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Data Assimilation and Parameter Estimation for a Multiscale Stochastic System with Α-Stable Lévy Noise
Data assimilation and parameter estimation for a multiscale stochastic system with α-stable L´evy noise Yanjie Zhang1, Zhuan Cheng2, Xinyong Zhang3, Xiaoli Chen1, Jinqiao Duan2 and Xiaofan Li2 1Center for Mathematical Sciences & School of Mathematics and Statistics, Huazhong University of Science and Technology, Wuhan 430074, China 2Department of Applied Mathematics, Illinois Institute of Technology, Chicago, IL 60616, USA 3Department of Mathematical Sciences, Tsinghua University, Beijing 100084, China E-mail: [email protected], [email protected], [email protected], [email protected], [email protected] and [email protected] . ∗This work was partly supported by the NSF grant 1620449, and NSFC grants 11531006, 11371367, and 11271290. Abstract. This work is about low dimensional reduction for a slow-fast data assimilation system with non-Gaussian α stable L´evy noise via stochastic averaging. − When the observations are only available for slow components, we show that the averaged, low dimensional filter approximates the original filter, by examining the corresponding Zakai stochastic partial differential equations. Furthermore, we demonstrate that the low dimensional slow system approximates the slow dynamics of the original system, by examining parameter estimation and most probable paths. Keywords: Multiscale systems, non-Gaussian L´evy noise, averaging principle, Zakai equation, parameter estimation, most probable paths arXiv:1801.02846v1 [math.DS] 9 Jan 2018 1. Introduction Data assimilation is a procedure to extract system state information with the help of observations [18]. The state evolution and the observations are usually under random fluctuations. The general idea is to gain the best estimate for the true system state, in terms of the probability distribution for the system state, given only some noisy observations of the system. -
Limit Theorems for Non-Stationary and Random
LIMIT THEOREMS FOR NON-STATIONARY AND RANDOM DYNAMICAL SYSTEMS by Yaofeng Su A dissertation submitted to the Department of Mathematics, College of Natural Sciences and Mathematics in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Mathematics Chair of Committee: Andrew T¨or¨ok Committee Member: Vaughn Climenhaga Committee Member: Gemunu Gunaratne Committee Member: Matthew Nicol University of Houston May 2020 Copyright 2020, Yaofeng Su ACKNOWLEDGMENTS This dissertation would not have been possible without the guidance and the help of several in- dividuals who in one way or another contributed and extended their valuable assistance in the preparation and completion of this study. First, my utmost gratitude to my advisor Dr. Andrew T¨or¨okfor the support and help he provided me throughout my graduate education; my commit- tee members, Dr. Vaughn Climenhaga, Dr. Gemunu Gunaratne, and Dr. Matthew Nicol for their participation and their thoughtful comments; all professors in the dynamical system research group of University of Houston, Dr. Vaughn Climenhaga, Dr. Alan Haynes, Dr. Matthew Nicol, Dr. William Ott, and Dr. Andrew T¨or¨okfor organizing the wonderful \Houston Summer School on Dynamical Systems", where I learned a lot about dynamical systems, ergodic theory, number theory, and quantum mechanics. iii ABSTRACT We study the limit behavior of the non-stationary/random chaotic dynamical systems and prove a strong statistical limit theorem: (vector-valued) almost sure invariance principle for the non- stationary dynamical systems and quenched (vector-valued) almost sure invariance principle for the random dynamical systems. It is a matching of the trajectories of the dynamical system with a Brownian motion in such a way that the error is negligible in comparison with the Birkhoff sum. -
MAST31801 Mathematical Finance II, Spring 2019. Problem Sheet 8 (4-8.4.2019)
