Proved That Every Real Separable Banach Space Contains a Separable Hilbert Space As a Dense Embedding, and This Space Is the Support of a Gaussian Measure
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The Hilbert Transform
(February 14, 2017) The Hilbert transform Paul Garrett [email protected] http:=/www.math.umn.edu/egarrett/ [This document is http:=/www.math.umn.edu/egarrett/m/fun/notes 2016-17/hilbert transform.pdf] 1. The principal-value functional 2. Other descriptions of the principal-value functional 3. Uniqueness of odd/even homogeneous distributions 4. Hilbert transforms 5. Examples 6. ... 7. Appendix: uniqueness of equivariant functionals 8. Appendix: distributions supported at f0g 9. Appendix: the snake lemma Formulaically, the Cauchy principal-value functional η is Z 1 f(x) Z f(x) ηf = principal-value functional of f = P:V: dx = lim dx −∞ x "!0+ jxj>" x This is a somewhat fragile presentation. In particular, the apparent integral is not a literal integral! The uniqueness proven below helps prove plausible properties like the Sokhotski-Plemelj theorem from [Sokhotski 1871], [Plemelji 1908], with a possibly unexpected leading term: Z 1 f(x) Z 1 f(x) lim dx = −iπ f(0) + P:V: dx "!0+ −∞ x + i" −∞ x See also [Gelfand-Silov 1964]. Other plausible identities are best certified using uniqueness, such as Z f(x) − f(−x) ηf = 1 dx (for f 2 C1( ) \ L1( )) 2 x R R R f(x)−f(−x) using the canonical continuous extension of x at 0. Also, 2 Z f(x) − f(0) · e−x ηf = dx (for f 2 Co( ) \ L1( )) x R R R The Hilbert transform of a function f on R is awkwardly described as a principal-value integral 1 Z 1 f(t) 1 Z f(t) (Hf)(x) = P:V: dt = lim dt π −∞ x − t π "!0+ jt−xj>" x − t with the leading constant 1/π understandable with sufficient hindsight: we will see that this adjustment makes H extend to a unitary operator on L2(R). -
L2-Theory of Semiclassical Psdos: Hilbert-Schmidt And
2 LECTURE 13: L -THEORY OF SEMICLASSICAL PSDOS: HILBERT-SCHMIDT AND TRACE CLASS OPERATORS In today's lecture we start with some abstract properties of Hilbert-Schmidt operators and trace class operators. Then we will investigate the following natural t questions: for which class of symbols, the quantized operator Op~(a) is a Hilbert- Schmidt or trace class operator? How to compute its trace? 1. Hilbert-Schmidt and Trace class operators: Abstract theory { Definitions via singular values. As we have mentioned last time, we are aiming at developing the spectral theory for semiclassical pseudodifferential operators. For a 2 S(m), where m is a decaying t 2 n symbol, we showed that Op~(a) is a compact operator acting on L (R ). As a t consequence, either Op~(a) has only finitely many nonzero eigenvalues, or it has infinitely nonzero eigenvalues which can be arranged to a sequence whose norms converges to 0. However, in general the eigenvalues of a compact operator A are non-real. A very simple way to get real eigenvalues is to consider the operator A∗A, which is 1 a compact self-adjoint linear operator acting on L2(Rn). Thus the eigenvalues of A∗A can be list2 in decreasing order as 2 2 2 s1 ≥ s2 ≥ s3 ≥ · · · : The numbers sj (which will always be taken to be the positive one) are called the singular values of A. Definition 1.1. We say a compact operator3 A is a Hilbert-Schmidt operator if !1=2 X 2 (1) kAkHS := sj < +1: j The number kAkHS is called the Hilbert-Schmidt norm (or Schatten 2-norm) of A. -
Design and Application of a Hilbert Transformer in a Digital Receiver
Proceedings of the SDR 11 Technical Conference and Product Exposition, Copyright © 2011 Wireless Innovation Forum All Rights Reserved DESIGN AND APPLICATION OF A HILBERT TRANSFORMER IN A DIGITAL RECEIVER Matt Carrick (Northrop Grumman, Chantilly, VA, USA; [email protected]); Doug Jaeger (Northrop Grumman, Chantilly, VA, USA; [email protected]); fred harris (San Diego State University, San Diego, CA, USA; [email protected]) ABSTRACT A common method of down converting a signal from an intermediate frequency (IF) to baseband is using a quadrature down-converter. One problem with the quadrature down-converter is it requires two low pass filters; one for the real branch and one for the imaginary branch. A more efficient way is to transform the real signal