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Random Signals
RANDOM SIGNALS Random Variables A random variable x(ξ) is a mapping that assigns a real number x to every outcome ξ from an abstract probability space. The mapping should satisfy the following two conditions: • the interval {x(ξ) ≤ x} is an event in the abstract probabilty space for every x; • Pr[x(ξ) < ∞] = 1 and Pr[x(ξ) = −∞] = 0. Cumulative distribution function (cdf) of a random variable x(ξ): Fx(x) = Pr{x(ξ) ≤ x}. Probability density function (pdf): dF (x) f (x) = x . x dx Then Z x Fx(x) = fx(x) dx. −∞ EE 524, Fall 2004, # 7 1 Since Fx(∞) = 1, we have normalization condition: Z ∞ fx(x)dx = 1. −∞ Several important properties: 0 ≤ Fx(x) ≤ 1,Fx(−∞) = 0,Fx(∞) = 1, Z ∞ fx(x) ≥ 0, fx(x) dx = 1. −∞ Simple interpretation: Pr{x − ∆/2 ≤ x(ξ) ≤ x + ∆/2} fx(x) = lim . ∆→0 ∆ EE 524, Fall 2004, # 7 2 Expectation of an arbitrary function g(x(ξ)): Z ∞ E {g(x(ξ))} = g(x)fx(x) dx. −∞ Mean: Z ∞ µx = E {x(ξ)} = xfx(x) dx. −∞ Variance of a real random variable x(ξ): 2 2 var{x} = σx = E {(x − E {x}) } = E {x2 − 2xE {x} + E {x}2} = E {x2} − (E {x})2 2 2 = E {x } − µx. Complex random variables: A complex random variable x(ξ) = xR(ξ) + jxI(ξ). Although the definition of the mean remains unchanged, the definition of variance changes for complex x(ξ): 2 2 var{x} = σx = E {|x − E {x}| } = E {|x|2 − xE {x}∗ − x∗E {x} + |E {x}|2} = E {|x|2} − |E {x}|2 2 2 = E {|x| } − |µx| . -
Random Signals
Chapter 8 RANDOM SIGNALS Signals can be divided into two main categories - deterministic and random. The term random signal is used primarily to denote signals, which have a random in its nature source. As an example we can mention the thermal noise, which is created by the random movement of electrons in an electric conductor. Apart from this, the term random signal is used also for signals falling into other categories, such as periodic signals, which have one or several parameters that have appropriate random behavior. An example is a periodic sinusoidal signal with a random phase or amplitude. Signals can be treated either as deterministic or random, depending on the application. Speech, for example, can be considered as a deterministic signal, if one specific speech waveform is considered. It can also be viewed as a random process if one considers the ensemble of all possible speech waveforms in order to design a system that will optimally process speech signals, in general. The behavior of stochastic signals can be described only in the mean. The description of such signals is as a rule based on terms and concepts borrowed from probability theory. Signals are, however, a function of time and such description becomes quickly difficult to manage and impractical. Only a fraction of the signals, known as ergodic, can be handled in a relatively simple way. Among those signals that are excluded are the class of the non-stationary signals, which otherwise play an essential part in practice. Working in frequency domain is a powerful technique in signal processing. While the spectrum is directly related to the deterministic signals, the spectrum of a ran- dom signal is defined through its correlation function. -
Arcsine Laws for Random Walks Generated from Random Permutations with Applications to Genomics
Applied Probability Trust (4 February 2021) ARCSINE LAWS FOR RANDOM WALKS GENERATED FROM RANDOM PERMUTATIONS WITH APPLICATIONS TO GENOMICS XIAO FANG,1 The Chinese University of Hong Kong HAN LIANG GAN,2 Northwestern University SUSAN HOLMES,3 Stanford University HAIYAN HUANG,4 University of California, Berkeley EROL PEKOZ,¨ 5 Boston University ADRIAN ROLLIN,¨ 6 National University of Singapore WENPIN TANG,7 Columbia University 1 Email address: [email protected] 2 Email address: [email protected] 3 Email address: [email protected] 4 Email address: [email protected] 5 Email address: [email protected] 6 Email address: [email protected] 7 Email address: [email protected] 1 Postal address: Department of Statistics, The Chinese University of Hong Kong, Shatin, N.T., Hong Kong 2 Postal address: Department of Mathematics, Northwestern University, 2033 Sheridan