UH|Master program Mathematics and Statistics|MAST31801 Mathematical Finance II, Spring 2019. Problem sheet 8 (4-8.4.2019) 1. Show that a local martingale (Xt : t ≥ 0) in a filtration F, which is bounded from below is a supermartingale. Hint: use localization together with Fatou lemma. 2. A non-negative local martingale Xt ≥ 0 is a martingale if and only if E(Xt) = E(X0) 8t. 3. Recall Ito formula, for f(x; s) 2 C2;1 and a continuous semimartingale Xt with quadratic covariation hXit 1 Z t @2f Z t @f Z t @f f(Xt; t) − f(X0; 0) − 2 (Xs; s)dhXis − (Xs; s)ds = (Xs; s)dXs 2 0 @x 0 @s 0 @x where on the right side we have the Ito integral. We can also understand the Ito integral as limit in probability of Riemann sums X @f n n n n X(tk−1); tk−1 X(tk ^ t) − X(tk−1 ^ t) n n @x tk 2Π among a sequence of partitions Πn with ∆(Πn) ! 0. Recalling that the Brownian motion Wt has quadratic variation hW it = t, write the following Ito integrals explicitely by using Ito formula: R t n (a) 0 Ws dWs, n 2 N. R t (b) 0 exp σWs σdWs R t 2 (c) 0 exp σWs − σ s=2 σdWs R t (d) 0 sin(σWs)dWs R t (e) 0 cos(σWs)dWs 4. These Ito integrals as stochastic processes are semimartingales. Com- pute the quadratic variation of the Ito-integrals above. Hint: recall that the finite variation part of a semimartingale has zero quadratic variation, and the quadratic variation is bilinear. -
Math.DS] 5 Aug 2014 Etns E PK O Opeesv Uvyo H Ujc.I Subject
SYNCHRONIZATION PROPERTIES OF RANDOM PIECEWISE ISOMETRIES VICTOR KLEPTSYN AND ANTON GORODETSKI Abstract. We study the synchronization properties of the random double rotations on tori. We give a criterion that show when synchronization is present in the case of random double rotations on the circle and prove that it is always absent in dimensions two and higher. 1. Introduction The observation of a synchronization effect goes back at least to 17th century, when Huygens [Hu] discovered the synchronization of two linked pendulums. Since then, synchronization phenomena have been observed in numerous systems and settings, see [PRK] for a comprehensive survey of the subject. In the theory of dynamical systems, synchronization usually refers to random dynamical system trajectories of different initial points converging to each other under the applica- tion of a sequence of random transformations. A first such result is the famous Furstenberg’s Theorem [Fur1], stating that under some very mild assumptions, the angle (mod π) between the images of any two vectors under a long product of random matrices (exponentially) tends to zero. Projectivizing the dynamics, it is easy to see that this theorem in fact states that random trajectories of the quotient system on the projective space (exponentially) approach each other. For random dynamical systems on the circle, several results are known. Surely, in random projective dynamics there is a synchronization due to the simplest pos- sible case of Furstenberg’s Theorem. In 1984, this result was generalized to the setting of homeomorphisms (with some very mild and natural assumptions of min- imality of the action and the presence of a North-South map) in the work of a physicist V. -
A Model of Gene Expression Based on Random Dynamical Systems Reveals Modularity Properties of Gene Regulatory Networks†
A Model of Gene Expression Based on Random Dynamical Systems Reveals Modularity Properties of Gene Regulatory Networks† Fernando Antoneli1,4,*, Renata C. Ferreira3, Marcelo R. S. Briones2,4 1 Departmento de Informática em Saúde, Escola Paulista de Medicina (EPM), Universidade Federal de São Paulo (UNIFESP), SP, Brasil 2 Departmento de Microbiologia, Imunologia e Parasitologia, Escola Paulista de Medicina (EPM), Universidade Federal de São Paulo (UNIFESP), SP, Brasil 3 College of Medicine, Pennsylvania State University (Hershey), PA, USA 4 Laboratório de Genômica Evolutiva e Biocomplexidade, EPM, UNIFESP, Ed. Pesquisas II, Rua Pedro de Toledo 669, CEP 04039-032, São Paulo, Brasil Abstract. Here we propose a new approach to modeling gene expression based on the theory of random dynamical systems (RDS) that provides a general coupling prescription between the nodes of any given regulatory network given the dynamics of each node is modeled by a RDS. The main virtues of this approach are the following: (i) it provides a natural way to obtain arbitrarily large networks by coupling together simple basic pieces, thus revealing the modularity of regulatory networks; (ii) the assumptions about the stochastic processes used in the modeling are fairly general, in the sense that the only requirement is stationarity; (iii) there is a well developed mathematical theory, which is a blend of smooth dynamical systems theory, ergodic theory and stochastic analysis that allows one to extract relevant dynamical and statistical information without solving -
