1 Introduction to Markov Random Fields
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Multivariate Poisson Hidden Markov Models for Analysis of Spatial Counts
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by University of Saskatchewan's Research Archive MULTIVARIATE POISSON HIDDEN MARKOV MODELS FOR ANALYSIS OF SPATIAL COUNTS A Thesis Submitted to the Faculty of Graduate Studies and Research in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy in the Department of Mathematics and Statistics University of Saskatchewan, Saskatoon, SK, Canada by Chandima Piyadharshani Karunanayake @Copyright Chandima Piyadharshani Karunanayake, June 2007. All rights Reserved. PERMISSION TO USE The author has agreed that the libraries of this University may provide the thesis freely available for inspection. Moreover, the author has agreed that permission for copying of the thesis in any manner, entirely or in part, for scholarly purposes may be granted by the Professor or Professors who supervised my thesis work or in their absence, by the Head of the Department of Mathematics and Statistics or the Dean of the College in which the thesis work was done. It is understood that any copying or publication or use of the thesis or parts thereof for finanancial gain shall not be allowed without my written permission. It is also understood that due recognition shall be given to the author and to the University of Saskatchewan in any scholarly use which may be made of any material in this thesis. Requests for permission to copy or to make other use of any material in the thesis should be addressed to: Head Department of Mathematics and Statistics University of Saskatchewan 106, Wiggins Road Saskatoon, Saskatchewan Canada, S7N 5E6 i ABSTRACT Multivariate count data are found in a variety of fields. -
Inference Algorithm for Finite-Dimensional Spin
PHYSICAL REVIEW E 84, 046706 (2011) Inference algorithm for finite-dimensional spin glasses: Belief propagation on the dual lattice Alejandro Lage-Castellanos and Roberto Mulet Department of Theoretical Physics and Henri-Poincare´ Group of Complex Systems, Physics Faculty, University of Havana, La Habana, Codigo Postal 10400, Cuba Federico Ricci-Tersenghi Dipartimento di Fisica, INFN–Sezione di Roma 1, and CNR–IPCF, UOS di Roma, Universita` La Sapienza, Piazzale Aldo Moro 5, I-00185 Roma, Italy Tommaso Rizzo Dipartimento di Fisica and CNR–IPCF, UOS di Roma, Universita` La Sapienza, Piazzale Aldo Moro 5, I-00185 Roma, Italy (Received 18 February 2011; revised manuscript received 15 September 2011; published 24 October 2011) Starting from a cluster variational method, and inspired by the correctness of the paramagnetic ansatz [at high temperatures in general, and at any temperature in the two-dimensional (2D) Edwards-Anderson (EA) model] we propose a message-passing algorithm—the dual algorithm—to estimate the marginal probabilities of spin glasses on finite-dimensional lattices. We use the EA models in 2D and 3D as benchmarks. The dual algorithm improves the Bethe approximation, and we show that in a wide range of temperatures (compared to the Bethe critical temperature) our algorithm compares very well with Monte Carlo simulations, with the double-loop algorithm, and with exact calculation of the ground state of 2D systems with bimodal and Gaussian interactions. Moreover, it is usually 100 times faster than other provably convergent methods, as the double-loop algorithm. In 2D and 3D the quality of the inference deteriorates only where the correlation length becomes very large, i.e., at low temperatures in 2D and close to the critical temperature in 3D. -
Regime Heteroskedasticity in Bitcoin: a Comparison of Markov Switching Models
