Zeta Functions of Finite Graphs and Coverings, III
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Class Numbers of Quadratic Fields Ajit Bhand, M Ram Murty
Class Numbers of Quadratic Fields Ajit Bhand, M Ram Murty To cite this version: Ajit Bhand, M Ram Murty. Class Numbers of Quadratic Fields. Hardy-Ramanujan Journal, Hardy- Ramanujan Society, 2020, Volume 42 - Special Commemorative volume in honour of Alan Baker, pp.17 - 25. hal-02554226 HAL Id: hal-02554226 https://hal.archives-ouvertes.fr/hal-02554226 Submitted on 1 May 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. Hardy-Ramanujan Journal 42 (2019), 17-25 submitted 08/07/2019, accepted 07/10/2019, revised 15/10/2019 Class Numbers of Quadratic Fields Ajit Bhand and M. Ram Murty∗ Dedicated to the memory of Alan Baker Abstract. We present a survey of some recent results regarding the class numbers of quadratic fields Keywords. class numbers, Baker's theorem, Cohen-Lenstra heuristics. 2010 Mathematics Subject Classification. Primary 11R42, 11S40, Secondary 11R29. 1. Introduction The concept of class number first occurs in Gauss's Disquisitiones Arithmeticae written in 1801. In this work, we find the beginnings of modern number theory. Here, Gauss laid the foundations of the theory of binary quadratic forms which is closely related to the theory of quadratic fields. -
Li's Criterion and Zero-Free Regions of L-Functions
CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector Journal of Number Theory 111 (2005) 1–32 www.elsevier.com/locate/jnt Li’s criterion and zero-free regions of L-functions Francis C.S. Brown A2X, 351 Cours de la Liberation, F-33405 Talence cedex, France Received 9 September 2002; revised 10 May 2004 Communicated by J.-B. Bost Abstract −s/ Let denote the Riemann zeta function, and let (s) = s(s− 1) 2(s/2)(s) denote the completed zeta function. A theorem of X.-J. Li states that the Riemann hypothesis is true if and only if certain inequalities Pn() in the first n coefficients of the Taylor expansion of at s = 1 are satisfied for all n ∈ N. We extend this result to a general class of functions which includes the completed Artin L-functions which satisfy Artin’s conjecture. Now let be any such function. For large N ∈ N, we show that the inequalities P1(),...,PN () imply the existence of a certain zero-free region for , and conversely, we prove that a zero-free region for implies a certain number of the Pn() hold. We show that the inequality P2() implies the existence of a small zero-free region near 1, and this gives a simple condition in (1), (1), and (1), for to have no Siegel zero. © 2004 Elsevier Inc. All rights reserved. 1. Statement of results 1.1. Introduction Let (s) = s(s − 1)−s/2(s/2)(s), where is the Riemann zeta function. Li [5] proved that the Riemann hypothesis is equivalent to the positivity of the real parts E-mail address: [email protected]. -
Interlacing Families I: Bipartite Ramanujan Graphs of All Degrees
Annals of Mathematics 182 (2015), 307{325 Interlacing families I: Bipartite Ramanujan graphs of all degrees By Adam W. Marcus, Daniel A. Spielman, and Nikhil Srivastava Abstract We prove that there exist infinite families of regular bipartite Ramanujan graphs of every degree bigger than 2. We do this by proving a variant of a conjecture of Bilu and Linial about the existence of good 2-lifts of every graph. We also establish the existence of infinite families of \irregular Ramanujan" graphs, whose eigenvalues are bounded by the spectral radius of their universal cover. Such families were conjectured to exist by Linial and others. In particular, we prove the existence of infinite families of (c; d)-biregular bipartite graphs with all nontrivial eigenvalues bounded by p p c − 1 + d − 1 for all c; d ≥ 3. Our proof exploits a new technique for controlling the eigenvalues of certain random matrices, which we call the \method of interlacing polynomials." 