Derivatives of Self-Intersection Local Times
Derivatives of self-intersection local times Jay Rosen? Department of Mathematics College of Staten Island, CUNY Staten Island, NY 10314 e-mail: [email protected] Summary. We show that the renormalized self-intersection local time γt(x) for both the Brownian motion and symmetric stable process in R1 is differentiable in 0 the spatial variable and that γt(0) can be characterized as the continuous process of zero quadratic variation in the decomposition of a natural Dirichlet process. This Dirichlet process is the potential of a random Schwartz distribution. Analogous results for fractional derivatives of self-intersection local times in R1 and R2 are also discussed. 1 Introduction In their study of the intrinsic Brownian local time sheet and stochastic area integrals for Brownian motion, [14, 15, 16], Rogers and Walsh were led to analyze the functional Z t A(t, Bt) = 1[0,∞)(Bt − Bs) ds (1) 0 where Bt is a 1-dimensional Brownian motion. They showed that A(t, Bt) is not a semimartingale, and in fact showed that Z t Bs A(t, Bt) − Ls dBs (2) 0 x has finite non-zero 4/3-variation. Here Ls is the local time at x, which is x R s formally Ls = 0 δ(Br − x) dr, where δ(x) is Dirac’s ‘δ-function’. A formal d d2 0 application of Ito’s lemma, using dx 1[0,∞)(x) = δ(x) and dx2 1[0,∞)(x) = δ (x), yields Z t 1 Z t Z s Bs 0 A(t, Bt) − Ls dBs = t + δ (Bs − Br) dr ds (3) 0 2 0 0 ? This research was supported, in part, by grants from the National Science Foun- dation and PSC-CUNY. -
Skorohod Stochastic Integration with Respect to Non-Adapted Processes on Wiener Space Nicolas Privault
Skorohod stochastic integration with respect to non-adapted processes on Wiener space Nicolas Privault Equipe d'Analyse et Probabilit´es,Universit´ed'Evry-Val d'Essonne Boulevard des Coquibus, 91025 Evry Cedex, France e-mail: [email protected] Abstract We define a Skorohod type anticipative stochastic integral that extends the It^ointegral not only with respect to the Wiener process, but also with respect to a wide class of stochastic processes satisfying certain homogeneity and smoothness conditions, without requirements relative to filtrations such as adaptedness. Using this integral, a change of variable formula that extends the classical and Skorohod It^oformulas is obtained. Key words: It^ocalculus, Malliavin calculus, Skorohod integral. Mathematics Subject Classification (1991): 60H05, 60H07. 1 Introduction The Skorohod integral, defined by creation on Fock space, is an extension of the It^o integral with respect to the Wiener or Poisson processes, depending on the probabilis- tic interpretation chosen for the Fock space. This means that it coincides with the It^ointegral on square-integrable adapted processes. It can also extend the stochastic integral with respect to certain normal martingales, cf. [10], but it always acts with respect to the underlying process relative to a given probabilistic interpretation. The Skorohod integral is also linked to the Stratonovich, forward and backward integrals, and allows to extend the It^oformula to a class of Skorohod integral processes which contains non-adapted processes that have a certain structure. In this paper we introduce an extended Skorohod stochastic integral on Wiener space that can act with respect to processes other than Brownian motion. -
Lecture 19 Semimartingales
