Stochastic Models Laws of Large Numbers and Functional Central
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Poisson Processes Stochastic Processes
Poisson Processes Stochastic Processes UC3M Feb. 2012 Exponential random variables A random variable T has exponential distribution with rate λ > 0 if its probability density function can been written as −λt f (t) = λe 1(0;+1)(t) We summarize the above by T ∼ exp(λ): The cumulative distribution function of a exponential random variable is −λt F (t) = P(T ≤ t) = 1 − e 1(0;+1)(t) And the tail, expectation and variance are P(T > t) = e−λt ; E[T ] = λ−1; and Var(T ) = E[T ] = λ−2 The exponential random variable has the lack of memory property P(T > t + sjT > t) = P(T > s) Exponencial races In what follows, T1;:::; Tn are independent r.v., with Ti ∼ exp(λi ). P1: min(T1;:::; Tn) ∼ exp(λ1 + ··· + λn) . P2 λ1 P(T1 < T2) = λ1 + λ2 P3: λi P(Ti = min(T1;:::; Tn)) = λ1 + ··· + λn P4: If λi = λ and Sn = T1 + ··· + Tn ∼ Γ(n; λ). That is, Sn has probability density function (λs)n−1 f (s) = λe−λs 1 (s) Sn (n − 1)! (0;+1) The Poisson Process as a renewal process Let T1; T2;::: be a sequence of i.i.d. nonnegative r.v. (interarrival times). Define the arrival times Sn = T1 + ··· + Tn if n ≥ 1 and S0 = 0: The process N(t) = maxfn : Sn ≤ tg; is called Renewal Process. If the common distribution of the times is the exponential distribution with rate λ then process is called Poisson Process of with rate λ. Lemma. N(t) ∼ Poisson(λt) and N(t + s) − N(s); t ≥ 0; is a Poisson process independent of N(s); t ≥ 0 The Poisson Process as a L´evy Process A stochastic process fX (t); t ≥ 0g is a L´evyProcess if it verifies the following properties: 1. -
Stochastic Processes and Applications Mongolia 2015
NATIONAL UNIVERSITY OF MONGOLIA Stochastic Processes and Applications Mongolia 2015 27th July - 7th August 2015 National University of Mongolia Ulan Bator Mongolia National University of Mongolia 1 1 Basic information Venue: The meeting will take place at the National University of Mongolia. The map below shows the campus of the University which is located in the North-Eastern block relative to the Government Palace and Chinggis Khaan Square (see the red circle with arrow indicating main entrance in map below) in the very heart of down-town Ulan Bator. • All lectures, contributed talks and tutorials will be held in the Room 320 at 3rd floor, Main building, NUM. • Registration and Opening Ceremony will be held in the Academic Hall (Round Hall) at 2nd floor of the Main building. • The welcome reception will be held at the 2nd floor of the Broadway restaurant pub which is just on the West side of Chinggis Khaan Square (see the blue circle in map below). NATIONAL UNIVERSITY OF MONGOLIA 2 National University of Mongolia 1 Facilities: The main venue is equipped with an electronic beamer, a blackboard and some movable white- boards. There will also be magic whiteboards which can be used on any vertical surface. White-board pens and chalk will be provided. Breaks: Refreshments will be served between talks (see timetable below) at the conference venue. Lunches: Arrangements for lunches will be announced at the start of the meeting. Accommodation: Various places are being used for accommodation. The main accommodation are indi- cated on the map below relative to the National University (red circle): The Puma Imperial Hotel (purple circle), H9 Hotel (black circle), Ulanbaatar Hotel (blue circle), Student Dormitories (green circle) Mentoring: A mentoring scheme will be running which sees more experienced academics linked with small groups of junior researchers. -
Extinction, Survival and Duality to P-Jump Processes
Markov branching processes with disasters: extinction, survival and duality to p-jump processes by Felix Hermann and Peter Pfaffelhuber Albert-Ludwigs University Freiburg Abstract A p-jump process is a piecewise deterministic Markov process with jumps by a factor of p. We prove a limit theorem for such processes on the unit interval. Via duality with re- spect to probability generating functions, we deduce limiting results for the survival proba- bilities of time-homogeneous branching processes with arbitrary offspring distributions, un- derlying binomial disasters. Extending this method, we obtain corresponding results for time-inhomogeneous birth-death processes underlying time-dependent binomial disasters and continuous state branching processes with p-jumps. 