1. Introduction Ramanujan graphs have been the focus of substantial study in Theoret- ical Computer Science and Mathematics. They are graphs whose nontrivial adjacency matrix eigenvalues are as small as possible. Previous constructions of Ramanujan graphs have been sporadic, only producing infinite families of Ramanujan graphs of certain special degrees. In this paper, we prove a variant of a conjecture of Bilu and Linial [4] and use it to realize an approach they suggested for constructing bipartite Ramanujan graphs of every degree. Our main technical contribution is a novel existence argument. The con- jecture of Bilu and Linial requires us to prove that every graph has a signed adjacency matrix with all of its eigenvalues in a small range. -
Ramanujan Graphs of Every Degree
Ramanujan Graphs of Every Degree Adam Marcus (Crisply, Yale) Daniel Spielman (Yale) Nikhil Srivastava (MSR India) Expander Graphs Sparse, regular well-connected graphs with many properties of random graphs. Random walks mix quickly. Every set of vertices has many neighbors. Pseudo-random generators. Error-correcting codes. Sparse approximations of complete graphs. Spectral Expanders Let G be a graph and A be its adjacency matrix a 0 1 0 0 1 b 1 0 1 0 1 e 0 1 0 1 0 c 0 0 1 0 1 1 1 0 1 0 d Eigenvalues λ1 λ2 λn “trivial” ≥ ≥ ···≥ If d-regular (every vertex has d edges), λ1 = d Spectral Expanders If bipartite (all edges between two parts/colors) eigenvalues are symmetric about 0 If d-regular and bipartite, λ = d n − “trivial” a b 0 0 0 1 0 1 0 0 0 1 1 0 0 0 0 0 1 1 c d 1 1 0 0 0 0 0 1 1 0 0 0 e f 1 0 1 0 0 0 Spectral Expanders G is a good spectral expander if all non-trivial eigenvalues are small [ ] -d 0 d Bipartite Complete Graph Adjacency matrix has rank 2, so all non-trivial eigenvalues are 0 a b 0 0 0 1 1 1 0 0 0 1 1 1 0 0 0 1 1 1 c d 1 1 1 0 0 0 1 1 1 0 0 0 e f 1 1 1 0 0 0 Spectral Expanders G is a good spectral expander if all non-trivial eigenvalues are small [ ] -d 0 d Challenge: construct infinite families of fixed degree Spectral Expanders G is a good spectral expander if all non-trivial eigenvalues are small [ ] ( 0 ) -d 2pd 1 2pd 1 d − − − Challenge: construct infinite families of fixed degree Alon-Boppana ‘86: Cannot beat 2pd 1 − Ramanujan Graphs: 2pd 1 − G is a Ramanujan Graph if absolute value of non-trivial eigs 2pd 1 − [ -
X-Ramanujan-Graphs.Pdf
X-Ramanujan graphs Sidhanth Mohanty* Ryan O’Donnell† April 4, 2019 Abstract Let X be an infinite graph of bounded degree; e.g., the Cayley graph of a free product of finite groups. If G is a finite graph covered by X, it is said to be X-Ramanujan if its second- largest eigenvalue l2(G) is at most the spectral radius r(X) of X, and more generally k-quasi- X-Ramanujan if lk(G) is at most r(X). In case X is the infinite D-regular tree, this reduces to the well known notion of a finite D-regular graph being Ramanujan. Inspired by the Interlacing Polynomials method of Marcus, Spielman, and Srivastava, we show the existence of infinitely many k-quasi-X-Ramanujan graphs for a variety of infinite X. In particular, X need not be a tree; our analysis is applicable whenever X is what we call an additive product graph. This additive product is a new construction of an infinite graph A1 + ··· + Ac from finite “atom” graphs A1,..., Ac over a common vertex set. It generalizes the notion of the free product graph A1 ∗ · · · ∗ Ac when the atoms Aj are vertex-transitive, and it generalizes the notion of the uni- versal covering tree when the atoms Aj are single-edge graphs. Key to our analysis is a new graph polynomial a(A1,..., Ac; x) that we call the additive characteristic polynomial. It general- izes the well known matching polynomial m(G; x) in case the atoms Aj are the single edges of G, and it generalizes the r-characteristic polynomial introduced in [Rav16, LR18]. -