to a complex signal and then complex heterodyne the resultant signal to baseband. The transformation of a real signal to a complex signal can be done using a Hilbert transform. Building a Hilbert transform directly from its sampled data sequence produces suboptimal results due to time series truncation; another method is building a Hilbert transformer by synthesizing the filter coefficients from half Figure 1: A quadrature down-converter band filter coefficients. Designing the Hilbert transform filter using a half band filter allows for a much more Another way of viewing the problem is that the structured design process as well as greatly improved quadrature down-converter not only extracts the desired results. segment of the spectrum it rejects the undesired spectral image, the spectral replica present in the Hermetian 1. INTRODUCTION symmetric spectra of a real signal. Removing this image would result in a single sided spectrum which being non- The digital portion of a receiver is typically designed to Hermetian symmetric is the transform of a complex signal. -
Communication Theory II Slides 04
Communication Theory II Lecture 4: Review on Fourier analysis and probabilty theory Ahmed Elnakib, PhD Assistant Professor, Mansoura University, Egypt Febraury 19th, 2015 1 Course Website o http://lms.mans.edu.eg/eng/ o The site contains the lectures, quizzes, homework, and open forums for feedback and questions o Log in using your name and password o Password for quizzes: third o One page quiz: for less download time 2 Lecture Outlines o Review on Fourier analysis of signals and systems . The Dirac delta function . Fourier transform of periodic signals . Transmission of signals through LTI systems . Hilbert transform o Review on probability theory . Deterministic vs. probabilistic mathematical models . Probability theory, random variables, and the distribution functions . The concept of expectation and second order statistics . Characteristic function, the center limit theory and the Bayesian interface 3 The Dirac Delta Function (Unit Impulse) δ(t) t 0 o An even function of time t, centered at the origin t = 0 o Sifting property: sifts out the value g(t0) of the function g(t) at time t = t0, where o Replication property: convolution of any function with the delta function leaves that function unchanged 4 The Dirac Delta Function (cont’d) W=1 Amplitude W=2 Amplitude W=5 f(t)=δ(t) F(f)=1 1 t Amplitude 0 0 f5 The Dirac Delta Function (cont’d) T→0 The delta function may be viewed Rectangular impulse as the limiting form of a pulse of unit area (symmetric with respect to the origin) as the duration of the pulse approaches zero Sinc impulse T=1/2W 6 Existence of Fourier Transform o Physical realizability is a sufficient condition for the existence of a Fourier transform (e.g., all energy signals are Fourier transformable ). -
On Some Integral Operators Appearing in Scattering Theory, And
On some integral operators appearing in scattering theory, and their resolutions S. Richard,∗ T. Umeda† Graduate school of mathematics, Nagoya University, Chikusa-ku, Nagoya 464-8602, Japan Department of Mathematical Sciences, University of Hyogo, Shosha, Himeji 671-2201, Japan E-mail: [email protected], [email protected] Abstract We discuss a few integral operators and provide expressions for them in terms of smooth functions of some natural self-adjoint operators. These operators appear in the context of scattering theory, but are independent of any perturbation theory. The Hilbert transform, the Hankel transform, and the finite interval Hilbert transform are among the operators considered. 2010 Mathematics Subject Classification: 47G10 Keywords: integral operators, Hilbert transform, Hankel transform, dilation operator, scattering theory 1 Introduction Investigations on the wave operators in the context of scattering theory have a long history, and several powerful technics have been developed for the proof of their existence and of their completeness. More recently, properties of these operators in various spaces have been studied, and the importance of these operators for non-linear problems has also been acknowledged. A quick search on MathSciNet shows that the terms wave operator(s) appear in the title of numerous papers, confirming their importance in various fields of mathematics. For the last decade, the wave operators have also played a key role for the arXiv:1909.01712v1 [math-ph] 4 Sep 2019 search of index theorems in scattering theory, as a tool linking the scattering part of a physical system to its bound states. For such investigations, a very detailed ∗Supported by the grantTopological invariants through scattering theory and noncommuta- tive geometry from Nagoya University, and by JSPS Grant-in-Aid for scientific research (C) no 18K03328, and on leave of absence from Univ. -