Lecture 19:Semimartingales 1 of 10 Course: Theory of Probability II Term: Spring 2015 Instructor: Gordan Zitkovic Lecture 19 Semimartingales Continuous local martingales While tailor-made for the L2-theory of stochastic integration, martin- 2,c gales in M0 do not constitute a large enough class to be ultimately useful in stochastic analysis. It turns out that even the class of all mar- tingales is too small. When we restrict ourselves to processes with continuous paths, a naturally stable family turns out to be the class of so-called local martingales. Definition 19.1 (Continuous local martingales). A continuous adapted stochastic process fMtgt2[0,¥) is called a continuous local martingale if there exists a sequence ftngn2N of stopping times such that 1. t1 ≤ t2 ≤ . and tn ! ¥, a.s., and tn 2. fMt gt2[0,¥) is a uniformly integrable martingale for each n 2 N. In that case, the sequence ftngn2N is called the localizing sequence for (or is said to reduce) fMtgt2[0,¥). The set of all continuous local loc,c martingales M with M0 = 0 is denoted by M0 . Remark 19.2. 1. There is a nice theory of local martingales which are not neces- sarily continuous (RCLL), but, in these notes, we will focus solely on the continuous case. In particular, a “martingale” or a “local martingale” will always be assumed to be continuous. 2. While we will only consider local martingales with M0 = 0 in these notes, this is assumption is not standard, so we don’t put it into the definition of a local martingale. tn 3. -
The Mathematics of Critical Shifts in Ecological Networks with Alternative Stable State Theory, a Potential Framework for Early Warning Indicators
The Mathematics of Critical Shifts in Ecological Networks with Alternative Stable State Theory, A Potential Framework for Early Warning Indicators by Michael Kupperman A THESIS submitted to Oregon State University Honors College in partial fulfillment of the requirements for the degree of Honors Bachelors of Science in Mathematics (Honors Scholar) Honors Bachelors of Science in Biochemistry & Molecular Biology (Honors Scholar) Presented June 14, 2019 Commencement June 2020 AN ABSTRACT OF THE THESIS OF Michael Kupperman for the degree of Honors Bachelors of Science in Mathematics and Honors Bachelors of Science in Biochemistry & Molecular Biology presented on June 14, 2019. Title: The Mathematics of Critical Shifts in Ecological Networks with Alternative Stable State Theory, A Potential Framework for Early Warning Indicators Abstract approved: David Koslicki A long running problem in mathematical biology is the prediction of extinction events, a specialized case of the larger global stability problem found in differential equations and dynamical systems theory. A central technical question is how to introduce the randomness observed in real ecological systems not accounted for in deterministic models. This work introduces the SP-system as a new mathematical object in which ecological parameters are treated as sequences of random variables that attain values over intervals of random lengths of time. The SP-system characterization of ecological networks leads to two differ- ent novel approaches for the simulation and extinction prediction. The first approach uses a construct new to modeling literature to describe the probability of a parameter transition event into an extinction event. The second approach utilizes Markov chains for both sim- ulation and extinction prediction. -
Local Time and Tanaka Formula for G-Brownian Motion
Local time and Tanaka formula for the G-Brownian motion∗ Qian LIN 1,2† 1School of Mathematics, Shandong University, Jinan 250100, China; 2 Laboratoire de Math´ematiques, CNRS UMR 6205, Universit´ede Bretagne Occidentale, 6, avenue Victor Le Gorgeu, CS 93837, 29238 Brest cedex 3, France. Abstract In this paper, we study the notion of local time and obtain the Tanaka formula for the G-Brownian motion. Moreover, the joint continuity of the local time of the G- Brownian motion is obtained and its quadratic variation is proven. As an application, we generalize Itˆo’s formula with respect to the G-Brownian motion to convex functions. Keywords: G-expectation; G-Brownian motion; local time; Tanaka formula; quadratic variation. 