Road, Evanston, IL 60208 2 Current address: University of Waikato, Private Bag 3105, Hamilton 3240, New Zealand 1 2 X. Fang et al. Abstract A classical result for the simple symmetric random walk with 2n steps is that the number of steps above the origin, the time of the last visit to the origin, and the time of the maximum height all have exactly the same distribution and converge when scaled to the arcsine law. Motivated by applications in genomics, we study the distributions of these statistics for the non-Markovian random walk generated from the ascents and descents of a uniform random permutation and a Mallows(q) permutation and show that they have the same asymptotic distributions as for the simple random walk. -
Free Infinite Divisibility and Free Multiplicative Mixtures of the Wigner Distribution
FREE INFINITE DIVISIBILITY AND FREE MULTIPLICATIVE MIXTURES OF THE WIGNER DISTRIBUTION Victor Pérez-Abreu and Noriyoshi Sakuma Comunicación del CIMAT No I-09-0715/ -10-2009 ( PE/CIMAT) Free Infinite Divisibility of Free Multiplicative Mixtures of the Wigner Distribution Victor P´erez-Abreu∗ Department of Probability and Statistics, CIMAT Apdo. Postal 402, Guanajuato Gto. 36000, Mexico [email protected] Noriyoshi Sakumay Department of Mathematics, Keio University, 3-14-1, Hiyoshi, Yokohama 223-8522, Japan. [email protected] March 19, 2010 Abstract Let I∗ and I be the classes of all classical infinitely divisible distributions and free infinitely divisible distributions, respectively, and let Λ be the Bercovici-Pata bijection between I∗ and I: The class type W of symmetric distributions in I that can be represented as free multiplicative convolutions of the Wigner distribution is studied. A characterization of this class under the condition that the mixing distribution is 2-divisible with respect to free multiplicative convolution is given. A correspondence between sym- metric distributions in I and the free counterpart under Λ of the positive distributions in I∗ is established. It is shown that the class type W does not include all symmetric distributions in I and that it does not coincide with the image under Λ of the mixtures of the Gaussian distribution in I∗. Similar results for free multiplicative convolutions with the symmetric arcsine measure are obtained. Several well-known and new concrete examples are presented. AMS 2000 Subject Classification: 46L54, 15A52. Keywords: Free convolutions, type G law, free stable law, free compound distribution, Bercovici-Pata bijection. -
Location-Scale Distributions
Location–Scale Distributions Linear Estimation and Probability Plotting Using MATLAB Horst Rinne Copyright: Prof. em. Dr. Horst Rinne Department of Economics and Management Science Justus–Liebig–University, Giessen, Germany Contents Preface VII List of Figures IX List of Tables XII 1 The family of location–scale distributions 1 1.1 Properties of location–scale distributions . 1 1.2 Genuine location–scale distributions — A short listing . 5 1.3 Distributions transformable to location–scale type . 11 2 Order statistics 18 2.1 Distributional concepts . 18 2.2 Moments of order statistics . 21 2.2.1 Definitions and basic formulas . 21 2.2.2 Identities, recurrence relations and approximations . 26 2.3 Functions of order statistics . 32 3 Statistical graphics 36 3.1 Some historical remarks . 36 3.2 The role of graphical methods in statistics . 38 3.2.1 Graphical versus numerical techniques . 38 3.2.2 Manipulation with graphs and graphical perception . 39 3.2.3 Graphical displays in statistics . 41 3.3 Distribution assessment by graphs . 43 3.3.1 PP–plots and QQ–plots . 43 3.3.2 Probability paper and plotting positions . 47 3.3.3 Hazard plot . 54 3.3.4 TTT–plot . 56 4 Linear estimation — Theory and methods 59 4.1 Types of sampling data . 59 IV Contents 4.2 Estimators based on moments of order statistics . 63 4.2.1 GLS estimators . 64 4.2.1.1 GLS for a general location–scale distribution . 65 4.2.1.2 GLS for a symmetric location–scale distribution . 71 4.2.1.3 GLS and censored samples . -
Probability Theory and Stochastic Processes (R18a0403)