Arxiv:1611.05269V3 [Cs.IT] 29 Jan 2018 Graph Analytic Signal, and Associated Amplitude and Frequency Modulations Reveal Com
On Hilbert Transform, Analytic Signal, and Modulation Analysis for Signals over Graphs Arun Venkitaraman, Saikat Chatterjee, Peter Handel¨ Department of Information Science and Engineering, School of Electrical Engineering and ACCESS Linnaeus Center KTH Royal Institute of Technology, SE-100 44 Stockholm, Sweden . Abstract We propose Hilbert transform and analytic signal construction for signals over graphs. This is motivated by the popularity of Hilbert transform, analytic signal, and mod- ulation analysis in conventional signal processing, and the observation that comple- mentary insight is often obtained by viewing conventional signals in the graph setting. Our definitions of Hilbert transform and analytic signal use a conjugate-symmetry-like property exhibited by the graph Fourier transform (GFT), resulting in a ’one-sided’ spectrum for the graph analytic signal. The resulting graph Hilbert transform is shown to possess many interesting mathematical properties and also exhibit the ability to high- light anomalies/discontinuities in the graph signal and the nodes across which signal discontinuities occur. Using the graph analytic signal, we further define amplitude, phase, and frequency modulations for a graph signal. We illustrate the proposed con- cepts by showing applications to synthesized and real-world signals. For example, we show that the graph Hilbert transform can indicate presence of anomalies and that arXiv:1611.05269v3 [cs.IT] 29 Jan 2018 graph analytic signal, and associated amplitude and frequency modulations reveal com- plementary information in speech signals. Keywords: Graph signal, analytic signal, Hilbert transform, demodulation, anomaly detection. Email addresses: [email protected] (Arun Venkitaraman), [email protected] (Saikat Chatterjee), [email protected] (Peter Handel)¨ Preprint submitted to Signal Processing 1 1 0.8 0.8 0.6 0.6 0.4 0.4 0.2 0.2 0 0 (a) (b) Figure 1: Anomaly highlighting behavior of the graph Hilbert transform for 2D image signal graph. -
Hilbert Transform and Singular Integrals on the Spaces of Tempered Ultradistributions
ALGEBRAIC ANALYSIS AND RELATED TOPICS BANACH CENTER PUBLICATIONS, VOLUME 53 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 2000 HILBERT TRANSFORM AND SINGULAR INTEGRALS ON THE SPACES OF TEMPERED ULTRADISTRIBUTIONS ANDRZEJKAMINSKI´ Institute of Mathematics, University of Rzesz´ow Rejtana 16 C, 35-310 Rzesz´ow,Poland E-mail: [email protected] DUSANKAPERIˇ SIˇ C´ Institute of Mathematics, University of Novi Sad Trg Dositeja Obradovi´ca4, 21000 Novi Sad, Yugoslavia E-mail: [email protected] STEVANPILIPOVIC´ Institute of Mathematics, University of Novi Sad Trg Dositeja Obradovi´ca4, 21000 Novi Sad, Yugoslavia E-mail: [email protected] Abstract. The Hilbert transform on the spaces S0∗(Rd) of tempered ultradistributions is defined, uniquely in the sense of hyperfunctions, as the composition of the classical Hilbert transform with the operators of multiplying and dividing a function by a certain elliptic ultra- polynomial. We show that the Hilbert transform of tempered ultradistributions defined in this way preserves important properties of the classical Hilbert transform. We also give definitions and prove properties of singular integral operators with odd and even kernels on the spaces S0∗(Rd), whose special cases are the Hilbert transform and Riesz operators. 1. Introduction. The Hilbert transform on distribution and ultradistribution spaces has been studied by many mathematicians, see e.g. Tillmann [17], Beltrami and Wohlers [1], Vladimirov [18], Singh and Pandey [15], Ishikawa [2], Ziemian [20] and Pilipovi´c[11]. In all these papers the Hilbert transform is defined by one of the two methods: by the method of adjoints or by considering a generalized function on the kernel which belongs to the corresponding test function space. -
