Bridging the Gap between Center and Tail for Multiscale Processes

Similar documents
Exact Simulation of Diffusions and Jump Diffusions

Hypoelliptic multiscale Langevin diffusions and Slow fast stochastic reaction diffusion equations.

Dynamical systems with Gaussian and Levy noise: analytical and stochastic approaches

Reaction-Diffusion Equations In Narrow Tubes and Wave Front P

Mathematical Methods for Neurosciences. ENS - Master MVA Paris 6 - Master Maths-Bio ( )

Large Deviations from the Hydrodynamic Limit for a System with Nearest Neighbor Interactions

Theoretical Tutorial Session 2

Discretization of SDEs: Euler Methods and Beyond

Stochastic Viral Dynamics with Beddington-DeAngelis Functional Response

Stochastic Gradient Descent in Continuous Time

Introduction to numerical simulations for Stochastic ODEs

Nonlinear representation, backward SDEs, and application to the Principal-Agent problem

Gillespie s Algorithm and its Approximations. Des Higham Department of Mathematics and Statistics University of Strathclyde

2012 NCTS Workshop on Dynamical Systems

Continuous dependence estimates for the ergodic problem with an application to homogenization

Irreversible Langevin samplers and variance reduction: a large deviations approach

GARCH processes continuous counterparts (Part 2)

Weak convergence and large deviation theory

Intertwinings for Markov processes

HJB equations. Seminar in Stochastic Modelling in Economics and Finance January 10, 2011

On density asymptotics for diffusions, old and new

Large deviations and averaging for systems of slow fast stochastic reaction diffusion equations.

lim n C1/n n := ρ. [f(y) f(x)], y x =1 [f(x) f(y)] [g(x) g(y)]. (x,y) E A E(f, f),

ON THE POLICY IMPROVEMENT ALGORITHM IN CONTINUOUS TIME

arxiv: v2 [math.pr] 12 Sep 2018

DUBLIN CITY UNIVERSITY

A Class of Fractional Stochastic Differential Equations

A random perturbation approach to some stochastic approximation algorithms in optimization.

Paul Dupuis Konstantinos Spiliopoulos Hui Wang

Stability of Stochastic Differential Equations

Least Squares Estimators for Stochastic Differential Equations Driven by Small Lévy Noises

Stochastic optimal control with rough paths

Nonlinear Dynamical Systems Lecture - 01

Multilevel Monte Carlo for Lévy Driven SDEs

Annealed Brownian motion in a heavy tailed Poissonian potential

BSDEs and PDEs with discontinuous coecients Applications to homogenization K. Bahlali, A. Elouain, E. Pardoux. Jena, March 2009

On the fast convergence of random perturbations of the gradient flow.

Multilevel Monte Carlo for Stochastic McKean-Vlasov Equations

Simulation methods for stochastic models in chemistry

Sensitivity analysis of the expected utility maximization problem with respect to model perturbations

Partial Differential Equations, Winter 2015

Importance sampling of rare events using cross-entropy minimization

The concentration of a drug in blood. Exponential decay. Different realizations. Exponential decay with noise. dc(t) dt.

Obstacle problems for nonlocal operators

On continuous time contract theory

Affine Processes. Econometric specifications. Eduardo Rossi. University of Pavia. March 17, 2009

Efficient rare-event simulation for sums of dependent random varia

Homogenization with stochastic differential equations

Math 240 Calculus III

Fractional Laplacian

Convergence of Particle Filtering Method for Nonlinear Estimation of Vortex Dynamics

Introduction to Random Diffusions

Nonparametric Drift Estimation for Stochastic Differential Equations

Path Decomposition of Markov Processes. Götz Kersting. University of Frankfurt/Main

Look-down model and Λ-Wright-Fisher SDE

Approximations of displacement interpolations by entropic interpolations

Convergence to equilibrium for rough differential equations

Linearization problem. The simplest example

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 22 12/09/2013. Skorokhod Mapping Theorem. Reflected Brownian Motion

Short-time expansions for close-to-the-money options under a Lévy jump model with stochastic volatility

Backward Stochastic Differential Equations with Infinite Time Horizon

Walsh Diffusions. Andrey Sarantsev. March 27, University of California, Santa Barbara. Andrey Sarantsev University of Washington, Seattle 1 / 1

Sequential Monte Carlo Methods for Bayesian Computation

Calculating the domain of attraction: Zubov s method and extensions

Optimal transportation and optimal control in a finite horizon framework

Gaussian processes for inference in stochastic differential equations

The Chaotic Character of the Stochastic Heat Equation

Introduction to multiscale modeling and simulation. Almost every system is multiscale.

On the Goodness-of-Fit Tests for Some Continuous Time Processes

Exact Simulation of Multivariate Itô Diffusions

On Stopping Times and Impulse Control with Constraint

1. Numerical Methods for Stochastic Control Problems in Continuous Time (with H. J. Kushner), Second Revised Edition, Springer-Verlag, New York, 2001.

