L-Moments and TL-Moments of Probability Distributions
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Use of Proc Iml to Calculate L-Moments for the Univariate Distributional Shape Parameters Skewness and Kurtosis
Statistics 573 USE OF PROC IML TO CALCULATE L-MOMENTS FOR THE UNIVARIATE DISTRIBUTIONAL SHAPE PARAMETERS SKEWNESS AND KURTOSIS Michael A. Walega Berlex Laboratories, Wayne, New Jersey Introduction Exploratory data analysis statistics, such as those Gaussian. Bickel (1988) and Van Oer Laan and generated by the sp,ge procedure PROC Verdooren (1987) discuss the concept of robustness UNIVARIATE (1990), are useful tools to characterize and how it pertains to the assumption of normality. the underlying distribution of data prior to more rigorous statistical analyses. Assessment of the As discussed by Glass et al. (1972), incorrect distributional shape of data is usually accomplished conclusions may be reached when the normality by careful examination of the values of the third and assumption is not valid, especially when one-tail tests fourth central moments, skewness and kurtosis. are employed or the sample size or significance level However, when the sample size is small or the are very small. Hopkins and Weeks (1990) also underlying distribution is non-normal, the information discuss the effects of highly non-normal data on obtained from the sample skewness and kurtosis can hypothesis testing of variances. Thus, it is apparent be misleading. that examination of the skewness (departure from symmetry) and kurtosis (deviation from a normal One alternative to the central moment shape statistics curve) is an important component of exploratory data is the use of linear combinations of order statistics (L analyses. moments) to examine the distributional shape characteristics of data. L-moments have several Various methods to estimate skewness and kurtosis theoretical advantages over the central moment have been proposed (MacGillivray and Salanela, shape statistics: Characterization of a wider range of 1988). -
Probability and Statistics
APPENDIX A Probability and Statistics The basics of probability and statistics are presented in this appendix, provid- ing the reader with a reference source for the main body of this book without interrupting the flow of argumentation there with unnecessary excursions. Only the basic definitions and results have been included in this appendix. More complicated concepts (such as stochastic processes, Ito Calculus, Girsanov Theorem, etc.) are discussed directly in the main body of the book as the need arises. A.1 PROBABILITY, EXPECTATION, AND VARIANCE A variable whose value is dependent on random events, is referred to as a random variable or a random number. An example of a random variable is the number observed when throwing a dice. The distribution of this ran- dom number is an example of a discrete distribution. A random number is discretely distributed if it can take on only discrete values such as whole numbers, for instance. A random variable has a continuous distribution if it can assume arbitrary values in some interval (which can by all means be the infinite interval from −∞ to ∞). Intuitively, the values which can be assumed by the random variable lie together densely, i.e., arbitrarily close to one another. An example of a discrete distribution on the interval from 0 to ∞ (infinity) might be a random variable which could take on the values 0.00, 0.01, 0.02, 0.03, ..., 99.98, 99.99, 100.00, 100.01, 100.02, ..., etc., like a Bund future with a tick-size of 0.01% corresponding to a value change of 10 euros per tick on a nominal of 100,000 euros. -
18.440: Lecture 9 Expectations of Discrete Random Variables
18.440: Lecture 9 Expectations of discrete random variables Scott Sheffield MIT 18.440 Lecture 9 1 Outline Defining expectation Functions of random variables Motivation 18.440 Lecture 9 2 Outline Defining expectation Functions of random variables Motivation 18.440 Lecture 9 3 Expectation of a discrete random variable I Recall: a random variable X is a function from the state space to the real numbers. I Can interpret X as a quantity whose value depends on the outcome of an experiment. I Say X is a discrete random variable if (with probability one) it takes one of a countable set of values. I For each a in this countable set, write p(a) := PfX = ag. Call p the probability mass function. I The expectation of X , written E [X ], is defined by X E [X ] = xp(x): x:p(x)>0 I Represents weighted average of possible values X can take, each value being weighted by its probability. 18.440 Lecture 9 4 Simple examples I Suppose that a random variable X satisfies PfX = 1g = :5, PfX = 2g = :25 and PfX = 3g = :25. I What is E [X ]? I Answer: :5 × 1 + :25 × 2 + :25 × 3 = 1:75. I Suppose PfX = 1g = p and PfX = 0g = 1 − p. Then what is E [X ]? I Answer: p. I Roll a standard six-sided die. What is the expectation of number that comes up? 1 1 1 1 1 1 21 I Answer: 6 1 + 6 2 + 6 3 + 6 4 + 6 5 + 6 6 = 6 = 3:5. 18.440 Lecture 9 5 Expectation when state space is countable II If the state space S is countable, we can give SUM OVER STATE SPACE definition of expectation: X E [X ] = PfsgX (s): s2S II Compare this to the SUM OVER POSSIBLE X VALUES definition we gave earlier: X E [X ] = xp(x): x:p(x)>0 II Example: toss two coins. -
