Birth and Poisson Processes

Total Page:16

File Type:pdf, Size:1020Kb

Birth and Poisson Processes Poisson, birth and death Waiting queues Risk process Cat Bonds Birth and Poisson processes Olivier Scaillet University of Geneva and Swiss Finance Institute 1/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Outline 1 Poisson, birth and death 2 Waiting queues 3 Risk process 4 Cat Bonds 2/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Introduction Many natural phenomenons exhibit changes of value at random times rather than fixed times. We model this behavior with continuous-time models, that is, processes of the form fXt : t ≥ 0g, where t is continuous. The sample paths of the processes we consider here have integer values. 3/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Poisson process The Poisson process is ideal to model the occurrence of successive events. Every event is such that, in a time interval (t; t + ∆t) with ∆t small, its probability of occurrence is proportional to ∆t, and that the probability of occurrence of two events in the same small interval is negligible. 4/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Poisson process (cont’d) A Poisson process with intensity λ is a process N = fNt : t ≥ 0g, whose values belong to 0; 1; 2; 3; ::: and such that: 1 N0 = 0 and Ns ≤ Nt , if s < t, 2 if s < t , the number Nt − Ns of events in the time interval (s; t] is independent of the arrival times and the arrivals in the interval [0; s] (process with independent increments) 8 λ∆t + o(∆t) if i = 1 <> 3 P[Nt+∆t = n + ijNt = n] = o(∆t) if i > 1 :>1 − λ∆t + o(∆t) if i = 0 f (∆t) Notation: f (∆t) = o(∆t) is equivalent to lim∆t!0 ∆t = 0. 5/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Poisson process (cont’d) The function f has a smaller asymptotic order than ∆t, and is negligible in comparison to ∆t. We say that Nt stands for the number of arrivals, occurrences, or events of the process until time t. The process fNt g is a counting process and is a simple example of continuous-time Markov chains. The intensity λ (or birth rate) corresponds to the probability of occurrence of one event per unit of time. The Poisson process Nt follows a Poisson distribution with (λt)i −λt parameter λt, P[Nt = i] = i! e , i = 0; 1; 2;::: . In particular, we have E[Nt ] = λt. 6/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Poisson process (cont’d) We can also characterize the Poisson process using the duration between successive events. Let T0; T1;::: be given by T0 = 0, Tn = infft : Nt = ng. Tn is the date of the nth arrival. The durations (or intervals) are random variables dn = Tn − Tn−1. These variables d1; d2;::: are independent and follow an exponential distribution with parameter λ, whose density function is given by f (d) = λe−λd . The distribution function is given by F (d) = 1 − e−λd , and the 1 expectation of the durations is E[dt ] = λ . 7/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Poisson process (cont’d) Remarks: one can rebuild the process N with durations d, using Pn Tn = i=1 di , Nt = maxfn : Tn ≤ tg. the estimation of the lambda parameter is trivial as the maximum likelihood estimator for an exponential law is the inverse of the empirical mean:λ^ = 1 , where d¯ is the empirical d¯ mean of the observed durations. 8/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Birth process The Poisson process has a constant intensity (or birth rate). We may introduce a dependence between the number of previous events and the birth rate. A birth process with intensities λ0; λ1; λ2;::: is a process N = fNt : t ≥ 0g, whose values lie in f0; 1; 2; 3;:::g and such that: 1 N0 = 0 and Ns ≤ Nt , if s < t 2 if s < t , conditionally on the value of Ns , the number of events Nt − Ns in the time interval (s; t] is independent of all previous arrivals in the interval[0; s] 8 λ ∆t + o(∆t) if i = 1 <> n 3 P[Nt+∆t = n + ijNt = n] = o(∆t) if i > 1 > :1 − λn∆t + o(∆t) if i = 0 9/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Birth process (cont’d) Particular cases: Poisson process: λn = λ, 8n Simple birth: λn = nλ. Population growth where each individual gives birth independently of the others, with probability λ∆t + o(∆t) during the time interval (t; t + ∆t), and where there is no death. Birth with immigration: λn = nλ + v. Birth process where the birth rate depends on an external immigration rate. 10/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Birth and death process A more realistic model in the context of a population growth also allows for deaths. Let Nt be the number of alive individuals at time t in a particular population. This number follows a birth and death process if: 1 Nt is a Markov chain with values f0; 1; 2;:::g 2 P[Nt+∆t = n + ijNt = n] = 8 λ ∆t + o(∆t) if i = 1 > n > <µn∆t + o(∆t) if i = −1 o(∆t) if jij > 1 > > :1 − λn∆t − µn∆t + o(∆t) if i = 0 3 The birth rates λ0; λ1; λ2;::: and death rates µ0; µ1; µ2;::: are such that λi ≥ 0, µi ≥ 0, and µ0 = 0. 