Symmetric Operators and Reproducing Kernel Hilbert Spaces
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Spectral Geometry Spring 2016
Spectral Geometry Spring 2016 Michael Magee Lecture 5: The resolvent. Last time we proved that the Laplacian has a closure whose domain is the Sobolev space H2(M)= u L2(M): u L2(M), ∆u L2(M) . { 2 kr k2 2 } We view the Laplacian as an unbounded densely defined self-adjoint operator on L2 with domain H2. We also stated the spectral theorem. We’ll now ask what is the nature of the pro- jection valued measure associated to the Laplacian (its ‘spectral decomposition’). Until otherwise specified, suppose M is a complete Riemannian manifold. Definition 1. The resolvent set of the Laplacian is the set of λ C such that λI ∆isa bijection of H2 onto L2 with a boundedR inverse (with respect to L2 norms)2 − 1 2 2 R(λ) (λI ∆)− : L (M) H (M). ⌘ − ! The operator R(λ) is called the resolvent of the Laplacian at λ. We write spec(∆) = C −R and call it the spectrum. Note that the projection valued measure of ∆is supported in R 0. Otherwise one can find a function in H2(M)where ∆ , is negative, but since can be≥ approximated in Sobolev norm by smooth functions, thish will contradicti ∆ , = g( , )Vol 0. (1) h i ˆ r r ≥ Note then the spectral theorem implies that the resolvent set contains C R 0 (use the Borel functional calculus). − ≥ Theorem 2 (Stone’s formula [1, VII.13]). Let P be the projection valued measure on R associated to the Laplacan by the spectral theorem. The following formula relates the resolvent to P b 1 1 lim(2⇡i)− [R(λ + i✏) R(λ i✏)] dλ = P[a,b] + P(a,b) . -
Unbounded Jacobi Matrices with a Few Gaps in the Essential Spectrum: Constructive Examples
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Springer - Publisher Connector Integr. Equ. Oper. Theory 69 (2011), 151–170 DOI 10.1007/s00020-010-1856-x Published online January 11, 2011 c The Author(s) This article is published Integral Equations with open access at Springerlink.com 2010 and Operator Theory Unbounded Jacobi Matrices with a Few Gaps in the Essential Spectrum: Constructive Examples Anne Boutet de Monvel, Jan Janas and Serguei Naboko Abstract. We give explicit examples of unbounded Jacobi operators with a few gaps in their essential spectrum. More precisely a class of Jacobi matrices whose absolutely continuous spectrum fills any finite number of bounded intervals is considered. Their point spectrum accumulates to +∞ and −∞. The asymptotics of large eigenvalues is also found. Mathematics Subject Classification (2010). Primary 47B36; Secondary 47A10, 47B25. Keywords. Jacobi matrix, essential spectrum, gaps, asymptotics. 1. Introduction In this paper we look for examples of unbounded Jacobi matrices with sev- 2 2 eral gaps in the essential spectrum. Let 0 = 0(N) be the space of sequences ∞ {fk}1 with a finite number of nonzero coordinates. For given real sequences ∞ ∞ 2 {ak}1 and {bk}1 the Jacobi operator J 0 acts in 0 by the formula (J 0 f)k = ak−1fk−1 + bkfk + akfk+1 (1.1) where k =1, 2, ... and a0 = f0 =0.Theak’s and bk’s are called the weights and diagonal terms, respectively. ∞ In what follows we deal with positive sequences {ak}1 . By Carleman’s 2 2 criterion [1] one can extend J 0 to a self-adjoint operator J in = (N) provided that 1 =+∞. -
Spectral Geometry for Structural Pattern Recognition
Spectral Geometry for Structural Pattern Recognition HEWAYDA EL GHAWALBY Ph.D. Thesis This thesis is submitted in partial fulfilment of the requirements for the degree of Doctor of Philosophy. Department of Computer Science United Kingdom May 2011 Abstract Graphs are used pervasively in computer science as representations of data with a network or relational structure, where the graph structure provides a flexible representation such that there is no fixed dimensionality for objects. However, the analysis of data in this form has proved an elusive problem; for instance, it suffers from the robustness to structural noise. One way to circumvent this problem is to embed the nodes of a graph in a vector space and to study the properties of the point distribution that results from the embedding. This is a problem that arises in a number of areas including manifold learning theory and graph-drawing. In this thesis, our first contribution is to investigate