PROBABILITY THEORY AND STOCHASTIC PROCESSES (R18A0403) LECTURE NOTES B.TECH (II YEAR – I SEM) (2020-21) Prepared by: Mrs.N.Saritha, Assistant Professor Mr.G.S. Naveen Kumar, Assoc.Professor Department of Electronics and Communication Engineering MALLA REDDY COLLEGE OF ENGINEERING & TECHNOLOGY (Autonomous Institution – UGC, Govt. of India) Recognized under 2(f) and 12 (B) of UGC ACT 1956 (Affiliated to JNTUH, Hyderabad, Approved by AICTE - Accredited by NBA & NAAC – ‘A’ Grade - ISO 9001:2015 Certified) Maisammaguda, Dhulapally (Post Via. Kompally), Secunderabad – 500100, Telangana State, India Sensitivity: Internal & Restricted MALLA REDDY COLLEGE OF ENGINEERING AND TECHNOLOGY (AUTONOMOUS INSTITUTION: UGC, GOVT. OF INDIA) ELECTRONICS AND COMMUNICATION ENGINEERING II ECE I SEM PROBABILITY THEORY AND STOCHASTIC PROCESSES CONTENTS SYLLABUS UNIT-I-PROBABILITY AND RANDOM VARIABLE UNIT-II- DISTRIBUTION AND DENSITY FUNCTIONS AND OPERATIONS ON ONE RANDOM VARIABLE UNIT-III-MULTIPLE RANDOM VARIABLES AND OPERATIONS UNIT-IV-STOCHASTIC PROCESSES-TEMPORAL CHARACTERISTICS UNIT-V- STOCHASTIC PROCESSES-SPECTRAL CHARACTERISTICS UNITWISE IMPORTANT QUESTIONS PROBABILITY THEORY AND STOCHASTIC PROCESS Course Objectives: To provide mathematical background and sufficient experience so that student can read, write and understand sentences in the language of probability theory. To introduce students to the basic methodology of “probabilistic thinking” and apply it to problems. To understand basic concepts of Probability theory and Random Variables, how to deal with multiple Random Variables. To understand the difference between time averages statistical averages. To teach students how to apply sums and integrals to compute probabilities, and expectations. UNIT I: Probability and Random Variable Probability: Set theory, Experiments and Sample Spaces, Discrete and Continuous Sample Spaces, Events, Probability Definitions and Axioms, Joint Probability, Conditional Probability, Total Probability, Bayes’ Theorem, and Independent Events, Bernoulli’s trials. -
High-Dimensional Mahalanobis Distances of Complex Random Vectors
mathematics Article High-Dimensional Mahalanobis Distances of Complex Random Vectors Deliang Dai 1,* and Yuli Liang 2 1 Department of Economics and Statistics, Linnaeus University, 35195 Växjö, Sweden 2 Department of Statistics, Örebro Univeristy, 70281 Örebro, Sweden; [email protected] * Correspondence: [email protected] Abstract: In this paper, we investigate the asymptotic distributions of two types of Mahalanobis dis- tance (MD): leave-one-out MD and classical MD with both Gaussian- and non-Gaussian-distributed complex random vectors, when the sample size n and the dimension of variables p increase under a fixed ratio c = p/n ! ¥. We investigate the distributional properties of complex MD when the random samples are independent, but not necessarily identically distributed. Some results regarding −1 the F-matrix F = S2 S1—the product of a sample covariance matrix S1 (from the independent variable array (be(Zi)1×n) with the inverse of another covariance matrix S2 (from the independent variable array (Zj6=i)p×n)—are used to develop the asymptotic distributions of MDs. We generalize the F-matrix results so that the independence between the two components S1 and S2 of the F-matrix is not required. Keywords: Mahalanobis distance; complex random vector; moments of MDs Citation: Dai, D.; Liang, Y. 1. Introduction High-Dimensional Mahalanobis Mahalanobis distance (MD) is a fundamental statistic in multivariate analysis. It Distances of Complex Random is used to measure the distance between two random vectors or the distance between Vectors. Mathematics 2021, 9, 1877. a random vector and its center of distribution. MD has received wide attention since it https://doi.org/10.3390/ was proposed by Mahalanobis [1] in the 1930’s. -
Handbook on Probability Distributions