And Siegel's Theorem We Used Positivi
Math 259: Introduction to Analytic Number Theory A nearly zero-free region for L(s; χ), and Siegel's theorem We used positivity of the logarithmic derivative of ζq to get a crude zero-free region for L(s; χ). Better zero-free regions can be obtained with some more effort by working with the L(s; χ) individually. The situation is most satisfactory for 2 complex χ, that is, for characters with χ = χ0. (Recall that real χ were also the characters that gave us the most difficulty6 in the proof of L(1; χ) = 0; it is again in the neighborhood of s = 1 that it is hard to find a good zero-free6 region for the L-function of a real character.) To obtain the zero-free region for ζ(s), we started with the expansion of the logarithmic derivative ζ 1 0 (s) = Λ(n)n s (σ > 1) ζ X − − n=1 and applied the inequality 1 0 (z + 2 +z ¯)2 = Re(z2 + 4z + 3) = 3 + 4 cos θ + cos 2θ (z = eiθ) ≤ 2 it iθ s to the phases z = n− = e of the terms n− . To apply the same inequality to L 1 0 (s; χ) = χ(n)Λ(n)n s; L X − − n=1 it it we must use z = χ(n)n− instead of n− , obtaining it 2 2it 0 Re 3 + 4χ(n)n− + χ (n)n− : ≤ σ Multiplying by Λ(n)n− and summing over n yields L0 L0 L0 0 3 (σ; χ ) + 4 Re (σ + it; χ) + Re (σ + 2it; χ2) : (1) ≤ − L 0 − L − L 2 Now we see why the case χ = χ0 will give us trouble near s = 1: for such χ the last term in (1) is within O(1) of Re( (ζ0/ζ)(σ + 2it)), so the pole of (ζ0/ζ)(s) at s = 1 will undo us for small t . -
SPEECH: SIEGEL ZERO out Line: 1. Introducing the Problem of Existence of Infinite Primes in Arithmetic Progressions (Aps), 2. Di
SPEECH: SIEGEL ZERO MEHDI HASSANI Abstract. We talk about the effect of the positions of the zeros of Dirichlet L-function in the distribution of prime numbers in arithmetic progressions. We point to effect of possible existence of Siegel zero on above distribution, distribution of twin primes, entropy of black holes, and finally in the size of least prime in arithmetic progressions. Out line: 1. Introducing the problem of existence of infinite primes in Arithmetic Progressions (APs), 2. Dirichlet characters and Dirichlet L-functions, 3. Brief review of Dirichlet's proof, and pointing importance of L(1; χ) 6= 0 in proof, 4. About the zeros of Dirichlet L-functions: Zero Free Regions (ZFR), Siegel zero and Siegel's theorem, 5. Connection between zeros of L-functions and distribution of primes in APs: Explicit formula, 6. Prime Number Theorem (PNT) for APs, 7. More about Siegel zero and the problem of least prime in APs. Extended abstract: After introducing the problem of existence of infinite primes in the arithmetic progression a; a + q; a + 2q; ··· with (a; q) = 1, we give some fast information about Dirichlet characters and Dirichlet L-functions: mainly we write orthogonality relations for Dirichlet characters and Euler product for L-fucntions, and after taking logarithm we arrive at 1 X X (1) χ(a) log L(s; χ) = m−1p−ms '(q) χ p;m pm≡a [q] where the left sum is over all '(q) characters molulo q, and in the right sum m rins over all positive integers and p runs over all primes. -
Arxiv:1511.09340V2 [Math.NT] 25 Mar 2017 from Below by Logk−1(N) and It Could Get As Large As a Scalar Multiple of N