1 Introduction Consider a population evolving according to a branching process ′. In addition to reproduction events, global events called disasters occur at some random times Z(independent of ′) that kill off every individual alive with probability 1 p (0, 1), independently of each other.Z The resulting process of population sizes will be called− a branching∈ process subject to binomial disasters with survival probability p. ProvidedZ no information regarding fitness of the individuals in terms of resistance against disasters, this binomial approach appears intuitive, since the survival events of single individuals are iid. Applications span from natural disasters as floods and droughts to effects of radiation treatment or chemotherapy on cancer cells as well as antibiotics on popula- tions of bacteria. Also, Bernoulli sampling comes into mind as in the Lenski Experiment (cf. arXiv:1808.00073v2 [math.PR] 7 Jan 2019 Casanova et al., 2016). In the general setting of Bellman-Harris processes with non-lattice lifetime-distribution subject to binomial disasters, Kaplan et al. -
Joint Pricing and Inventory Control for a Stochastic Inventory System With
Joint pricing and inventory control for a stochastic inventory system with Brownian motion demand Dacheng Yao Academy of Mathematics and Systems Science, Chinese Academy of Sciences, Beijing, 100190, China; [email protected] Abstract In this paper, we consider an infinite horizon, continuous-review, stochastic inventory system in which cumulative customers' demand is price-dependent and is modeled as a Brownian motion. Excess demand is backlogged. The revenue is earned by selling products and the costs are incurred by holding/shortage and ordering, the latter consists of a fixed cost and a proportional cost. Our objective is to simultaneously determine a pricing strategy and an inventory control strategy to maximize the expected long-run average profit. Specifically, the pricing strategy provides the price pt for any time t ≥ 0 and the inventory control strategy characterizes when and how much we need to order. We show that an (s∗;S∗; p∗) policy is ∗ ∗ optimal and obtain the equations of optimal policy parameters, where p = fpt : t ≥ 0g. ∗ Furthermore, we find that at each time t, the optimal price pt depends on the current inventory level z, and it is increasing in [s∗; z∗] and is decreasing in [z∗; 1), where z∗ is a negative level. Keywords: Stochastic inventory model, pricing, Brownian motion demand, (s; S; p) policy, impulse control, drift rate control. arXiv:1608.03033v2 [math.OC] 11 Jul 2017 1 Introduction Exogenous selling price is always assumed in the classic production/inventory models; see e.g., Scarf(1960) and the research thereafter. In practice, however, dynamic pricing is one important tool for revenue management by balancing customers' demand and inventory level. -
Renewal and Regenerative Processes
Chapter 2 Renewal and Regenerative Processes Renewal and regenerative processes are models of stochastic phenomena in which an event (or combination of events) occurs repeatedly over time, and the times between occurrences are i.i.d. Models of such phenomena typically focus on determining limiting averages for costs or other system parameters, or establishing whether certain probabilities or expected values for a system converge over time, and evaluating their limits. The chapter begins with elementary properties of renewal processes, in- cluding several strong laws of large numbers for renewal and related stochastic processes. The next part of the chapter covers Blackwell’s renewal theorem, and an equivalent key renewal theorem. These results are important tools for characterizing the limiting behavior of probabilities and expectations of stochastic processes. We present strong laws of large numbers and central limit theorems for Markov chains and regenerative processes in terms of a process with regenerative increments (which is essentially a random walk with auxiliary paths). The rest of the chapter is devoted to studying regenera- tive processes (including ergodic Markov chains), processes with regenerative increments, terminating renewal processes, and stationary renewal processes. 2.1 Renewal Processes This section introduces renewal processes and presents several examples. The discussion covers Poisson processes and renewal processes that are “embed- ded” in stochastic processes. We begin with notation and terminology for point processes that we use in later chapters as well. Suppose 0 ≤ T1 ≤ T2 ≤ ... are finite random times at which a certain event occurs. The number of the times Tn in the interval (0,t]is ∞ N(t)= 1(Tn ≤ t),t≥ 0. -