the heat kernel embed- ding as a route to computing geometric characterisations of graphs. The reason for turning to the heat kernel is that it encapsulates information concerning the distribution of path lengths and hence node affinities on the graph. The heat ker- nel of the graph is found by exponentiating the Laplacian eigensystem over time. The matrix of embedding co-ordinates for the nodes of the graph is obtained by performing a Young-Householder decomposition on the heat kernel. Once the embedding of its nodes is to hand we proceed to characterise a graph in a geometric manner. With the embeddings to hand, we establish a graph character- ization based on differential geometry by computing sets of curvatures associated ii Abstract iii with the graph nodes, edges and triangular faces. -
The Essential Spectrum of Schr¨Odinger, Jacobi, And
THE ESSENTIAL SPECTRUM OF SCHRODINGER,¨ JACOBI, AND CMV OPERATORS YORAM LAST1;3 AND BARRY SIMON2;3 Abstract. We provide a very general result that identifies the essential spectrum of broad classes of operators as exactly equal to the closure of the union of the spectra of suitable limits at infinity. Included is a new result on the essential spectra when potentials are asymptotic to isospectral tori. We also recover with a unified framework the HVZ theorem and Krein’s results on orthogonal polynomials with finite essential spectra. 1. Introduction One of the most simple but also most powerful ideas in spectral the- ory is Weyl’s theorem, of which a typical application is (in this intro- duction, in order to avoid technicalities, we take potentials bounded): Theorem 1.1. If V; W are bounded functions on Rº and limjxj!1[V (x) ¡ W (x)] = 0, then σess(¡∆ + V ) = σess(¡∆ + W ) (1.1) Our goal in this paper is to find a generalization of this result that allows “slippage” near infinity. Typical of our results are the following: Theorem 1.2. Let V be a bounded periodic function on (¡1; 1) d2 2 and HV the operator ¡ dx2 + V (x) on L (R). For x > 0, define p d2 2 W (x) = V (x + x) and let HW be ¡ dx2 + W (x) on L (0; 1) with some selfadjoint boundary conditions at zero. Then σess(HW ) = σ(HV ) (1.2) Date: March 7, 2005. 1 Institute of Mathematics, The Hebrew University, 91904 Jerusalem, Israel. E- mail: [email protected]. -
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. -
Spectral Theory of Translation Surfaces : a Short Introduction Volume 28 (2009-2010), P
Institut Fourier — Université de Grenoble I Actes du séminaire de Théorie spectrale et géométrie Luc HILLAIRET Spectral theory of translation surfaces : A short introduction Volume 28 (2009-2010), p. 51-62. <http://tsg.cedram.org/item?id=TSG_2009-2010__28__51_0> © Institut Fourier, 2009-2010, tous droits réservés. L’accès aux articles du Séminaire de théorie spectrale et géométrie (http://tsg.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://tsg.cedram.org/legal/). cedram Article mis en ligne dans le cadre du Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/ Séminaire de théorie spectrale et géométrie Grenoble Volume 28 (2009-2010) 51-62 SPECTRAL THEORY OF TRANSLATION SURFACES : A SHORT INTRODUCTION Luc Hillairet Abstract. — We define translation surfaces and, on these, the Laplace opera- tor that is associated with the Euclidean (singular) metric. This Laplace operator is not essentially self-adjoint and we recall how self-adjoint extensions are chosen. There are essentially two geometrical self-adjoint extensions and we show that they actually share the same spectrum Résumé. — On définit les surfaces de translation et le Laplacien associé à la mé- trique euclidienne (avec singularités). Ce laplacien n’est pas essentiellement auto- adjoint et on rappelle la façon dont les extensions auto-adjointes sont caractérisées. Il y a deux choix naturels dont on montre que les spectres coïncident. 1. Introduction Spectral geometry aims at understanding how the geometry influences the spectrum of geometrically related operators such as the Laplace oper- ator. The more interesting the geometry is, the more interesting we expect the relations with the spectrum to be. -
Discrete Spectral Geometry