Munich Personal RePEc Archive Regime heteroskedasticity in Bitcoin: A comparison of Markov switching models Chappell, Daniel Birkbeck College, University of London 28 September 2018 Online at https://mpra.ub.uni-muenchen.de/90682/ MPRA Paper No. 90682, posted 24 Dec 2018 06:38 UTC Regime heteroskedasticity in Bitcoin: A comparison of Markov switching models Daniel R. Chappell Department of Economics, Mathematics and Statistics Birkbeck College, University of London [email protected] 28th September 2018 Abstract Markov regime-switching (MRS) models, also known as hidden Markov models (HMM), are used extensively to account for regime heteroskedasticity within the returns of financial assets. However, we believe this paper to be one of the first to apply such methodology to the time series of cryptocurrencies. In light of Moln´arand Thies (2018) demonstrating that the price data of Bitcoin contained seven distinct volatility regimes, we will fit a sample of Bitcoin returns with six m-state MRS estimations, with m ∈ {2,..., 7}. Our aim is to identify the optimal number of states for modelling the regime heteroskedasticity in the price data of Bitcoin. Goodness-of-fit will be judged using three information criteria, namely: Bayesian (BIC); Hannan-Quinn (HQ); and Akaike (AIC). We determined that the restricted 5-state model generated the optimal estima- tion for the sample. In addition, we found evidence of volatility clustering, volatility jumps and asymmetric volatility transitions whilst also inferring the persistence of shocks in the price data of Bitcoin. Keywords Bitcoin; Markov regime-switching; regime heteroskedasticity; volatility transitions. 1 2 List of Tables Table 1. Summary statistics for Bitcoin (23rd April 2014 to 31st May 2018) . -
Methods of Monte Carlo Simulation II
Methods of Monte Carlo Simulation II Ulm University Institute of Stochastics Lecture Notes Dr. Tim Brereton Summer Term 2014 Ulm, 2014 2 Contents 1 SomeSimpleStochasticProcesses 7 1.1 StochasticProcesses . 7 1.2 RandomWalks .......................... 7 1.2.1 BernoulliProcesses . 7 1.2.2 RandomWalks ...................... 10 1.2.3 ProbabilitiesofRandomWalks . 13 1.2.4 Distribution of Xn .................... 13 1.2.5 FirstPassageTime . 14 2 Estimators 17 2.1 Bias, Variance, the Central Limit Theorem and Mean Square Error................................ 19 2.2 Non-AsymptoticErrorBounds. 22 2.3 Big O and Little o Notation ................... 23 3 Markov Chains 25 3.1 SimulatingMarkovChains . 28 3.1.1 Drawing from a Discrete Uniform Distribution . 28 3.1.2 Drawing From A Discrete Distribution on a Small State Space ........................... 28 3.1.3 SimulatingaMarkovChain . 28 3.2 Communication .......................... 29 3.3 TheStrongMarkovProperty . 30 3.4 RecurrenceandTransience . 31 3.4.1 RecurrenceofRandomWalks . 33 3.5 InvariantDistributions . 34 3.6 LimitingDistribution. 36 3.7 Reversibility............................ 37 4 The Poisson Process 39 4.1 Point Processes on [0, )..................... 39 ∞ 3 4 CONTENTS 4.2 PoissonProcess .......................... 41 4.2.1 Order Statistics and the Distribution of Arrival Times 44 4.2.2 DistributionofArrivalTimes . 45 4.3 SimulatingPoissonProcesses. 46 4.3.1 Using the Infinitesimal Definition to Simulate Approx- imately .......................... 46 4.3.2 SimulatingtheArrivalTimes . 47 4.3.3 SimulatingtheInter-ArrivalTimes . 48 4.4 InhomogenousPoissonProcesses. 48 4.5 Simulating an Inhomogenous Poisson Process . 49 4.5.1 Acceptance-Rejection. 49 4.5.2 Infinitesimal Approach (Approximate) . 50 4.6 CompoundPoissonProcesses . 51 5 ContinuousTimeMarkovChains 53 5.1 TransitionFunction. 53 5.2 InfinitesimalGenerator . 54 5.3 ContinuousTimeMarkovChains . -
12 : Conditional Random Fields 1 Hidden Markov Model
10-708: Probabilistic Graphical Models 10-708, Spring 2014 12 : Conditional Random Fields Lecturer: Eric P. Xing Scribes: Qin Gao, Siheng Chen 1 Hidden Markov Model 1.1 General parametric form In hidden Markov model (HMM), we have three sets of parameters, j i transition probability matrix A : p(yt = 1jyt−1 = 1) = ai;j; initialprobabilities : p(y1) ∼ Multinomial(π1; π2; :::; πM ); i emission probabilities : p(xtjyt) ∼ Multinomial(bi;1; bi;2; :::; bi;K ): 1.2 Inference k k The inference can be done with forward algorithm which computes αt ≡ µt−1!t(k) = P (x1; :::; xt−1; xt; yt = 1) recursively by k k X i αt = p(xtjyt = 1) αt−1ai;k; (1) i k k and the backward algorithm which computes βt ≡ µt t+1(k) = P (xt+1; :::; xT jyt = 1) recursively by