Reliable Reasoning”
Abstracta SPECIAL ISSUE III, pp. 10 – 17, 2009 COMMENTS ON HARMAN AND KULKARNI’S “RELIABLE REASONING” Glenn Shafer Gil Harman and Sanjeev Kulkarni have written an enjoyable and informative book that makes Vladimir Vapnik’s ideas accessible to a wide audience and explores their relevance to the philosophy of induction and reliable reasoning. The undertaking is important, and the execution is laudable. Vapnik’s work with Alexey Chervonenkis on statistical classification, carried out in the Soviet Union in the 1960s and 1970s, became popular in computer science in the 1990s, partly as the result of Vapnik’s books in English. Vapnik’s statistical learning theory and the statistical methods he calls support vector machines now dominate machine learning, the branch of computer science concerned with statistical prediction, and recently (largely after Harman and Kulkarni completed their book) these ideas have also become well known among mathematical statisticians. A century ago, when the academic world was smaller and less specialized, philosophers, mathematicians, and scientists interested in probability, induction, and scientific methodology talked with each other more than they do now. Keynes studied Bortkiewicz, Kolmogorov studied von Mises, Le Dantec debated Borel, and Fisher debated Jeffreys. Today, debate about probability and induction is mostly conducted within more homogeneous circles, intellectual communities that sometimes cross the boundaries of academic disciplines but overlap less in their discourse than in their membership. Philosophy of science, cognitive science, and machine learning are three of these communities. The greatest virtue of this book is that it makes ideas from these three communities confront each other. In particular, it looks at how Vapnik’s ideas in machine learning can answer or dissolve questions and puzzles that have been posed by philosophers. -
18.600: Lecture 31 .1In Strong Law of Large Numbers and Jensen's
18.600: Lecture 31 Strong law of large numbers and Jensen's inequality Scott Sheffield MIT Outline A story about Pedro Strong law of large numbers Jensen's inequality Outline A story about Pedro Strong law of large numbers Jensen's inequality I One possibility: put the entire sum in government insured interest-bearing savings account. He considers this completely risk free. The (post-tax) interest rate equals the inflation rate, so the real value of his savings is guaranteed not to change. I Riskier possibility: put sum in investment where every month real value goes up 15 percent with probability :53 and down 15 percent with probability :47 (independently of everything else). I How much does Pedro make in expectation over 10 years with risky approach? 100 years? Pedro's hopes and dreams I Pedro is considering two ways to invest his life savings. I Riskier possibility: put sum in investment where every month real value goes up 15 percent with probability :53 and down 15 percent with probability :47 (independently of everything else). I How much does Pedro make in expectation over 10 years with risky approach? 100 years? Pedro's hopes and dreams I Pedro is considering two ways to invest his life savings. I One possibility: put the entire sum in government insured interest-bearing savings account. He considers this completely risk free. The (post-tax) interest rate equals the inflation rate, so the real value of his savings is guaranteed not to change. I How much does Pedro make in expectation over 10 years with risky approach? 100 years? Pedro's hopes and dreams I Pedro is considering two ways to invest his life savings. -
Exploiting Regenerative Structure to Estimate Finite Time Averages Via Simulation