Discrete Spectral Geometry Discrete Spectral Geometry Amir Daneshgar Department of Mathematical Sciences Sharif University of Technology Hossein Hajiabolhassan is mathematically dense in this talk!! May 31, 2006 Discrete Spectral Geometry Outline Outline A viewpoint based on mappings A general non-symmetric discrete setup Weighted energy spaces Comparison and variational formulations Summary A couple of comparison theorems Graph homomorphisms A comparison theorem The isoperimetric spectrum ε-Uniformizers Symmetric spaces and representation theory Epilogue Discrete Spectral Geometry A viewpoint based on mappings Basic Objects I H is a geometric objects, we are going to analyze. Discrete Spectral Geometry A viewpoint based on mappings Basic Objects I There are usually some generic (i.e. well-known, typical, close at hand, important, ...) types of these objects. Discrete Spectral Geometry A viewpoint based on mappings Basic Objects (continuous case) I These are models and objects of Euclidean and non-Euclidean geometry. Discrete Spectral Geometry A viewpoint based on mappings Basic Objects (continuous case) I Two important generic objects are the sphere and the upper half plane. Discrete Spectral Geometry A viewpoint based on mappings Basic Objects (discrete case) I Some important generic objects in this case are complete graphs, infinite k-regular tree and fractal-meshes in Rn. Discrete Spectral Geometry A viewpoint based on mappings Basic Objects (discrete case) I These are models and objects in network analysis and design, discrete state-spaces of algorithms and discrete geometry (e.g. in geometric group theory). Discrete Spectral Geometry A viewpoint based on mappings Comparison method I The basic idea here is to try to understand (or classify if we are lucky!) an object by comparing it with the generic ones. -
Ultra-Weak Time Operators of Schrodinger Operators
Title Ultra-Weak Time Operators of Schrodinger Operators Author(s) Arai, Asao; Hiroshima, Fumio Annales Henri Poincaré, 18(9), 2995-3033 Citation https://doi.org/10.1007/s00023-017-0586-x Issue Date 2017-09 Doc URL http://hdl.handle.net/2115/71420 Rights The final publication is available at link.springer.com Type article (author version) File Information arai-hiroshima-rev.pdf Instructions for use Hokkaido University Collection of Scholarly and Academic Papers : HUSCAP Ultra-Weak Time Operators of SchrÄodinger Operators Asao Arai and Fumio Hiroshima Abstract. In an abstract framework, a new concept on time operator, ultra-weak time operator, is introduced, which is a concept weaker than that of weak time operator. Theorems on the existence of an ultra- weak time operator are established. As an application of the theorems, it is shown that SchrÄodingeroperators HV with potentials V obeying suitable conditions, including the Hamiltonian of the hydrogen atom, have ultra-weak time operators. Moreover, a class of Borel measurable functions f : R ! R such that f(HV ) has an ultra-weak time operator is found. Keywords. Time operators, Weyl relations, CCR, SchrÄodingeroperators. 1. Introduction The present paper concerns a time operator in quantum theory which is de- ¯ned, in a ¯rst stage of cognition, as a symmetric operator canonically con- jugate to a Hamiltonian if it exists. The uncertainty relation which is derived from the canonical commutation relation of a time operator and a Hamil- tonian may be interpreted as a mathematically rigorous form of time-energy uncertainty relation. Moreover time operators may play important roles in quantum phenomena [Miy01, Ara05, Ara08b, AM08b , MME08, MME09]. -
Pose Analysis Using Spectral Geometry
Vis Comput DOI 10.1007/s00371-013-0850-0 ORIGINAL ARTICLE Pose analysis using spectral geometry Jiaxi Hu · Jing Hua © Springer-Verlag Berlin Heidelberg 2013 Abstract We propose a novel method to analyze a set 1 Introduction of poses of 3D models that are represented with trian- gle meshes and unregistered. Different shapes of poses are Shape deformation is one of the major research topics in transformed from the 3D spatial domain to a geometry spec- computer graphics. Recently there have been extensive lit- trum domain that is defined by Laplace–Beltrami opera- eratures on this topic. There are two major categories of re- tor. During this space-spectrum transform, all near-isometric searches on this topic. One is surface-based and the other deformations, mesh triangulations and Euclidean transfor- one is skeleton-driven