R powered R-forge project Handbook on probability distributions R-forge distributions Core Team University Year 2009-2010 LATEXpowered Mac OS' TeXShop edited Contents Introduction 4 I Discrete distributions 6 1 Classic discrete distribution 7 2 Not so-common discrete distribution 27 II Continuous distributions 34 3 Finite support distribution 35 4 The Gaussian family 47 5 Exponential distribution and its extensions 56 6 Chi-squared's ditribution and related extensions 75 7 Student and related distributions 84 8 Pareto family 88 9 Logistic distribution and related extensions 108 10 Extrem Value Theory distributions 111 3 4 CONTENTS III Multivariate and generalized distributions 116 11 Generalization of common distributions 117 12 Multivariate distributions 133 13 Misc 135 Conclusion 137 Bibliography 137 A Mathematical tools 141 Introduction This guide is intended to provide a quite exhaustive (at least as I can) view on probability distri- butions. It is constructed in chapters of distribution family with a section for each distribution. Each section focuses on the tryptic: definition - estimation - application. Ultimate bibles for probability distributions are Wimmer & Altmann (1999) which lists 750 univariate discrete distributions and Johnson et al. (1994) which details continuous distributions. In the appendix, we recall the basics of probability distributions as well as \common" mathe- matical functions, cf. section A.2. And for all distribution, we use the following notations • X a random variable following a given distribution, • x a realization of this random variable, • f the density function (if it exists), • F the (cumulative) distribution function, • P (X = k) the mass probability function in k, • M the moment generating function (if it exists), • G the probability generating function (if it exists), • φ the characteristic function (if it exists), Finally all graphics are done the open source statistical software R and its numerous packages available on the Comprehensive R Archive Network (CRAN∗). -
Field Guide to Continuous Probability Distributions
Field Guide to Continuous Probability Distributions Gavin E. Crooks v 1.0.0 2019 G. E. Crooks – Field Guide to Probability Distributions v 1.0.0 Copyright © 2010-2019 Gavin E. Crooks ISBN: 978-1-7339381-0-5 http://threeplusone.com/fieldguide Berkeley Institute for Theoretical Sciences (BITS) typeset on 2019-04-10 with XeTeX version 0.99999 fonts: Trump Mediaeval (text), Euler (math) 271828182845904 2 G. E. Crooks – Field Guide to Probability Distributions Preface: The search for GUD A common problem is that of describing the probability distribution of a single, continuous variable. A few distributions, such as the normal and exponential, were discovered in the 1800’s or earlier. But about a century ago the great statistician, Karl Pearson, realized that the known probabil- ity distributions were not sufficient to handle all of the phenomena then under investigation, and set out to create new distributions with useful properties. During the 20th century this process continued with abandon and a vast menagerie of distinct mathematical forms were discovered and invented, investigated, analyzed, rediscovered and renamed, all for the purpose of de- scribing the probability of some interesting variable. There are hundreds of named distributions and synonyms in current usage. The apparent diver- sity is unending and disorienting. Fortunately, the situation is less confused than it might at first appear. Most common, continuous, univariate, unimodal distributions can be orga- nized into a small number of distinct families, which are all special cases of a single Grand Unified Distribution. This compendium details these hun- dred or so simple distributions, their properties and their interrelations. -
2.1 Stochastic Processes and Random Fields