k X i i βt = ak;ip(xt+1jyt+1 = 1)βt+1: (2) i Another key quantity is the conditional probability of any hidden state given the entire sequence, which can be computed by the dot product of forward message and backward message by, i i i i X i;j γt = p(yt = 1jx1:T ) / αtβt = ξt ; (3) j where we define, i;j i j ξt = p(yt = 1; yt−1 = 1; x1:T ); i j / µt−1!t(yt = 1)µt t+1(yt+1 = 1)p(xt+1jyt+1)p(yt+1jyt); i j i = αtβt+1ai;jp(xt+1jyt+1 = 1): The implementation in Matlab can be vectorized by using, i Bt(i) = p(xtjyt = 1); j i A(i; j) = p(yt+1 = 1jyt = 1): 1 2 12 : Conditional Random Fields The relation of those quantities can be simply written in pseudocode as, T αt = (A αt−1): ∗ Bt; βt = A(βt+1: ∗ Bt+1); T ξt = (αt(βt+1: ∗ Bt+1) ): ∗ A; γt = αt: ∗ βt: 1.3 Learning 1.3.1 Supervised Learning The supervised learning is trivial if only we know the true state path. -
Modeling Dependence in Data: Options Pricing and Random Walks
UNIVERSITY OF CALIFORNIA, MERCED PH.D. DISSERTATION Modeling Dependence in Data: Options Pricing and Random Walks Nitesh Kumar A dissertation submitted in partial fulfillment of the requirements for the degree Doctor of Philosophy in Applied Mathematics March, 2013 UNIVERSITY OF CALIFORNIA, MERCED Graduate Division This is to certify that I have examined a copy of a dissertation by Nitesh Kumar and found it satisfactory in all respects, and that any and all revisions required by the examining committee have been made. Faculty Advisor: Harish S. Bhat Committee Members: Arnold D. Kim Roummel F. Marcia Applied Mathematics Graduate Studies Chair: Boaz Ilan Arnold D. Kim Date Contents 1 Introduction 2 1.1 Brief Review of the Option Pricing Problem and Models . ......... 2 2 Markov Tree: Discrete Model 6 2.1 Introduction.................................... 6 2.2 Motivation...................................... 7 2.3 PastWork....................................... 8 2.4 Order Estimation: Methodology . ...... 9 2.5 OrderEstimation:Results. ..... 13 2.6 MarkovTreeModel:Theory . 14 2.6.1 NoArbitrage.................................. 17 2.6.2 Implementation Notes. 18 2.7 TreeModel:Results................................ 18 2.7.1 Comparison of Model and Market Prices. 19 2.7.2 Comparison of Volatilities. 20 2.8 Conclusion ...................................... 21 3 Markov Tree: Continuous Model 25 3.1 Introduction.................................... 25 3.2 Markov Tree Generation and Computational Tractability . ............. 26 3.2.1 Persistentrandomwalk. 27 3.2.2 Number of states in a tree of fixed depth . ..... 28 3.2.3 Markov tree probability mass function . ....... 28 3.3 Continuous Approximation of the Markov Tree . ........ 30 3.3.1 Recursion................................... 30 3.3.2 Exact solution in Fourier space . -
The Ising Model
The Ising Model Today we will switch topics and discuss one of the most studied models in statistical physics the Ising Model • Some applications: – Magnetism (the original application) – Liquid-gas transition – Binary alloys (can be generalized to multiple components) • Onsager solved the 2D square lattice (1D is easy!) • Used to develop renormalization group theory of phase transitions in 1970’s. • Critical slowing down and “cluster methods”. Figures from Landau and Binder (LB), MC Simulations in Statistical Physics, 2000. Atomic Scale Simulation 1 The Model • Consider a lattice with L2 sites and their connectivity (e.g. a square lattice). • Each lattice site has a single spin variable: si = ±1. • With magnetic field h, the energy is: N −β H H = −∑ Jijsis j − ∑ hisi and Z = ∑ e ( i, j ) i=1 • J is the nearest neighbors (i,j) coupling: – J > 0 ferromagnetic. – J < 0 antiferromagnetic. • Picture of spins at the critical temperature Tc. (Note that connected (percolated) clusters.) Atomic Scale Simulation 2 Mapping liquid-gas to Ising • For liquid-gas transition let n(r) be the density at lattice site r and have two values n(r)=(0,1). E = ∑ vijnin j + µ∑ni (i, j) i • Let’s map this into the Ising model spin variables: 1 s = 2n − 1 or n = s + 1 2 ( ) v v + µ H s s ( ) s c = ∑ i j + ∑ i + 4 (i, j) 2 i J = −v / 4 h = −(v + µ) / 2 1 1 1 M = s n = n = M + 1 N ∑ i N ∑ i 2 ( ) i i Atomic Scale Simulation 3 JAVA Ising applet http://physics.weber.edu/schroeder/software/demos/IsingModel.html Dynamically runs using heat bath algorithm. -