11/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Birth and death process (cont’d) Particular cases: Birth process: µn = 0, 8n. Simple death with immigration: λn = λ, µn = nµ, 8n. Population that does not give birth but with some immigration corresponding to a Poisson process, and for which each individual has a probability µ∆t + o(∆t) to die in the time interval (t; t + ∆t). Simple birth and death: λn = nλ, µn = nµ, 8n. Each invidividual that is alive may either die during the time interval (t; t + ∆t) with a probability µ∆t + o(∆t), or split with a probability λ∆t + o(∆t). 12/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Waiting queues Waiting queues theory is an important application of the stochastic process theory. Practical examples: Connections to a server. Call center capacity. Number of counters in a bank. 13/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Inflows A waiting queue has an input stream that stands for the client arrivals (“client” has a broad meaning, e.g., cars, memory calls of a computer, phone call in a call center). As a first approximation, we assume that the durations between arrivals are i.i.d. random variables. The input stream is then a so-called stationary renewal process. We get the simplest case by using a duration following the exponential law: the input flow follows a Poisson process. 14/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Service A waiting queue generally has a service provider that is specified by The duration of the service, whose distribution is assumed to be known. The number of ticket offices (or counters). 15/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Service (cont’d) A waiting queue is also characterized by a rule of service that defines the service behavior: System with or without waiting queue (i.e., in a system without queue, clients are lost if they are not served immediately); system with a limited capacity (i.e., clients are lost when the queue is too long). The order in which clients are served: first in first out (FIFO), last in first out (LIFO). Multiple client priority classes. Contingent probability of client loss: the client may be lost with a probability depending on the length of the queue. 16/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Kendall notation For a mathematical study, we classify the waiting queues following the standardized Kendall notation A/B/C/D. The letters have the following meaning: A: input stream B: duration of service C: number of ticket offices D: additional information, as follows. The letter M (for Markov) for input streams stands for a Poisson stream; for the duration of service, it stands for an exponential duration. The letter D (for Determinist) for input streams stands for regular interval durations; for the duration of service, it stands for a fixed time for any client. The letter G stands for the general case. 17/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Example: M/M/1 queue It is the simplest example of a waiting queue: The input stream follows a Poisson process with intensity λ, or, equivalently, the durations between the arrivals follow an i.i.d. exponential distribution with parameter λ. The service durations are i.i.d. and follow an exponential law with parameter µ. There is only one ticket office and client are served according to a first in first out rule; the capacity of the queue is infinite. Remark: the M/M/1 queue is equivalent to a birth and death process whose birth and death rates are given by λn = λ, 8n and µ0 = 0, µn = µ, 8n > 0, respectively. 18/31 Poisson, birth and death Waiting queues Risk process Cat Bonds Example: M/M/1 queue (cont’d) If the ticket office is open without interruption, the average service rate is equal to µ.