DIAMETER OF RAMANUJAN GRAPHS AND RANDOM CAYLEY GRAPHS NASER T SARDARI Abstract. We study the diameter of LPS Ramanujan graphs Xp;q. We show that the diameter of the bipartite Ramanujan graphs is greater than (4=3) logp(n) + O(1) where n is the number of vertices of Xp;q. We also con- struct an infinite family of (p + 1)-regular LPS Ramanujan graphs Xp;m such that the diameter of these graphs is greater than or equal to b(4=3) logp(n)c. On the other hand, for any k-regular Ramanujan graph we show that the distance of only a tiny fraction of all pairs of vertices is greater than (1 + ) logk−1(n). We also have some numerical experiments for LPS Ramanu- jan graphs and random Cayley graphs which suggest that the diameters are asymptotically (4=3) logk−1(n) and logk−1(n), respectively. Contents 1. Introduction 1 1.1. Motivation 1 1.2. Statement of results 3 1.3. Outline of the paper 5 1.4. Acknowledgments 5 2. Lower bound for the diameter of the Ramanujan graphs 6 3. Visiting almost all points after (1 + ) logk−1(n) steps 9 4. Numerical Results 11 References 14 1. Introduction 1.1. Motivation. The diameter of any k-regular graph with n vertices is bounded arXiv:1511.09340v2 [math.NT] 25 Mar 2017 from below by logk−1(n) and it could get as large as a scalar multiple of n. It is known that the diameter of any k-regular Ramanujan graph is bounded from above by 2(1 + ) logk−1(n) [LPS88]. -
RAMANUJAN GRAPHS and SHIMURA CURVES What Follows
RAMANUJAN GRAPHS AND SHIMURA CURVES PETE L. CLARK What follows are some long, rambling notes of mine on Ramanujan graphs. For a period of about two months in 2006 I thought very intensely on this subject and had thoughts running in several different directions. In paricular this document contains the most complete exposition so far of my construction of expander graphs using Hecke operators on Shimura curves. I am posting this document now (March 2009) by request of John Voight. Introduction Let q be a positive integer. A finite, connected graph G in which each vertex has degree q +1 and for which every eigenvalue λ of the adjacency matrix A(G) satisfies √ |λ| = q + 1 (such eigenvalues are said to be trivial) or |λ| ≤ 2 q is a Ramanujan graph, and an infinite sequence Gi of pairwise nonisomorphic Ramanujan graphs of common vertex degree q + 1 is called a Ramanujan family. These definitions may not in themselves arouse immediate excitement, but in fact the search for Ramanujan families of vertex degree q + 1 has made for some of the most intriguing and beautiful mathematics of recent times. In this paper we offer a survey of the theory of Ramanujan graphs and families, together with a new result and a “new” perspective in terms of relations to (Drinfeld-)Shimura curves. We must mention straightaway that the literature already contains many fine surveys on Ramanujan graphs: especially recommended are the introductory treat- ment of Murty [?], the short book of Davidoff, Sarnak and Vallette [?] (which can be appreciated by undergraduates and research mathematicians alike), and the beau- tiful books of Sarnak [?] and Lubotzsky [?], which are especially deft at exposing connections to many different areas of mathematics. -
Standard Zero-Free Regions for Rankin–Selberg L-Functions
STANDARD ZERO-FREE REGIONS FOR RANKIN–SELBERG L-FUNCTIONS VIA SIEVE THEORY PETER HUMPHRIES, WITH AN APPENDIX BY FARRELL BRUMLEY Abstract. We give a simple proof of a standard zero-free region in the t- aspect for the Rankin–Selberg L-function L(s,π × πe) for any unitary cuspidal automorphic representation π of GLn(AF ) that is tempered at every nonar- chimedean place outside a set of Dirichlet density zero. 1. Introduction Let F be a number field, let n be a positive integer, and let π be a unitary cuspidal automorphic representation of GLn(AF ) with L-function L(s, π), with π normalised such that its central character is trivial on the diagonally embedded copy of the positive reals. The proof of the prime number theorem due to de la