A Class of Measure-Valued Markov Chains and Bayesian Nonparametrics
Bernoulli 18(3), 2012, 1002–1030 DOI: 10.3150/11-BEJ356 A class of measure-valued Markov chains and Bayesian nonparametrics STEFANO FAVARO1, ALESSANDRA GUGLIELMI2 and STEPHEN G. WALKER3 1Universit`adi Torino and Collegio Carlo Alberto, Dipartimento di Statistica e Matematica Ap- plicata, Corso Unione Sovietica 218/bis, 10134 Torino, Italy. E-mail: [email protected] 2Politecnico di Milano, Dipartimento di Matematica, P.zza Leonardo da Vinci 32, 20133 Milano, Italy. E-mail: [email protected] 3University of Kent, Institute of Mathematics, Statistics and Actuarial Science, Canterbury CT27NZ, UK. E-mail: [email protected] Measure-valued Markov chains have raised interest in Bayesian nonparametrics since the seminal paper by (Math. Proc. Cambridge Philos. Soc. 105 (1989) 579–585) where a Markov chain having the law of the Dirichlet process as unique invariant measure has been introduced. In the present paper, we propose and investigate a new class of measure-valued Markov chains defined via exchangeable sequences of random variables. Asymptotic properties for this new class are derived and applications related to Bayesian nonparametric mixture modeling, and to a generalization of the Markov chain proposed by (Math. Proc. Cambridge Philos. Soc. 105 (1989) 579–585), are discussed. These results and their applications highlight once again the interplay between Bayesian nonparametrics and the theory of measure-valued Markov chains. Keywords: Bayesian nonparametrics; Dirichlet process; exchangeable sequences; linear functionals -
A Study of Hidden Markov Model
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Masters Theses Graduate School 8-2004 A Study of Hidden Markov Model Yang Liu University of Tennessee - Knoxville Follow this and additional works at: https://trace.tennessee.edu/utk_gradthes Part of the Mathematics Commons Recommended Citation Liu, Yang, "A Study of Hidden Markov Model. " Master's Thesis, University of Tennessee, 2004. https://trace.tennessee.edu/utk_gradthes/2326 This Thesis is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Masters Theses by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a thesis written by Yang Liu entitled "A Study of Hidden Markov Model." I have examined the final electronic copy of this thesis for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Master of Science, with a major in Mathematics. Jan Rosinski, Major Professor We have read this thesis and recommend its acceptance: Xia Chen, Balram Rajput Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) To the Graduate Council: I am submitting herewith a thesis written by Yang Liu entitled “A Study of Hidden Markov Model.” I have examined the final electronic copy of this thesis for form and content and recommend that it be accepted in partial fulfillment of the requirements for the degree of Master of Science, with a major in Mathematics. -
Many-Pairs Mutual Information for Adding Structure to Belief Propagation Approximations
Proceedings of the Twenty-Third AAAI Conference on Artificial Intelligence (2008) Many-Pairs Mutual Information for Adding Structure to Belief Propagation Approximations Arthur Choi and Adnan Darwiche Computer Science Department University of California, Los Angeles Los Angeles, CA 90095 {aychoi,darwiche}@cs.ucla.edu Abstract instances of the satisfiability problem (Braunstein, Mezard,´ and Zecchina 2005). IBP has also been applied towards a We consider the problem of computing mutual informa- variety of computer vision tasks (Szeliski et al. 2006), par- tion between many pairs of variables in a Bayesian net- work. This task is relevant to a new class of Generalized ticularly stereo vision, where methods based on belief prop- Belief Propagation (GBP) algorithms that characterizes agation have been particularly successful. Iterative Belief Propagation (IBP) as a polytree