The Hilbert Transform
The Hilbert transform 1 Definition and properties 1 Recall the distribution pv( x ), defined by Z '(x) pv(1=x)(') := lim dx: !0 jx|≥ x The Hilbert transform is defined via the convolution with pv(1=x), namely 1 Z f(x − t) (Hf)(x) := lim dt: π !0 jt|≥ t The main theorem we are going to prove in this note is the following. Theorem 1.1. For any p 2 (1; +1), there exists a constant Cp such that kHfkp < Cpkfkp (1.1) for all f 2 S(R). Thus, H extends to a bounded linear operator on all of Lp(R). The first remark we make is that the above theorem is false when p = 1. To see this, note that for smooth f with compact support, when x is very large, the main contribution to the integral Z f(x − t) dt t comes from the values t which are not far away from x. This in general gives the decay 1 rate of order jxj , unless there is a magical cancellation due to the sign changes of f, in which case one can hope for a faster decay. Indeed, it is not hard to show that if f is continuous and has compact support with R f(t)dt = a, then a (Hf)(x) = + O(1=x2) πx 1 R for all large x. As a consequence, Hf 2 L (R) if and only if f = 0. The statement of 1 the above theorem is also not true for p = +1. The reason is that x is not integrable at infinity, so one can not bound on kHfk1 merely by using the maximum of f without any other information (e.g., the size of the support). -
Preduals for Spaces of Operators Involving Hilbert Spaces and Trace
PREDUALS FOR SPACES OF OPERATORS INVOLVING HILBERT SPACES AND TRACE-CLASS OPERATORS HANNES THIEL Abstract. Continuing the study of preduals of spaces L(H,Y ) of bounded, linear maps, we consider the situation that H is a Hilbert space. We establish a natural correspondence between isometric preduals of L(H,Y ) and isometric preduals of Y . The main ingredient is a Tomiyama-type result which shows that every contractive projection that complements L(H,Y ) in its bidual is automatically a right L(H)-module map. As an application, we show that isometric preduals of L(S1), the algebra of operators on the space of trace-class operators, correspond to isometric preduals of S1 itself (and there is an abundance of them). On the other hand, the compact operators are the unique predual of S1 making its multiplication separately weak∗ continuous. 1. Introduction An isometric predual of a Banach space X is a Banach space F together with an isometric isomorphism X =∼ F ∗. Every predual induces a weak∗ topology. Due to the importance of weak∗ topologies, it is interesting to study the existence and uniqueness of preduals; see the survey [God89] and the references therein. Given Banach spaces X and Y , let L(X, Y ) denote the space of operators from X to Y . Every isometric predual of Y induces an isometric predual of L(X, Y ): If Y =∼ F ∗, then L(X, Y ) =∼ (X⊗ˆ F )∗. Problem 1.1. Find conditions on X and Y guaranteeing that every isometric predual of L(X, Y ) is induced from an isometric predual of Y . -
Discrete Hilbert Transform. Numeric Algorithms
Volume 49, Number 4, 2008 485 Discrete Hilbert Transform. Numeric Algorithms Gheorghe TODORAN, Rodica HOLONEC and Ciprian IAKAB Abstract - The Hilbert and Fourier transforms are tools used for signal analysis in the time/frequency domains. The Hilbert transform is applied to casual continuous signals. The majority of the practical signals are discrete signals and they are limited in time. It appeared therefore the need to create numeric algorithms for the Hilbert transform. Such an algorithm is a numeric operator, named the Discrete Hilbert Transform. This paper makes a brief presentation of known algorithms and proposes an algorithm derived from the properties of the analytic complex signal. The methods for time and frequency calculus are also presented. 