Stochastic differential equations in neuroscience

VARIANCE REDUCTION FOR IRREVERSIBLE LANGEVIN SAMPLERS AND DIFFUSION ON GRAPHS LUC REY-BELLET

l approche des grandes déviations

ODE Homework Solutions of Linear Homogeneous Equations; the Wronskian

Nonlinear Control. Nonlinear Control Lecture # 3 Stability of Equilibrium Points

Simulation of conditional diffusions via forward-reverse stochastic representations

I forgot to mention last time: in the Ito formula for two standard processes, putting

Fast-slow systems with chaotic noise

(1) Recap of Differential Calculus and Integral Calculus (2) Preview of Calculus in three dimensional space (3) Tools for Calculus 3

PH.D. PRELIMINARY EXAMINATION MATHEMATICS

On the Multi-Dimensional Controller and Stopper Games

A MODEL FOR THE LONG-TERM OPTIMAL CAPACITY LEVEL OF AN INVESTMENT PROJECT

Exponential functionals of Lévy processes

18.01 Single Variable Calculus Fall 2006

Partial Differential Equations with Applications to Finance Seminar 1: Proving and applying Dynkin s formula

Improved diffusion Monte Carlo

Proceedings of the 2014 Winter Simulation Conference A. Tolk, S. D. Diallo, I. O. Ryzhov, L. Yilmaz, S. Buckley, and J. A. Miller, eds.

ON THE FIRST TIME THAT AN ITO PROCESS HITS A BARRIER

A class of globally solvable systems of BSDE and applications

UNIVERSITY OF MANITOBA

Introduction to self-similar growth-fragmentations

Formulas that must be memorized:

Schilder theorem for the Brownian motion on the diffeomorphism group of the circle

Effective dynamics for the (overdamped) Langevin equation

Kolmogorov Equations and Markov Processes

Lower Tail Probabilities and Related Problems

Solution of Additional Exercises for Chapter 4

Mean-Field optimization problems and non-anticipative optimal transport. Beatrice Acciaio

Transcription:

Bridging the Gap between Center and Tail for Multiscale Processes Matthew R. Morse Department of Mathematics and Statistics Boston University BU-Keio 2016, August 16 Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 1 / 19

Introduction A multiscale process is characterized by multiple coupled processes which evolve at separated time scales. Event probabilities on the order of greater than one in one thousand are estimated by the Central Limit Theorem. Event probabilities on the order of less than 10 9 are estimated by the Large Deviations Principle. We focus on the Moderate Deviations Principle, which provides estimates for probabilities between these two extremes. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 2 / 19

Outline 1 Examples of Multiscale Processes Molecular Physics 2 Review of Related Work Multiscale Processes Large Deviations Principle 3 Moderate Deviations Principle 4 Future Work Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 3 / 19

Examples of Multiscale Processes Molecular Physics A Model of Protein Folding [Dupuis, et al., 2011] Define X ε (t) The configuration of a protein at time t V ε (x, x/δ) The potential surface of a protein X ε (t) satisfies the Langevin equation ( dx ε (t) = V ε X ε (t), X ε ) (t) dt + ε 2D dw (t), X ε (0) = x 0. δ where 2D is a diffusion constant, W (t) is standard Brownian motion, and δ and ε are small positive parameters. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 4 / 19

Examples of Multiscale Processes Molecular Physics Graph of a Potential Function V(x) -0.5 0.5 1.0 1.5 2.0 2.5 3.0-2 -1 0 1 2 x V ε (x, x δ ) = ε ( cos( x δ ) + sin( x δ )) + 3 2 (x 2 1) 2, ε = 0.1, δ = 0.01. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 5 / 19

Review of Related Work Multiscale Processes Definition of Multiscale Processes Let Xt ε be a n-dimensional process and Yt ε be a k-dimensional process for 0 t 1 which solve the system dx ε t = c(x ε t, Y ε t ) dt + εσ(x ε t, Y ε t ) dw t, X ε 0 = x 0 dy ε t = 1 ε g(x ε t, Y ε t ) dt + 1 ε τ(x ε t, Y ε t ) db t, Y ε 0 = y 0 where the coefficient functions c(x, y), σ(x, y), g(x, y), and τ(x, y) are twice differentiable, and all functions, derivatives, and second derivatives are bounded, W t and B t are independent m-dimensional Brownian motions, and ε is a small positive parameter. Furthermore, assume that lim y g(x, y) y = for all x and that ττ T is uniformly positive definite. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 6 / 19

Review of Related Work Multiscale Processes Law of Large Numbers [Spiliopoulos, 2014] Consider the Y process with the x variable frozen, that is, dỹt = g(x, Ỹt) dt + τ(x, Ỹt) db t, Ỹ 0 = y 0, where x R n is a fixed parameter. This is associated with the operator L x defined by L x F (y) = F (y)g(x, y) + 1 2 ττt (x, y) : F (y) and the invariant measure µ x (dy). Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 7 / 19

Review of Related Work Multiscale Processes Law of Large Numbers (cont.) Define the averaged drift c(x) = Y c(x, y)µ x (dy) and the averaged process X as the solution to d X t = c( X t ) dt, X0 = x 0. Then as ε 0, X ε t X t in probability. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 8 / 19