method. Shape interpolation [2, 9, 11] mations are filtered away. The different spatial poses from is a surface-based approach. The basic idea is that given two a 3D model are represented with near-isometric deforma- key frames of a shape, the intermediate deformation can be tions; therefore, they have similar behaviors in the spec- generated with interpolation and further deformations can be tral domain. Semantic parts of that model are then deter- predicted with extrapolation. It can also blend among sev- mined based on the computed geometric properties of all the eral shapes. Shape interpolation is convenient for animation mapped vertices in the geometry spectrum domain. Seman- generation but is not flexible enough for shape editing due tic skeleton can be automatically built with joints detected to the lack of local control. -
Spectral Theory for the Weil-Petersson Laplacian on the Riemann Moduli Space
SPECTRAL THEORY FOR THE WEIL-PETERSSON LAPLACIAN ON THE RIEMANN MODULI SPACE LIZHEN JI, RAFE MAZZEO, WERNER MULLER¨ AND ANDRAS VASY Abstract. We study the spectral geometric properties of the scalar Laplace-Beltrami operator associated to the Weil-Petersson metric gWP on Mγ , the Riemann moduli space of surfaces of genus γ > 1. This space has a singular compactification with respect to gWP, and this metric has crossing cusp-edge singularities along a finite collection of simple normal crossing divisors. We prove first that the scalar Laplacian is essentially self-adjoint, which then implies that its spectrum is discrete. The second theorem is a Weyl asymptotic formula for the counting function for this spectrum. 1. Introduction This paper initiates the analytic study of the natural geometric operators associated to the Weil-Petersson metric gWP on the Riemann moduli space of surfaces of genus γ > 1, denoted below by Mγ. We consider the Deligne- Mumford compactification of this space, Mγ, which is a stratified space with many special features. The topological and geometric properties of this space have been intensively investigated for many years, and Mγ plays a central role in many parts of mathematics. This paper stands as the first step in a development of analytic tech- niques to study the natural elliptic differential operators associated to the Weil-Petersson metric. More generally, our results here apply to the wider class of metrics with crossing cusp-edge singularities on certain stratified Rie- mannian pseudomanifolds. This fits into a much broader study of geometric analysis on stratified spaces using the techniques of geometric microlocal analysis. -
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. -
Spectrum (Functional Analysis) - Wikipedia, the Free Encyclopedia
Spectrum (functional analysis) - Wikipedia, the free encyclopedia http://en.wikipedia.org/wiki/Spectrum_(functional_analysis) Spectrum (functional analysis) From Wikipedia, the free encyclopedia In functional analysis, the concept of the spectrum of a bounded operator is a generalisation of the concept of eigenvalues for matrices. Specifically, a complex number λ is said to be in the spectrum of a bounded linear operator T if λI − T is not invertible, where I is the identity operator. The study of spectra and related properties is known as spectral theory, which has numerous applications, most notably the mathematical formulation of quantum mechanics. The spectrum of an operator on a finite-dimensional vector space is precisely the set of eigenvalues. However an operator on an infinite-dimensional space may have additional elements in its spectrum, and may have no eigenvalues. For example, consider the right shift operator R on the Hilbert space ℓ2, This has no eigenvalues, since if Rx=λx then by expanding this expression we see that x1=0, x2=0, etc. On the other hand 0 is in the spectrum because the operator R − 0 (i.e. R itself) is not invertible: it is not surjective since any vector with non-zero first component is not in its range. In fact every bounded linear operator on a complex Banach space must have a non-empty spectrum. The notion of spectrum extends to densely-defined unbounded operators. In this case a complex number λ is said to be in the spectrum of such an operator T:D→X (where D is dense in X) if there is no bounded inverse (λI − T)−1:X→D.