1 Introduction The objective of the present paper is to study the local time as well as the Tanaka formula for the G-Brownian motion. Motivated by uncertainty problems, risk measures and superhedging in finance, Peng has introduced a new notion of nonlinear expectation, the so-called G-expectation (see [10], [12], [13], [15], [16]), which is associated with the following nonlinear heat equation 2 ∂u(t,x) ∂ u(t,x) R arXiv:0912.1515v3 [math.PR] 20 Oct 2012 = G( 2 ), (t,x) [0, ) , ∂t ∂x ∈ ∞ × u(0,x)= ϕ(x), where, for given parameters 0 σ σ, the sublinear function G is defined as follows: ≤ ≤ 1 G(α)= (σ2α+ σ2α−), α R. 2 − ∈ The G-expectation represents a special case of general nonlinear expectations Eˆ whose importance stems from the fact that they are related to risk measures ρ in finance by ∗Corresponding address: Institute of Mathematical Economics, Bielefeld University, Postfach 100131, 33501 Bielefeld, Germany †Email address: [email protected] 1 the relation Eˆ[X] = ρ( X), where X runs the class of contingent claims. -
Lecture III: Review of Classic Quadratic Variation Results and Relevance to Statistical Inference in Finance
Lecture III: Review of Classic Quadratic Variation Results and Relevance to Statistical Inference in Finance Christopher P. Calderon Rice University / Numerica Corporation Research Scientist Chris Calderon, PASI, Lecture 3 Outline I Refresher on Some Unique Properties of Brownian Motion II Stochastic Integration and Quadratic Variation of SDEs III Demonstration of How Results Help Understand ”Realized Variation” Discretization Error and Idea Behind “Two Scale Realized Volatility Estimator” Chris Calderon, PASI, Lecture 3 Part I Refresher on Some Unique Properties of Brownian Motion Chris Calderon, PASI, Lecture 3 Outline For Items I & II Draw Heavily from: Protter, P. (2004) Stochastic Integration and Differential Equations, Springer-Verlag, Berlin. Steele, J.M. (2001) Stochastic Calculus and Financial Applications, Springer, New York. For Item III Highlight Results from: Barndorff-Nielsen, O. & Shepard, N. (2003) Bernoulli 9 243-265. Zhang, L.. Mykland, P. & Ait-Sahalia,Y. (2005) JASA 100 1394-1411. Chris Calderon, PASI, Lecture 3 Assuming Some Basic Familiarity with Brownian Motion (B.M.) • Stationary Independent Increments • Increments are Gaussian Bt Bs (0,t s) • Paths are Continuous but “Rough”− / “Jittery”∼ N − (Not Classically Differentiable) • Paths are of Infinite Variation so “Funny” Integrals Used in Stochastic Integration, e.g. t 1 2 BsdBs = 2 (Bt t) 0 − R Chris Calderon, PASI, Lecture 3 Assuming Some Basic Familiarity with Brownian Motion (B.M.) The Material in Parts I and II are “Classic” Fundamental & Established Results but Set the Stage to Understand Basics in Part III. The References Listed at the Beginning Provide a Detailed Mathematical Account of the Material I Summarize Briefly Here. Chris Calderon, PASI, Lecture 3 A Classic Result Worth Reflecting On N 2 lim (Bti Bti 1 ) = T N − →∞ i=1 − T Implies Something Not t = i Intuitive to Many Unfamiliar i N with Brownian Motion … Chris Calderon, PASI, Lecture 3 Discretely Sampled Brownian Motion Paths 2 1.8 Fix Terminal Time, “T” and Refine Mesh by 1.6 Increasing “N”. -
Notes on Brownian Motion II: Introduction to Stochastic Integration
Copyright c 2014 by Karl Sigman 1 IEOR 6712: Notes on Brownian Motion II: Introduction to stochastic integration 1.1 Functions of bounded variation A real-valued function f = f(t) on [0; 1) is said to be of bounded variation if the y−axis distance (e.g., up-down distance) it travels in any finite interval of time is finite. As we shall soon see, the paths of Brownian motion do not have this property leading us to conclude, among other things, that in fact the paths are not differentiable. If f is differentiable, then during an infinitesimal time interval of length dt, near t, the y−axis distance traversed is jdf(t)j = jf 0(t)jdt, R b 0 and so the total distance traveled over an interval [a; b] is a jf (t)jdt, as we know from calculus. To make this precise, consider an interval [a; b] and a partition Π of the interval of the form a = t0 < t1 < ··· < tn = b. Define the variation over [a; b] with respect to Π by n X VΠ(f)[a; b] = jf(tk) − f(tk−1)j: (1) k=1 As the partition gets finer and finer, this quantity approaches the total variation of f over [a; b]: Leting jΠj = max1≤k≤nftk − tk−1g denote the maximum interval length of a partition, the total variation of f over [a; b] is defined by V (f)[a; b] = lim VΠ(f)[a; b]; (2) jΠj!0 If V (f)[a; b] < 1, then f is said to be of bounded variation over [a; b].