EXPLOITING REGENERATIVE STRUCTURE TO ESTIMATE FINITE TIME AVERAGES VIA SIMULATION Wanmo Kang, Perwez Shahabuddin* and Ward Whitt Columbia University We propose nonstandard simulation estimators of expected time averages over ¯nite intervals [0; t], seeking to enhance estimation e±ciency. We make three key assumptions: (i) the underlying stochastic process has regenerative structure, (ii) the time average approaches a known limit as time t increases and (iii) time 0 is a regeneration time. To exploit those properties, we propose a residual-cycle estimator, based on data from the regenerative cycle in progress at time t, using only the data after time t. We prove that the residual-cycle estimator is unbiased and more e±cient than the standard estimator for all su±ciently large t. Since the relative e±ciency increases in t, the method is ideally suited to use when applying simulation to study the rate of convergence to the known limit. We also consider two other simulation techniques to be used with the residual-cycle estimator. The ¯rst involves overlapping cycles, paralleling the technique of overlapping batch means in steady-state estimation; multiple observations are taken from each replication, starting a new observation each time the initial regenerative state is revisited. The other technique is splitting, which involves independent replications of the terminal period after time t, for each simulation up to time t. We demonstrate that these alternative estimators provide e±ciency improvement by conducting simulations of queueing models. Categories and Subject Descriptors: G.3 [Mathematics of Computing]: Probability and Statis- tics|renewal theory; I.6.6 [Computing Methodologies]: Simulation and Modelling|simula- tion output analysis General Terms: Algorithms, Experimentation, Performance, Theory Additional Key Words and Phrases: e±ciency improvement, variance reduction, regenerative processes, time averages 1. -
On the Law of the Iterated Logarithm for L-Statistics Without Variance
Bulletin of the Institute of Mathematics Academia Sinica (New Series) Vol. 3 (2008), No. 3, pp. 417-432 ON THE LAW OF THE ITERATED LOGARITHM FOR L-STATISTICS WITHOUT VARIANCE BY DELI LI, DONG LIU AND ANDREW ROSALSKY Abstract Let {X, Xn; n ≥ 1} be a sequence of i.i.d. random vari- ables with distribution function F (x). For each positive inte- ger n, let X1:n ≤ X2:n ≤ ··· ≤ Xn:n be the order statistics of X1, X2, · · · , Xn. Let H(·) be a real Borel-measurable function de- fined on R such that E|H(X)| < ∞ and let J(·) be a Lipschitz function of order one defined on [0, 1]. Write µ = µ(F,J,H) = ← 1 n i E L : (J(U)H(F (U))) and n(F,J,H) = n Pi=1 J n H(Xi n), n ≥ 1, where U is a random variable with the uniform (0, 1) dis- ← tribution and F (t) = inf{x; F (x) ≥ t}, 0 <t< 1. In this note, the Chung-Smirnov LIL for empirical processes and the Einmahl- Li LIL for partial sums of i.i.d. random variables without variance are used to establish necessary and sufficient conditions for having L with probability 1: 0 < lim supn→∞ pn/ϕ(n) | n(F,J,H) − µ| < ∞, where ϕ(·) is from a suitable subclass of the positive, non- decreasing, and slowly varying functions defined on [0, ∞). The almost sure value of the limsup is identified under suitable con- ditions. Specializing our result to ϕ(x) = 2(log log x)p,p > 1 and to ϕ(x) = 2(log x)r,r > 0, we obtain an analog of the Hartman- Wintner-Strassen LIL for L-statistics in the infinite variance case. -
The Law of Large Numbers and the Monte-Carlo Method
Lecture 17: The Law of Large Numbers and the Monte-Carlo method The Law of Large numbers Suppose we perform an experiment and a measurement encoded in the random variable X and that we repeat this experiment n times each time in the same conditions and each time independently of each other. We thus obtain n independent copies of the random variable X which we denote X1;X2; ··· ;Xn Such a collection of random variable is called a IID sequence of random variables where IID stands for independent and identically distributed. This means that the random variables Xi have the same probability distribution. In particular they have all the same means and variance 2 E[Xi] = µ ; var(Xi) = σ ; i = 1; 2; ··· ; n Each time we perform the experiment n tiimes, the Xi provides a (random) measurement and if the average value X1 + ··· + Xn n is called the empirical average. The Law of Large Numbers states for large n the empirical average is very close to the expected value µ with very high probability Theorem 1. Let X1; ··· ;Xn IID random variables with E[Xi] = µ and var(Xi) for all i. Then we have 2 X1 + ··· Xn σ P − µ ≥ ≤ n n2 In particular the right hand side goes to 0 has n ! 1. Proof. The proof of the law of large numbers is a simple application from Chebyshev X1+···Xn inequality to the random variable n . Indeed by the properties of expectations we have X + ··· X 1 1 1 E 1 n = E [X + ··· X ] = (E [X ] + ··· E [X ]) = nµ = µ n n 1 n n 1 n n For the variance we use that the Xi are independent and so we have X + ··· X 1 1 σ2 var 1 n = var (X + ··· X ]) = (var(X ) + ··· + var(X )) = n n2 1 n n2 1 n n 1 By Chebyshev inequality we obtain then 2 X1 + ··· Xn σ P − µ ≥ ≤ n n2 Coin flip I: Suppose we flip a fair coin 100 times. -