Randomized Algorithms
Chapter 9 Randomized Algorithms randomized The theme of this chapter is madendrizo algorithms. These are algorithms that make use of randomness in their computation. You might know of quicksort, which is efficient on average when it uses a random pivot, but can be bad for any pivot that is selected without randomness. Analyzing randomized algorithms can be difficult, so you might wonder why randomiza- tion in algorithms is so important and worth the extra effort. Well it turns out that for certain problems randomized algorithms are simpler or faster than algorithms that do not use random- ness. The problem of primality testing (PT), which is to determine if an integer is prime, is a good example. In the late 70s Miller and Rabin developed a famous and simple random- ized algorithm for the problem that only requires polynomial work. For over 20 years it was not known whether the problem could be solved in polynomial work without randomization. Eventually a polynomial time algorithm was developed, but it is much more complicated and computationally more costly than the randomized version. Hence in practice everyone still uses the randomized version. There are many other problems in which a randomized solution is simpler or cheaper than the best non-randomized solution. In this chapter, after covering the prerequisite background, we will consider some such problems. The first we will consider is the following simple prob- lem: Question: How many comparisons do we need to find the top two largest numbers in a sequence of n distinct numbers? Without the help of randomization, there is a trivial algorithm for finding the top two largest numbers in a sequence that requires about 2n − 3 comparisons. -
Probability Cheatsheet V2.0 Thinking Conditionally Law of Total Probability (LOTP)
Probability Cheatsheet v2.0 Thinking Conditionally Law of Total Probability (LOTP) Let B1;B2;B3; :::Bn be a partition of the sample space (i.e., they are Compiled by William Chen (http://wzchen.com) and Joe Blitzstein, Independence disjoint and their union is the entire sample space). with contributions from Sebastian Chiu, Yuan Jiang, Yuqi Hou, and Independent Events A and B are independent if knowing whether P (A) = P (AjB )P (B ) + P (AjB )P (B ) + ··· + P (AjB )P (B ) Jessy Hwang. Material based on Joe Blitzstein's (@stat110) lectures 1 1 2 2 n n A occurred gives no information about whether B occurred. More (http://stat110.net) and Blitzstein/Hwang's Introduction to P (A) = P (A \ B1) + P (A \ B2) + ··· + P (A \ Bn) formally, A and B (which have nonzero probability) are independent if Probability textbook (http://bit.ly/introprobability). Licensed and only if one of the following equivalent statements holds: For LOTP with extra conditioning, just add in another event C! under CC BY-NC-SA 4.0. Please share comments, suggestions, and errors at http://github.com/wzchen/probability_cheatsheet. P (A \ B) = P (A)P (B) P (AjC) = P (AjB1;C)P (B1jC) + ··· + P (AjBn;C)P (BnjC) P (AjB) = P (A) P (AjC) = P (A \ B1jC) + P (A \ B2jC) + ··· + P (A \ BnjC) P (BjA) = P (B) Last Updated September 4, 2015 Special case of LOTP with B and Bc as partition: Conditional Independence A and B are conditionally independent P (A) = P (AjB)P (B) + P (AjBc)P (Bc) given C if P (A \ BjC) = P (AjC)P (BjC). -
Joint Probability Distributions
ST 380 Probability and Statistics for the Physical Sciences Joint Probability Distributions In many experiments, two or more random variables have values that are determined by the outcome of the experiment. For example, the binomial experiment is a sequence of trials, each of which results in success or failure. If ( 1 if the i th trial is a success Xi = 0 otherwise; then X1; X2;:::; Xn are all random variables defined on the whole experiment. 1 / 15 Joint Probability Distributions Introduction ST 380 Probability and Statistics for the Physical Sciences To calculate probabilities involving two random variables X and Y such as P(X > 0 and Y ≤ 0); we need the joint distribution of X and Y . The way we represent the joint distribution depends on whether the random variables are discrete or continuous. 2 / 15 Joint Probability Distributions Introduction ST 380 Probability and Statistics for the Physical Sciences Two Discrete Random Variables If X and Y are discrete, with ranges RX and RY , respectively, the joint probability mass function is p(x; y) = P(X = x and Y = y); x 2 RX ; y 2 RY : Then a probability like P(X > 0 and Y ≤ 0) is just X X p(x; y): x2RX :x>0 y2RY :y≤0 3 / 15 Joint Probability Distributions Two Discrete Random Variables ST 380 Probability and Statistics for the Physical Sciences Marginal Distribution To find the probability of an event defined only by X , we need the marginal pmf of X : X pX (x) = P(X = x) = p(x; y); x 2 RX : y2RY Similarly the marginal pmf of Y is X pY (y) = P(Y = y) = p(x; y); y 2 RY : x2RX 4 / 15 Joint -