Recommended publications
  • Ewens' Sampling Formula
    Ewens’ sampling formula; a combinatorial derivation Bob Griffiths, University of Oxford Sabin Lessard, Universit´edeMontr´eal Infinitely-many-alleles-model: unique mutations ......................................................................................................... •. •. •. ............................................................................................................ •. •. .................................................................................................... •. •. •. ............................................................. ......................................... .............................................. •. ............................... ..................... ..................... ......................................... ......................................... ..................... • ••• • • • ••• • • • • • Sample configuration of alleles 4 A1,1A2,4A3,3A4,3A5. Ewens’ sampling formula (1972) n sampled genes k b Probability of a sample having types with j types represented j times, jbj = n,and bj = k,is n! 1 θk · · b b 1 1 ···n n b1! ···bn! θ(θ +1)···(θ + n − 1) Example: Sample 4 A1,1A2,4A3,3A4,3A5. b1 =1, b2 =0, b3 =2, b4 =2. Old and New lineages . •. ............................... ......................................... •. .............................................. ............................... ............................... ..................... ..................... ......................................... ..................... ..................... ◦ ◦◦◦◦◦ n1 n2 nm nm+1
    [Show full text]
  • Copyrighted Material
    Index alternating renewal process, 353, 354 reflection principle, 474 scaling invariance, 471 Bayes rule, 23, 28 simulation, 480 Bernoulli process, 228, 293, 301–305, 309, 316 time invariance, 472 beta function, 60, 170, 265 Buffon’s needle problem, 83, 94 birth and catastrophe chain, 377 birth and death chain, 375, 392 Cauchy–Bunyakovsky–Schwarz inequality, 135, birthday problem, 30–31 137, 143, 149 Black–Karasinski model, 509 Central Limit Theorem, 2, 87, 92, 241, Blackwell renewal theorem, 346, 348 244, 245, 273, 282, 302, 342, 343, block replacement policy, 344 482, 523 Borel–Cantelli lemmas, 34–142, 224, 304 DeMoivre-Laplace version, 151 bounded convergence theorem, 131, 251, 422, changing the order of derivation and integra- 448, 455 tion, 243 branching process, 363, 366, 368, 441, 461 Chapman-Kolmogorov equation, 378, 379, 381, Brownian bridge, 483 389, 420 Brownian motion conditional distribution, 468 characteristic function, 192–194 covariance structure,COPYRIGHTED 471 MATERIALcontinuity theorem, 203 definition, 467 examples, 194–199 drift, 471 multivariate random vector, 194 examples, 468, 471 properties, 193 generation, 176 uniqueness, 200 hitting time, 475, 476 characterization theorem for convergence in dis- multidimensional, 473 tribution, 218 quadratic variation, 478 Cholesky decomposition, 174–176, 514 547 Probability and Stochastic Processes, First Edition. Ionut¸Florescu C 2015 John Wiley & Sons, Inc. Published 2015 by John Wiley & Sons, Inc. 548 INDEX CIR model, 507 Darboux sums, 349 moments, 510, 511 De Morgan laws,
    [Show full text]
  • On a Fractional Alternating Poisson Process
    AIMS Mathematics, 1(3): 212-224 DOI:10.3934/Math.2016.3.212 Received: 5 September 2016 Accepted: 12 September 2016 http://www.aimspress.com/journal/Math Published: 20 September 2016 Research article On a fractional alternating Poisson process Antonio Di Crescenzo∗and Alessandra Meoli Department of Mathematics, University of Salerno, Via Giovanni Paolo II, 132, 84084 Fisciano (SA), Italy ∗ Correspondence: Email: [email protected]; Tel: +39 089 96 3349; Fax: +39 089 96 3303. Abstract: We propose a generalization of the alternating Poisson process from the point of view of fractional calculus. We consider the system of differential equations governing the state probabilities of the alternating Poisson process and replace the ordinary derivative with the fractional derivative (in the Caputo sense). This produces a fractional 2-state point process. We obtain the probability mass function of this process in terms of the (two-parameter) Mittag-Leffler function. Then we show that it can be recovered also by means of renewal theory. We study the limit state probability, and certain proportions involving the fractional moments of the sub-renewal periods of the process. In conclusion, in order to derive new Mittag-Leffler-like distributions related to the considered process, we exploit a transformation acting on pairs of stochastically ordered random variables, which is an extension of the equilibrium operator and deserves interest in the analysis of alternating stochastic processes. Keywords: Caputo derivative; Mittag-Leffler function; fractional process; alternating process; renewal process; renewal function 1. Introduction Extension of continuous-time point processes to the fractional case has been a major topic in liter- ature for several years.