approx- The successes of IBP as an approximate inference algo- imation found by deleting edges in a Bayesian network. rithm spawned a number of generalizations, in the hopes of By computing, in the simplified network, the mutual in- understanding the nature of IBP, and further to improve on formation between variables across a deleted edge, we the quality of its approximations. Among the most notable can estimate the impact that recovering the edge might are the family of Generalized Belief Propagation (GBP) al- have on the approximation. Unfortunately, it is compu- gorithms (Yedidia, Freeman, and Weiss 2005), where the tationally impractical to compute such scores for net- works over many variables having large state spaces. “structure” of an approximation is given by an auxiliary So that edge recovery can scale to such networks, we graph called a region graph, which specifies (roughly) which propose in this paper an approximation of mutual in- regions of the original network should be handled exactly, formation which is based on a soft extension of d- and to what extent different regions should be mutually con- separation (a graphical test of independence in Bayesian sistent. -
Markov Process Duality
Markov Process Duality Jan M. Swart Luminy, October 23 and 24, 2013 Jan M. Swart Markov Process Duality Markov Chains S finite set. RS space of functions f : S R. ! S For probability kernel P = (P(x; y))x;y2S and f R define left and right multiplication as 2 X X Pf (x) := P(x; y)f (y) and fP(x) := f (y)P(y; x): y y (I do not distinguish row and column vectors.) Def Chain X = (Xk )k≥0 of S-valued r.v.'s is Markov chain with transition kernel P and state space S if S E f (Xk+1) (X0;:::; Xk ) = Pf (Xk ) a:s: (f R ) 2 P (X0;:::; Xk ) = (x0;:::; xk ) , = P[X0 = x0]P(x0; x1) P(xk−1; xk ): ··· µ µ µ Write P ; E for process with initial law µ = P [X0 ]. x δx x 2 · P := P with δx (y) := 1fx=yg. E similar. Jan M. Swart Markov Process Duality Markov Chains Set k µ k x µk := µP (x) = P [Xk = x] and fk := P f (x) = E [f (Xk )]: Then the forward and backward equations read µk+1 = µk P and fk+1 = Pfk : In particular π invariant law iff πP = π. Function h harmonic iff Ph = h h(Xk ) martingale. , Jan M. Swart Markov Process Duality Random mapping representation (Zk )k≥1 i.i.d. with common law ν, take values in (E; ). φ : S E S measurable E × ! P(x; y) = P[φ(x; Z1) = y]: Random mapping representation (E; ; ν; φ) always exists, highly non-unique. -
1 Introduction Branching Mechanism in a Superprocess from a Branching
数理解析研究所講究録 1157 巻 2000 年 1-16 1 An example of random snakes by Le Gall and its applications 渡辺信三 Shinzo Watanabe, Kyoto University 1 Introduction The notion of random snakes has been introduced by Le Gall ([Le 1], [Le 2]) to construct a class of measure-valued branching processes, called superprocesses or continuous state branching processes ([Da], [Dy]). A main idea is to produce the branching mechanism in a superprocess from a branching tree embedded in excur- sions at each different level of a Brownian sample path. There is no clear notion of particles in a superprocess; it is something like a cloud or mist. Nevertheless, a random snake could provide us with a clear picture of historical or genealogical developments of”particles” in a superprocess. ” : In this note, we give a sample pathwise construction of a random snake in the case when the underlying Markov process is a Markov chain on a tree. A simplest case has been discussed in [War 1] and [Wat 2]. The construction can be reduced to this case locally and we need to consider a recurrence family of stochastic differential equations for reflecting Brownian motions with sticky boundaries. A special case has been already discussed by J. Warren [War 2] with an application to a coalescing stochastic flow of piece-wise linear transformations in connection with a non-white or non-Gaussian predictable noise in the sense of B. Tsirelson. 2 Brownian snakes Throughout this section, let $\xi=\{\xi(t), P_{x}\}$ be a Hunt Markov process on a locally compact separable metric space $S$ endowed with a metric $d_{S}(\cdot, *)$ .