Stochastic Processes and Applications Mongolia 2015
NATIONAL UNIVERSITY OF MONGOLIA Stochastic Processes and Applications Mongolia 2015 27th July - 7th August 2015 National University of Mongolia Ulaanbaatar Mongolia National University of Mongolia 1 1 Final Report Executive summary • The research school was attended by 120 individuals, the majority of which were students, 54 of which were Mongolians. There was representation from academic institutions in 20 different countries. The lecture room remained full on every one of the 10 working days without numbers waning. • The whole event was generously sponsored by: Centre International de Math´ematiquesPures et Ap- pliqu´ees(CIMPA), Deutscher Akademischer Austauschdienst (DAAD), National University of Mongo- lia (NUM), Mongolian University of Science and Technology (MUST), the State Bank (SB), Mongolian Agricultural Commodities Exchange (MACE), Index Based Livestock Insurance Project (IBLIP) and Tenger Insurance, Mongolia (TIM). There was also a kind cash contribution from Prof. Ga¨etanBorot. The total expenditure of the school came to around 56K EURO. • Feedback indicates the event was an overwhelming scientific success and the school is likely to remain as a landmark event in the history of the Department of Mathematics at the National University of Mongolia. • There was outstanding cultural exchange, with strong social mixing and interaction taking place fol- lowing traditional norms of Mongolian hospitality. Participants experienced cultural activities on two Wednesday afternoons as well as a weekend excursion into Terelj National Park. These include throat singing, ger building, hiking, visiting a Buddhist Temple, museum exhibitions, learning about Mongo- lia's Soviet past, socialising at lunches and dinners with the help of an engineered `buddy system'. • There was significant exchange between senior Mongolian and foreign academics at the meeting re- garding the current and future plight of Mongolian mathematics. -
Laws of Large Numbers in Stochastic Geometry with Statistical Applications
Bernoulli 13(4), 2007, 1124–1150 DOI: 10.3150/07-BEJ5167 Laws of large numbers in stochastic geometry with statistical applications MATHEW D. PENROSE Department of Mathematical Sciences, University of Bath, Bath BA2 7AY, United Kingdom. E-mail: [email protected] Given n independent random marked d-vectors (points) Xi distributed with a common density, define the measure νn = i ξi, where ξi is a measure (not necessarily a point measure) which stabilizes; this means that ξi is determined by the (suitably rescaled) set of points near Xi. For d bounded test functions fPon R , we give weak and strong laws of large numbers for νn(f). The general results are applied to demonstrate that an unknown set A in d-space can be consistently estimated, given data on which of the points Xi lie in A, by the corresponding union of Voronoi cells, answering a question raised by Khmaladze and Toronjadze. Further applications are given concerning the Gamma statistic for estimating the variance in nonparametric regression. Keywords: law of large numbers; nearest neighbours; nonparametric regression; point process; random measure; stabilization; Voronoi coverage 1. Introduction Many interesting random variables in stochastic geometry arise as sums of contributions from each point of a point process Xn comprising n independent random d-vectors Xi, 1 ≤ i ≤ n, distributed with common density function. General limit theorems, including laws of large numbers (LLNs), central limit theorems and large deviation principles, have been obtained for such variables, based on a notion of stabilization (local dependence) of the contributions; see [16, 17, 18, 20].