    [Show full text]
  • EE414 - Birth-Death Processes 1/17 Birth-Death Processes
    Birth-Death Processes Birth-Death Processes: Transient Solution Poisson Process: State Distribution Poisson Process: Inter-arrival Times Dr Conor McArdle EE414 - Birth-Death Processes 1/17 Birth-Death Processes Birth-Death Processes are Markov chains where transitions are allowed only between neighbouring states of the process. They may be discrete- or continuous-time. Our primary interest is in the continuous-time case. Birth-Death processes are used to simplify the analysis of systems that see random arrivals and departures of customers (packets, requests, or calls etc.) over time. We will develop results that are useful for performance evaluation of servers (or transmission lines) with associated input queues. The results also apply to circuit switches with limited numbers of outgoing channels. We start in this section by seeking the transient solution to the Birth-Death system. Recall that the general transient solution π(t) of a continuous-time Markov chain is given implicitly by π_ (t) = π(t)Q where Q is the matrix of state transition-rates between each pair of states in the process. The Birth-Death assumption imposes a certain structure on Q which gives the solution π(t) a simplified form. Dr Conor McArdle EE414 - Birth-Death Processes 2/17 Birth-Death Processes: Transition-rates Consider the state transition-rate diagram of the general Birth-Death process below. ë0 ë1 ëk-1 ëk 0 1 2 k-1 k k+1 ì1 ì2 ìk ìk+1 The states of the process are represented by numbered circles, the number indicating the state. For a birth-death process this number represents the number of individuals in the population, which for our purposes we interpret as the number of packets (or requests or calls) in the system.
    [Show full text]
  • Notes on the Poisson Point Process
    Notes on the Poisson point process Paul Keeler January 5, 2016 This work is licensed under a “CC BY-SA 3.0” license. Abstract The Poisson point process is a type of random object known as a point pro- cess that has been the focus of much study and application. This survey aims to give an accessible but detailed account of the Poisson point process by covering its history, mathematical definitions in a number of settings, and key properties as well detailing various terminology and applications of the process, with rec- ommendations for further reading. 1 Introduction In probability, statistics and related fields, a Poisson point process or a Poisson process or a Poisson point field is a type of random object known as a point pro- cess or point field that consists of randomly positioned points located on some underlying mathematical space [68]. The process has convenient mathematical properties [39], which has led to it being frequently defined in Euclidean space and used as a mathematical model for seemingly random processes in numer- ous disciplines such as astronomy [5], biology [53], ecology [70], geology [16], physics [61], image processing [12], and telecommunications [7][28]. The Poisson point process is often defined on the real line playing an impor- tant role in the field of queueing theory [40] where it is used to model certain random events happening in time such as the arrival of customers at a store or phone calls at an exchange. In the plane, the point process, also known as a spa- tial Poisson process [9], may represent scattered objects such as users in a wireless network [2, 6, 7, 27], particles colliding into a detector, or trees in a forest [68].