Review of Related Work Multiscale Processes Central Limit Theorem Central Limit Theorem As ε 0, 1 ε (X ε t X t ) η t in distribution, where η t is a single scale stochastic process. This is used to estimate probabilities for X ε near the center of the distribution. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 9 / 19

Review of Related Work Large Deviations Principle Definition of Large Deviations Let X ε, ε > 0, be a family of random variables parameterized by ε. X ε satisfies a large deviations principle with rate function I if for every closed set F, lim sup ε log P{X ε F } inf I (x) ε 0 x F and for every open set G, lim inf ε 0 ε log P{X ε G} inf x G I (x). If a family of random variables satisfies a large deviations principle with some rate function, that rate function is unique. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 10 / 19

Review of Related Work Large Deviations Principle The Laplace Principle [Dupuis and Ellis, 1997] The family X ε, ε > 0, satisfies a Laplace principle with rate function I if for every bounded continuous function a, lim ε log E{exp[ 1 ε 0 ε a(x ε )]} = inf{i (x) + a(x)}. x The Laplace principle and the large deviations principle are equivalent. The large deviations principle (or Laplace principle) is used to estimate probabilities in the tail of the distribution. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 11 / 19

Moderate Deviations Principle Definition of Moderate Deviations Let h(ε) be a function such that as ε 0, h(ε) and εh(ε) 0. Consider ηt ε 1 = (X ε εh(ε) t X t ). A family of stochastic processes X ε satisfies a moderate deviations principle with rate function I if for every bounded continuous function a, 1 lim ε 0 h 2 (ε) log E{exp[ h2 (ε)a(η ε )]} = inf{i (x) + a(x)}. x Previous results by [Guillin, 2003] and others. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 12 / 19

Moderate Deviations Principle Poisson Equation Define Φ(x, y) as the unique solution to L x Φ(x, y) = (c(x, y) c(x)), Y Φ(x, y)µ x (dy) = 0. (Existence and uniqueness due to [Pardoux and Veretennikov, 2003].) Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 13 / 19

Moderate Deviations Principle Statement of Theorem Theorem Let X ε and Y ε as previously defined be a multiscale process. Then X ε satisfies a moderate deviations principle with rate function I (φ) = 1 2 1 0 ( φ s r( X s, φ s )) T q 1 ( X s )( φ s r( X s, φ s ))ds if φ C([0, 1]; R n ) is absolutely continuous, and I (φ) = otherwise, where r(x, η) = c(x)η and q(x) = Y [ ] σσ T (x, y) + [ y Φτ] [ y Φτ] T (x, y) µ x (dy). Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 14 / 19

Moderate Deviations Principle Sketch of Proof The starting point for the proof is a stochastic control representation which follows from [Boué and Dupuis, 1998], which yields 1 h 2 (ε) log E [ exp{ h 2 (ε)a(η ε )} ] [ 1 1 ] = inf E u ε (s) 2 ds + a(η ε,uε ) u ε 2 where u ε is a stochastic control and η ε,uε 0 is a controlled process. Then, 1 Prove that (u ε, η ε,uε ) converges in distribution as ε 0. 2 Define the rate function I in terms of the limit of the control u ε, and prove the Laplace principle lower bound, lim inf ε 0 1 h 2 (ε) log E [ exp { h 2 (ε)a(η ε ) }] inf [I (φ) + a(φ)]. φ 3 Rewrite the rate function in the form given in the theorem statement, and use this to prove the Laplace principle upper bound, lim sup 1 ε 0 h 2 (ε) log E [ exp { h 2 (ε)a(η ε ) }] inf [I (φ) + a(φ)]. φ Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 15 / 19

Future Work Future Work 1 Importance sampling schemes for accelerated Monte Carlo simulation based on the stochastic control representation. 2 Statistical inference for multiscale processes. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 16 / 19

The End Thank You Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 17 / 19

Bibliography Bibliography I M. Boué and P. Dupuis, A Variational Representation for Certain Functionals of Brownian Motion, The Annals of Probability, Vol. 26, No. 4 (1998), pp. 1641 1659. P. Dupuis and R.S. Ellis, A Weak Convergence Approach to the Theory of Large Deviations, John Wiley & Sons, New York, 1997. P. Dupuis, K. Spiliopoulos, and H. Wang, Rare Event Simulation for Rough Energy Landscapes, Proceedings of the 2011 Winter Simulation Conference. A. Guillin, Averaging Principle of SDE with Small Diffusion: Moderate Deviations, The Annals of Probability, Vol. 31, No. 1 (2003), pp. 413 443. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 18 / 19

Bibliography Bibliography II E. Pardoux and A.Yu. Veretennikov, On Poisson Equation and Diffusion Approximation 2, The Annals of Probability, Vol. 31, No. 3 (2003), pp. 1166 1192. K. Spiliopoulos, Fluctuation Analysis and Short Time Asymptotics for Multiple Scales Diffusion Processes, Stochastics and Dynamics, Vol. 14, No. 3, (2014), pp. 1350026. Matthew R. Morse (BU) Moderate Deviations for Multiple Scales BU-Keio 2016, August 16 19 / 19