1. INTRODUCTION spectrum in order to avoid the aliasing process – the Nyquist condition. Signals can be classified into two classes: The discrete signal will be analyzed on a analytic signals (for instance = sin)( ωtAtx ), computer system, which implies its and experimental signals (measured signals). digitization (the digital signal is the discrete The last category represents real signals and is signal converted in binary format, accordingly of great importance in applications. to the adopted analog/numeric conversion; in An experimental signal represents a signal most of the cases, the signal acquisition observed during a limited interval of time. It is hardware also does the digitization of the a sample of the original signal, which signal samples). The resulted digital signal has characterizes a physical process of interest. the greatest importance in numeric analysis The experimental signal can be a operations. continuous time signal (analogical), or a Some other remarks need to be made. -
Spectral Decompositions in Banach Spaces and the Hilbert Transform
LINEAR OPERATORS BANACH CENTER PUBLICATIONS, VOLUME 38 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 1997 SPECTRAL DECOMPOSITIONS IN BANACH SPACES AND THE HILBERT TRANSFORM T. A. GILLESPIE Department of Mathematics and Statistics University of Edinburgh, James Clerk Maxwell Building Edinburgh EH9 3JZ, Scotland E-mail: [email protected] Abstract. This paper gives a survey of some recent developments in the spectral theory of linear operators on Banach spaces in which the Hilbert transform and its abstract analogues play a fundamental role. 1. Introduction. Various notions of self-adjointness have been developed for oper- ators acting on Banach spaces, each reflecting some aspect of the Hilbert space theory. One such notion is that of well-boundedness, a concept introduced by Smart [23] and first studied by Smart and Ringrose [21–23]. An operator is (by definition) well-bounded if it has a functional calculus based on the Banach algebra of absolutely continuous func- tions on a compact real interval. This functional calculus gives rise to a form of spectral diagonalization, as will be described in more detail below. Initially, there were relatively few examples of well-bounded operators, other than rather obvious ones, until Dowson and Spain [17] gave an interesting example of a well- bounded operator A acting on Lp(Z) for p in the range 1 <p< ∞. It can be shown that the operator they considered has the property that eiA is the bilateral shift on Lp(Z) (see [18, p. 1044]) and this observation illustrates the more general fact [19] that every translation operator on Lp(G), where G is a locally compact abelian group and 1 <p< ∞, is of the form eiA for some well-bounded operator A. -
S0002-9947-1980-0570783-0.Pdf
transactions of the american mathematical society Volume 260, Number 1, July 1980 NONSTANDARD EXTENSIONS OF TRANSFORMATIONS BETWEEN BANACH SPACES BY D. G. TACON Abstract. Let X and Y be (infinite-dimensional) Banach spaces and denote their nonstandard hulls with respect to an Nj -saturated enlargement by X and Y respectively. If 9> (X, Y) denotes the space of bounded linear transformations then a subset S of elements of ® (X, Y) extends naturally to a subset S of *$>(X, Y). This paper studies the behaviour of various kinds of transformations under this extension and introduces, in this context, the concepts of super weakly compact, super strictly singular and socially compact operators. It shows that (® (X, Y))~ c 'S (X, Y) provided X and Y are infinite dimensional and contrasts this with the inclusion %(H) c (%(H))~ where %(H) denotes the space of compact operators on a Hubert space. The nonstandard hull of a uniform space was introduced by Luxemburg [14] and the construction, in the case of normed spaces, has since been investigated in a number of papers (see, for example [4], [6], [7], [8], [9], [10], [15]). Our intention here is to examine the behaviour of single bounded linear transformations and classes of bounded linear transformations under the nonstandard hull extension. We recount the principal ideas. Consider a normed space (X, || • ||) embedded in a set theoretical structure 911 and consider an N, -sa tura ted enlargement *91t of 9H. An element p G *X is said to be finite if *||p|| is a finite element of *R, the set of such elements being denoted by fin(*Ar).