    [Show full text]
  • General Birth-Death Processes: Probabilities, Inference, and Applications
    Electronic Thesis and Dissertations UCLA Peer Reviewed Title: General birth-death processes: probabilities, inference, and applications Author: Crawford, Forrest Wrenn Acceptance Date: 2012 Series: UCLA Electronic Theses and Dissertations Degree: Ph.D., Biomathematics 0121UCLA Advisor(s): Suchard, Marc A Committee: Lange, Kenneth, Sinsheimer, Janet, Novembre, John Permalink: http://escholarship.org/uc/item/4gc165m0 Abstract: Copyright Information: All rights reserved unless otherwise indicated. Contact the author or original publisher for any necessary permissions. eScholarship is not the copyright owner for deposited works. Learn more at http://www.escholarship.org/help_copyright.html#reuse eScholarship provides open access, scholarly publishing services to the University of California and delivers a dynamic research platform to scholars worldwide. University of California Los Angeles General birth-death processes: probabilities, inference, and applications A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Biomathematics by Forrest Wrenn Crawford 2012 Abstract of the Dissertation General birth-death processes: probabilities, inference, and applications by Forrest Wrenn Crawford Doctor of Philosophy in Biomathematics University of California, Los Angeles, 2012 Professor Marc A. Suchard, Chair A birth-death process is a continuous-time Markov chain that counts the number of particles in a system over time. Each particle can give birth to another particle or die, and the rate of births and deaths at any given time depends on how many extant particles there are. Birth-death processes are popular modeling tools in evolution, population biology, genetics, epidemiology, and ecology. Despite the widespread interest in birth-death models, no efficient method exists to evaluate the finite-time transition probabilities in a process with arbitrary birth and death rates.
    [Show full text]
  • Genealogical Constructions of Population Models March 2, 2018
    Genealogical constructions of population models Alison M. Etheridge ∗ Thomas G. Kurtz y Department of Statistics Departments of Mathematics and Statistics Oxford University University of Wisconsin - Madison 24-29 St Giles 480 Lincoln Drive Oxford OX1 3LB Madison, WI 53706-1388 UK USA [email protected] [email protected] http://www.stats.ox.ac.uk/~etheridg/ http://www.math.wisc.edu/~kurtz/ March 2, 2018 Abstract Representations of population models in terms of countable systems of particles are constructed, in which each particle has a `type', typically recording both spatial position and genetic type, and a level. For finite intensity models, the levels are distributed on [0; λ], whereas in the infinite intensity limit λ ! 1, at each time t, the joint distribution of types and levels is conditionally Poisson, with mean measure Ξ(t)×` where ` denotes Lebesgue measure and Ξ(t) is a measure-valued population process. The time-evolution of the levels captures the genealogies of the particles in the population. Key forces of ecology and genetics can be captured within this common framework. Models covered incorporate both individual and event based births and deaths, one-for- one replacement, immigration, independent `thinning' and independent or exchange- able spatial motion and mutation of individuals. Since birth and death probabilities can depend on type, they also include natural selection. The primary goal of the paper is to present particle-with-level or lookdown constructions for each of these elements of a population model. Then the elements can be combined to specify the desired model. In particular, a non-trivial extension of the spatial Λ-Fleming-Viot process is constructed.
    [Show full text]
  • ROBUSTNESS of SCALE-FREE SPATIAL NETWORKS Emmanuel Jacob, Morters Peter
    ROBUSTNESS OF SCALE-FREE SPATIAL NETWORKS Emmanuel Jacob, Morters Peter To cite this version: Emmanuel Jacob, Morters Peter. ROBUSTNESS OF SCALE-FREE SPATIAL NETWORKS. 2015. hal-01139102 HAL Id: hal-01139102 https://hal.archives-ouvertes.fr/hal-01139102 Preprint submitted on 3 Apr 2015 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. ROBUSTNESS OF SCALE-FREE SPATIAL NETWORKS EMMANUEL JACOB AND PETER MORTERS¨ Abstract: A growing family of random graphs is called robust if it retains a giant component after percolation with arbitrary positive retention probabil- ity. We study robustness for graphs, in which new vertices are given a spatial position on the d-dimensional torus and are connected to existing vertices with a probability favouring short spatial distances and high degrees. In this model of a scale-free network with clustering we can independently tune the power law exponent τ of the degree distribution and the rate δd at which the connection probability decreases with the distance of two− vertices. We 1 show that the network is robust if τ < 2 + δ , but fails to be robust if τ > 3. In the case of one-dimensional space we also show that the network is not 1 robust if τ > 2 + δ−1 .