2 Random Fields 2.1 Stochastic Processes and Random Fields As you read in the Preface, for us a random field is simply a stochastic pro- cess, taking values in a Euclidean space, and defined over a parameter space of dimensionality at least one. Actually, we shall be rather loose about exchang- ing the terms `random field’ and `stochastic process'. In general, we shall use ‘field’ when the geometric structure of the parameter space is important to us, and shall use `process' otherwise. We shall usually denote parameter spaces by either T or M, generally using T when the parameter space is simple Euclidean domain, such as a cube, and M when refering to manifolds, or surfaces. Elements of both T and M will be denoted by t, in a notation harking back to the early days of stochastic processes when the parameter was always one-dimensional `time'. Of course, we have yet to define what a stochastic process is. To do this properly, we should really talk about notions such as probability spaces, mea- surability, separability, and so forth, as we did in RFG. However, we shall send the purist to RFG to read about such things, and here take a simpler route. Definition 2.1.1. Given a parameter space T , a stochastic process f over T is a collection of random variables ff(t): t 2 T g : If T is a set of dimension N, and the random variables f(t) are all vector valued of dimension d, then we call the vector valued random field f a (N; d) random field. -
Arcsine Laws for Random Walks Generated from Random
ARCSINE LAWS FOR RANDOM WALKS GENERATED FROM RANDOM PERMUTATIONS WITH APPLICATIONS TO GENOMICS XIAO FANG, HAN LIANG GAN, SUSAN HOLMES, HAIYAN HUANG, EROL PEKOZ,¨ ADRIAN ROLLIN,¨ AND WENPIN TANG Abstract. A classical result for the simple symmetric random walk with 2n steps is that the number of steps above the origin, the time of the last visit to the origin, and the time of the maximum height all have exactly the same distribution and converge when scaled to the arcsine law. Motivated by applications in genomics, we study the distributions of these statistics for the non-Markovian random walk generated from the ascents and descents of a uniform random permutation and a Mallows(q) permutation and show that they have the same asymptotic distributions as for the simple random walk. We also give an unexpected conjecture, along with numerical evidence and a partial proof in special cases, for the result that the number of steps above the origin by step 2n for the uniform permutation generated walk has exactly the same discrete arcsine distribution as for the simple random walk, even though the other statistics for these walks have very different laws. We also give explicit error bounds to the limit theorems using Stein’s method for the arcsine distribution, as well as functional central limit theorems and a strong embedding of the Mallows(q) permutation which is of independent interest. Key words : Arcsine distribution, Brownian motion, L´evy statistics, limiting distribu- tion, Mallows permutation, random walks, Stein’s method, strong embedding, uniform permutation. AMS 2010 Mathematics Subject Classification: 60C05, 60J65, 05A05. -
Probabilistic Arithmetic
Probabilistic Arithmetic by Rob ert Charles Williamson BE QIT MEngSc Qld A thesis submitted for the degree of Do ctor of Philosophy Department of Electrical Engineering University of Queensland August Statement of Originality To the b est of the candidates knowledge and b elief the material presented in this thesis is original except as acknowledged in the text and the material has not b een submitted either in whole or in part for a degree at this or any other university Rob ert Williamson ii Abstract This thesis develops the idea of probabilistic arithmetic The aim is to replace arithmetic op erations on numb ers with arithmetic op erations on random variables Sp ecicallyweareinterested in numerical metho ds of calculating convolutions of probability distributions The longterm goal is to b e able to handle random prob lems such as the determination of the distribution of the ro ots of random algebraic equations using algorithms whichhavebeendevelop ed for the deterministic case To this end in this thesis we survey a numb er of previously prop osed metho ds for calculating convolutions and representing probability distributions and examine their defects We develop some new results for some of these metho ds the Laguerre transform and the histogram metho d but ultimately nd them unsuitable We nd that the details on how the ordinary convolution equations are calculated are secondary to the diculties arising due to dep endencies When random variables app ear rep eatedly in an expression it is not p ossible to determine the distribution