Stochastic Time-Series Spectroscopy John Scoville1 San Jose State University, Dept
Stochastic Time-Series Spectroscopy John Scoville1 San Jose State University, Dept. of Physics, San Jose, CA 95192-0106, USA Spectroscopically measuring low levels of non-equilibrium phenomena (e.g. emission in the presence of a large thermal background) can be problematic due to an unfavorable signal-to-noise ratio. An approach is presented to use time-series spectroscopy to separate non-equilibrium quantities from slowly varying equilibria. A stochastic process associated with the non-equilibrium part of the spectrum is characterized in terms of its central moments or cumulants, which may vary over time. This parameterization encodes information about the non-equilibrium behavior of the system. Stochastic time-series spectroscopy (STSS) can be implemented at very little expense in many settings since a series of scans are typically recorded in order to generate a low-noise averaged spectrum. Higher moments or cumulants may be readily calculated from this series, enabling the observation of quantities that would be difficult or impossible to determine from an average spectrum or from prinicipal components analysis (PCA). This method is more scalable than PCA, having linear time complexity, yet it can produce comparable or superior results, as shown in example applications. One example compares an STSS-derived CO2 bending mode to a standard reference spectrum and the result of PCA. A second example shows that STSS can reveal conditions of stress in rocks, a scenario where traditional methods such as PCA are inadequate. This allows spectral lines and non-equilibrium behavior to be precisely resolved. A relationship between 2nd order STSS and a time-varying form of PCA is considered. -
Unbiased Central Moment Estimates
Unbiased Central Moment Estimates Inna Gerlovina1;2, Alan Hubbard1 February 11, 2020 1University of California, Berkeley 2University of California, San Francisco [email protected] Contents 1 Introduction 2 2 Estimators: na¨ıve biased to unbiased 2 3 Estimates obtained from a sample 4 4 Higher order estimates (symbolic expressions for expectations) 5 1 1 Introduction Umoments package calculates unbiased central moment estimates and their two-sample analogs, also known as pooled estimates, up to sixth order (sample variance and pooled variance are commonly used second order examples of corresponding estimators). Orders four and higher include powers and products of moments - for example, fifth moment and a product of second and third moments are both of fifth order; those estimators are also included in the package. The estimates can be obtained directly from samples or from na¨ıve biased moment estimates. If the estimates of orders beyond sixth are needed, they can be generated using the set of functions also provided in the package. Those functions generate symbolic expressions for expectations of moment combinations of an arbitrary order and, in addition to moment estimation, can be used for other derivations that require such expectations (e.g. Edgeworth expansions). 2 Estimators: na¨ıve biased to unbiased For a sample X1;:::;Xn, a na¨ıve biased estimate of a k'th central moment µk is n 1 X m = (X − X¯)k; k = 2; 3;:::: (1) k n i i=1 These biased estimates together with the sample size n can be used to calculate unbiased n estimates of a given order, e.g. -
Functions of Random Variables
Names for Eg(X ) Generating Functions Topic 8 The Expected Value Functions of Random Variables 1 / 19 Names for Eg(X ) Generating Functions Outline Names for Eg(X ) Means Moments Factorial Moments Variance and Standard Deviation Generating Functions 2 / 19 Names for Eg(X ) Generating Functions Means If g(x) = x, then µX = EX is called variously the distributional mean, and the first moment. • Sn, the number of successes in n Bernoulli trials with success parameter p, has mean np. • The mean of a geometric random variable with parameter p is (1 − p)=p . • The mean of an exponential random variable with parameter β is1 /β. • A standard normal random variable has mean0. Exercise. Find the mean of a Pareto random variable. Z 1 Z 1 βαβ Z 1 αββ 1 αβ xf (x) dx = x dx = βαβ x−β dx = x1−β = ; β > 1 x β+1 −∞ α x α 1 − β α β − 1 3 / 19 Names for Eg(X ) Generating Functions Moments In analogy to a similar concept in physics, EX m is called the m-th moment. The second moment in physics is associated to the moment of inertia. • If X is a Bernoulli random variable, then X = X m. Thus, EX m = EX = p. • For a uniform random variable on [0; 1], the m-th moment is R 1 m 0 x dx = 1=(m + 1). • The third moment for Z, a standard normal random, is0. The fourth moment, 1 Z 1 z2 1 z2 1 4 4 3 EZ = p z exp − dz = −p z exp − 2π −∞ 2 2π 2 −∞ 1 Z 1 z2 +p 3z2 exp − dz = 3EZ 2 = 3 2π −∞ 2 3 z2 u(z) = z v(t) = − exp − 2 0 2 0 z2 u (z) = 3z v (t) = z exp − 2 4 / 19 Names for Eg(X ) Generating Functions Factorial Moments If g(x) = (x)k , where( x)k = x(x − 1) ··· (x − k + 1), then E(X )k is called the k-th factorial moment. -