    [Show full text]
  • Evolutionary Dynamics of Speciation and Extinction
    Scholars' Mine Doctoral Dissertations Student Theses and Dissertations Fall 2015 Evolutionary dynamics of speciation and extinction Dawn Michelle King Follow this and additional works at: https://scholarsmine.mst.edu/doctoral_dissertations Part of the Biophysics Commons Department: Physics Recommended Citation King, Dawn Michelle, "Evolutionary dynamics of speciation and extinction" (2015). Doctoral Dissertations. 2464. https://scholarsmine.mst.edu/doctoral_dissertations/2464 This thesis is brought to you by Scholars' Mine, a service of the Missouri S&T Library and Learning Resources. This work is protected by U. S. Copyright Law. Unauthorized use including reproduction for redistribution requires the permission of the copyright holder. For more information, please contact [email protected]. 1 EVOLUTIONARY DYNAMICS OF SPECIATION AND EXTINCTION by DAWN MICHELLE KING A DISSERTATION Presented to the Faculty of the Graduate Faculty of the MISSOURI UNIVERSITY OF SCIENCE AND TECHNOLOGY and UNIVERSITY OF MISSOURI AT SAINT LOUIS In Partial Fulfillment of the Requirements for the Degree DOCTOR OF PHILOSOPHY in PHYSICS 2015 Approved by: Sonya Bahar, Advisor Ricardo Flores Nevena Marić Paul Parris Thomas Vojta 1 iii ABSTRACT Presented here is an interdisciplinary study that draws connections between the fields of physics, mathematics, and evolutionary biology. Importantly, as we move through the Anthropocene Epoch, where human-driven climate change threatens biodiversity, understanding how an evolving population responds to extinction stress could be key to saving endangered ecosystems. With a neutral, agent-based model that incorporates the main principles of Darwinian evolution, such as heritability, variability, and competition, the dynamics of speciation and extinction is investigated. The simulated organisms evolve according to the reaction-diffusion rules of the 2D directed percolation universality class.
    [Show full text]
  • Stochastic Processes II/ Wahrscheinlichkeitstheorie III Lecture Notes
    BMS Basic Course Stochastic Processes II/ Wahrscheinlichkeitstheorie III Michael Scheutzow Lecture Notes Technische Universit¨atBerlin Sommersemester 2018 preliminary version April 18th 2019 Contents 1 Processes, Filtrations, Martingales 1 1.1 Foundations . 1 1.2 Filtrations and stopping times . 2 1.3 Martingales . 7 1.4 Semimartingales, Quadratic Variation . 11 2 Stochastic Integrals and Stochastic Differential Equations 19 2.1 The stochastic integral . 19 2.2 It^o'sformula . 24 2.3 Representation of local martingales . 27 2.4 Stochastic differential equations . 28 3 L´evyProcesses 39 4 Markov Processes 43 4.1 Markov transition functions and Markov processes . 43 4.2 Strong Markov property . 49 4.3 Hille-Yosida Theory . 54 4.4 Invariant measures: existence . 61 4.5 Invariant measures: uniqueness . 65 4.6 Coupling, optimal transportation and Wasserstein distance . 69 5 Appendix 71 Bibliography 73 i Chapter 1 Processes, Filtrations, Martingales 1.1 Foundations Most of this chapter can be found in the first chapter of the monograph [KS91] or in [RY94]. Definition 1.1. Let (Ω; F) and (E; E) be measurable spaces and I a (non-empty) index set. A collection X = (Xt)t2I of measurable maps from (Ω; F) to (E; E) is called (E-valued) process. If { in addition { a probability measure is specified on (Ω; F), then we call X a stochastic process. Notation 1.2. If (E; d) is a metric space (or, more generally, E is a topological space), then we denote its Borel-σ-algebra (i.e. the smallest σ-algebra containing all open subsets of E) by d B(E).