Valle´e-Poussin gives a zero-free region for the Riemann zeta function ζ(s) of the form c σ> 1 − log(|t| + 3) for s = σ + it, and this generalises to a zero-free region for L(s, π) of the form c (1.1) σ ≥ 1 − (n[F : Q])4 log(q(π)(|t| + 3)) for some absolute constant c> 0, where q(π) is the analytic conductor of π in the sense of [IK04, Equation (5.7], with the possible exception of a simple real-zero βπ < 1 when π is self-dual. A proof of this is given in [IK04, Theorem 5.10]; the method requires constructing an auxiliary L-function having a zero of higher order than the order of the pole at s = 1, then using an effective version of Landau’s lemma [IK04, Lemma 5.9]. -
Spectra of Graphs
Spectra of graphs Andries E. Brouwer Willem H. Haemers 2 Contents 1 Graph spectrum 11 1.1 Matricesassociatedtoagraph . 11 1.2 Thespectrumofagraph ...................... 12 1.2.1 Characteristicpolynomial . 13 1.3 Thespectrumofanundirectedgraph . 13 1.3.1 Regulargraphs ........................ 13 1.3.2 Complements ......................... 14 1.3.3 Walks ............................. 14 1.3.4 Diameter ........................... 14 1.3.5 Spanningtrees ........................ 15 1.3.6 Bipartitegraphs ....................... 16 1.3.7 Connectedness ........................ 16 1.4 Spectrumofsomegraphs . 17 1.4.1 Thecompletegraph . 17 1.4.2 Thecompletebipartitegraph . 17 1.4.3 Thecycle ........................... 18 1.4.4 Thepath ........................... 18 1.4.5 Linegraphs .......................... 18 1.4.6 Cartesianproducts . 19 1.4.7 Kronecker products and bipartite double. 19 1.4.8 Strongproducts ....................... 19 1.4.9 Cayleygraphs......................... 20 1.5 Decompositions............................ 20 1.5.1 Decomposing K10 intoPetersengraphs . 20 1.5.2 Decomposing Kn into complete bipartite graphs . 20 1.6 Automorphisms ........................... 21 1.7 Algebraicconnectivity . 22 1.8 Cospectralgraphs .......................... 22 1.8.1 The4-cube .......................... 23 1.8.2 Seidelswitching. 23 1.8.3 Godsil-McKayswitching. 24 1.8.4 Reconstruction ........................ 24 1.9 Verysmallgraphs .......................... 24 1.10 Exercises ............................... 25 3 4 CONTENTS 2 Linear algebra 29 2.1 -
Spectral Graph Theory
Spectral Graph Theory Max Hopkins Dani¨elKroes Jiaxi Nie [email protected] [email protected] [email protected] Jason O'Neill Andr´esRodr´ıguezRey Nicholas Sieger [email protected] [email protected] [email protected] Sam Sprio [email protected] Winter 2020 Quarter Abstract Spectral graph theory is a vast and expanding area of combinatorics. We start these notes by introducing and motivating classical matrices associated with a graph, and then show how to derive combinatorial properties of a graph from the eigenvalues of these matrices. We then examine more modern results such as polynomial interlacing and high dimensional expanders. 1 Introduction These notes are comprised from a lecture series for graduate students in combinatorics at UCSD during the Winter 2020 Quarter. The organization of these expository notes is as follows. Each section corresponds to a fifty minute lecture given as part of the seminar. The first set of sections loosely deals with associating some specific matrix to a graph and then deriving combinatorial properties from its spectrum, and the second half focus on expanders. Throughout we use standard graph theory notation. In particular, given a graph G, we let V (G) denote its vertex set and E(G) its edge set. We write e(G) = jE(G)j, and for (possibly non- disjoint) sets A and B we write e(A; B) = jfuv 2 E(G): u 2 A; v 2 Bgj. We let N(v) denote the neighborhood of the vertex v and let dv denote its degree. We write u ∼ v when uv 2 E(G).