach to the quantum simulation of QFT is proposed through the use of QFT's internal quantum network Keywords: Quantum field theory; Quantum information; Quantum foam; Non-commutative geometry; Quantum simulation 1. Introduction Until the 1950s, the common opinion was that quantum field theory (QFT) was just quantum mechanics (QM) plus special relativity. But that is not the whole story, as well described in [1] [2]. There, the authors mainly say that the fact that QFT was "discovered" in an attempt to extend QM to the relativistic regime is only historically accidental. Indeed, QFT is necessary and applied also in the study of condensed matter, e.g. in the case of superconductivity, superfluidity, ferromagnetism, etc. -
Zeros of Dirichlet L-Functions Over Function Fields
ZEROS OF DIRICHLET L-FUNCTIONS OVER FUNCTION FIELDS JULIO C. ANDRADE, STEVEN J. MILLER, KYLE PRATT, AND MINH-TAM TRINH ABSTRACT. Random matrix theory has successfully modeled many systems in physics and math- ematics, and often the analysis and results in one area guide development in the other. Hughes and Rudnick computed 1-level density statistics for low-lying zeros of the family of primitive Dirichlet L-functions of fixed prime conductor Q, as Q , and verified the unitary symmetry predicted by random matrix theory. We compute 1- and 2→-level ∞ statistics of the analogous family of Dirichlet L-functions over Fq(T ). Whereas the Hughes-Rudnick results were restricted by the support of the Fourier transform of their test function, our test function is periodic and our results are only restricted by a decay condition on its Fourier coefficients. We show the main terms agree with unitary sym- metry, and also isolate error terms. In concluding, we discuss an Fq(T )-analogue of Montgomery’s Hypothesis on the distribution of primes in arithmetic progressions, which Fiorilli and Miller show would remove the restriction on the Hughes-Rudnick results. CONTENTS 1. Introduction 1 2. Dirichlet L-Function Preliminaries 6 3. The 1-Level Global Regime 7 4. The 2-Level Global Regime 11 5. The Local Regime 13 6. Montgomery’s Hypothesis 16 Appendix A. Proof of the Explicit Formula 18 Appendix B. Traces of the Frobenius Class 19 References 20 1. INTRODUCTION arXiv:1404.2435v1 [math.NT] 9 Apr 2014 1.1. Background. In the 1970s, Montgomery and Dyson conjectured that local statistics of crit- ical zeros of the Riemann zeta function—in the limit of large height—should match those of angles of eigenvalues of matrices in the Gaussian Unitary Ensemble (GUE), which Wigner, Dyson and others (see [FirM] for a historical overview) had already used with great success in modeling the energy levels of heavy nuclei.