    [Show full text]
  • Stochastic Process
    Stochastic Process Kazufumi Ito∗ August 19, 2013 1 Markov Chain In this section consider the discrete time stochastic process. Let S be the state space, e.g., S = Z = fintegersg, S = f0; 1; ··· ;Ng and S = {−N; ··· ; 0; ··· ;Ng. Definition We say that a stochastic process fXng; n ≥ 0 is a Markov chain with initial distribution π (P (X0) = πi) and (one-step) transition matrix P if for each n and ik; 0 ≤ k ≤ n − 1 P (Xn+1 = jjXn = i; Xn−1 = in−1; ··· ;X0 = i0) = P (Xn+1 = jjXn = i) = pij ≥ with X pij = 1; pij ≥ 0: j2S Thus, the distribution of Xn+1 depends only on the current state Xn and is independent of the past. Example Xn+1 = f(Xn; wn); f : S × R ! S; where fwng is independent identically distributed random variables and P (f(x; w) = jjx = i) = pij: The following theorem follows; n n Theorem Let P = fpij. X 2 (2) P (Xn+2 = jjXn = i) = pikpkj = (P )ij = pij k2S n X (n) P (Xn = j) = (πP )j = πipi;j and (m+n) X (n) (m) pij = pik pkj (Chapman-Kolmogorov): k2S ∗Department of Mathematics, North Carolina State University, Raleigh, North Carolina, USA 1 1.1 Classification of the States In this action we analyze the asymptotic behavior of the Markov chain, e.g. including (n) Questions (1) The limits πj = limn!1 pij exist are are independent of i. P (2) The limits (π1; π2; ··· ) form a probability distribution, that is, π ≥ 0 and πi = 1. (3) The chain is ergotic, i.e., πi > 0.
    [Show full text]
  • Markovian Queueing Networks
    Richard J. Boucherie Markovian queueing networks Lecture notes LNMB course MQSN September 5, 2020 Springer Contents Part I Solution concepts for Markovian networks of queues 1 Preliminaries .................................................. 3 1.1 Basic results for Markov chains . .3 1.2 Three solution concepts . 11 1.2.1 Reversibility . 12 1.2.2 Partial balance . 13 1.2.3 Kelly’s lemma . 13 2 Reversibility, Poisson flows and feedforward networks. 15 2.1 The birth-death process. 15 2.2 Detailed balance . 18 2.3 Erlang loss networks . 21 2.4 Reversibility . 23 2.5 Burke’s theorem and feedforward networks of MjMj1 queues . 25 2.6 Literature . 28 3 Partial balance and networks with Markovian routing . 29 3.1 Networks of MjMj1 queues . 29 3.2 Kelly-Whittle networks. 35 3.3 Partial balance . 39 3.4 State-dependent routing and blocking protocols . 44 3.5 Literature . 50 4 Kelly’s lemma and networks with fixed routes ..................... 51 4.1 The time-reversed process and Kelly’s Lemma . 51 4.2 Queue disciplines . 53 4.3 Networks with customer types and fixed routes . 59 4.4 Quasi-reversibility . 62 4.5 Networks of quasi-reversible queues with fixed routes . 68 4.6 Literature . 70 v Part I Solution concepts for Markovian networks of queues Chapter 1 Preliminaries This chapter reviews and discusses the basic assumptions and techniques that will be used in this monograph. Proofs of results given in this chapter are omitted, but can be found in standard textbooks on Markov chains and queueing theory, e.g. [?, ?, ?, ?, ?, ?, ?]. Results from these references are used in this chapter without reference except for cases where a specific result (e.g.
    [Show full text]