Expected Value and Variance
Expected Value and Variance Have you ever wondered whether it would be \worth it" to buy a lottery ticket every week, or pondered questions such as \If I were offered a choice between a million dollars, or a 1 in 100 chance of a billion dollars, which would I choose?" One method of deciding on the answers to these questions is to calculate the expected earnings of the enterprise, and aim for the option with the higher expected value. This is a useful decision making tool for problems that involve repeating many trials of an experiment | such as investing in stocks, choosing where to locate a business, or where to fish. (For once-off decisions with high stakes, such as the choice between a sure 1 million dollars or a 1 in 100 chance of a billion dollars, it is unclear whether this is a useful tool.) Example John works as a tour guide in Dublin. If he has 200 people or more take his tours on a given week, he earns e1,000. If the number of tourists who take his tours is between 100 and 199, he earns e700. If the number is less than 100, he earns e500. Thus John has a variable weekly income. From experience, John knows that he earns e1,000 fifty percent of the time, e700 thirty percent of the time and e500 twenty percent of the time. John's weekly income is a random variable with a probability distribution Income Probability e1,000 0.5 e700 0.3 e500 0.2 Example What is John's average income, over the course of a 50-week year? Over 50 weeks, we expect that John will earn I e1000 on about 25 of the weeks (50%); I e700 on about 15 weeks (30%); and I e500 on about 10 weeks (20%). -
Random Variables and Applications
Random Variables and Applications OPRE 6301 Random Variables. As noted earlier, variability is omnipresent in the busi- ness world. To model variability probabilistically, we need the concept of a random variable. A random variable is a numerically valued variable which takes on different values with given probabilities. Examples: The return on an investment in a one-year period The price of an equity The number of customers entering a store The sales volume of a store on a particular day The turnover rate at your organization next year 1 Types of Random Variables. Discrete Random Variable: — one that takes on a countable number of possible values, e.g., total of roll of two dice: 2, 3, ..., 12 • number of desktops sold: 0, 1, ... • customer count: 0, 1, ... • Continuous Random Variable: — one that takes on an uncountable number of possible values, e.g., interest rate: 3.25%, 6.125%, ... • task completion time: a nonnegative value • price of a stock: a nonnegative value • Basic Concept: Integer or rational numbers are discrete, while real numbers are continuous. 2 Probability Distributions. “Randomness” of a random variable is described by a probability distribution. Informally, the probability distribution specifies the probability or likelihood for a random variable to assume a particular value. Formally, let X be a random variable and let x be a possible value of X. Then, we have two cases. Discrete: the probability mass function of X specifies P (x) P (X = x) for all possible values of x. ≡ Continuous: the probability density function of X is a function f(x) that is such that f(x) h P (x < · ≈ X x + h) for small positive h. -
Lecture 2: Moments, Cumulants, and Scaling
Lecture 2: Moments, Cumulants, and Scaling Scribe: Ernst A. van Nierop (and Martin Z. Bazant) February 4, 2005 Handouts: • Historical excerpt from Hughes, Chapter 2: Random Walks and Random Flights. • Problem Set #1 1 The Position of a Random Walk 1.1 General Formulation Starting at the originX� 0= 0, if one takesN steps of size�xn, Δ then one ends up at the new position X� N . This new position is simply the sum of independent random�xn), variable steps (Δ N � X� N= Δ�xn. n=1 The set{ X� n} contains all the positions the random walker passes during its walk. If the elements of the{ setΔ�xn} are indeed independent random variables,{ X� n then} is referred to as a “Markov chain”. In a MarkovX� chain,N+1is independentX� ofnforn < N, but does depend on the previous positionX� N . LetPn(R�) denote the probability density function (PDF) for theR� of values the random variable X� n. Note that this PDF can be calculated for both continuous and discrete systems, where the discrete system is treated as a continuous system with Dirac delta functions at the allowed (discrete) values. Letpn(�r|R�) denote the PDF�x forn. Δ Note that in this more general notation we have included the possibility that�r (which is the value�xn) of depends Δ R� on. In Markovchain jargon,pn(�r|R�) is referred to as the “transition probability”X� N fromto state stateX� N+1. Using the PDFs we just defined, let’s return to Bachelier’s equation from the first lecture.