Brownian Motion and Stochastic Calculus

Similar documents
MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 7 9/25/2013

Iowa State University. Instructor: Alex Roitershtein Summer Homework #5. Solutions

Lecture 21 Representations of Martingales

d(x n, x) d(x n, x nk ) + d(x nk, x) where we chose any fixed k > N

Problem set 5, Real Analysis I, Spring, otherwise. (a) Verify that f is integrable. Solution: Compute since f is even, 1 x (log 1/ x ) 2 dx 1

Conditional Distributions

Brownian Motion. 1 Definition Brownian Motion Wiener measure... 3

1 Independent increments

Lecture 17 Brownian motion as a Markov process

PROBABILITY: LIMIT THEOREMS II, SPRING HOMEWORK PROBLEMS

Math 163 (23) - Midterm Test 1

Problem Sheet 1. You may assume that both F and F are σ-fields. (a) Show that F F is not a σ-field. (b) Let X : Ω R be defined by 1 if n = 1

MATH 6605: SUMMARY LECTURE NOTES

Verona Course April Lecture 1. Review of probability

1/12/05: sec 3.1 and my article: How good is the Lebesgue measure?, Math. Intelligencer 11(2) (1989),

On the martingales obtained by an extension due to Saisho, Tanemura and Yor of Pitman s theorem

Solutions to the Exercises in Stochastic Analysis

A D VA N C E D P R O B A B I L - I T Y

converges as well if x < 1. 1 x n x n 1 1 = 2 a nx n

Exercises Measure Theoretic Probability

1 Stat 605. Homework I. Due Feb. 1, 2011

Math 140A - Fall Final Exam

HOMEWORK ASSIGNMENT 6

17. Convergence of Random Variables

Part II Probability and Measure

Assignment-10. (Due 11/21) Solution: Any continuous function on a compact set is uniformly continuous.

PROBABILITY: LIMIT THEOREMS II, SPRING HOMEWORK PROBLEMS

Useful Probability Theorems

{σ x >t}p x. (σ x >t)=e at.

LECTURE 2: LOCAL TIME FOR BROWNIAN MOTION

Lecture 5. If we interpret the index n 0 as time, then a Markov chain simply requires that the future depends only on the present and not on the past.

Hardy-Stein identity and Square functions

Selected Exercises on Expectations and Some Probability Inequalities

Kolmogorov Equations and Markov Processes

On the quantiles of the Brownian motion and their hitting times.

(A n + B n + 1) A n + B n

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),

Austin Mohr Math 704 Homework 6

Lecture 4 Lebesgue spaces and inequalities

Brownian motion. Samy Tindel. Purdue University. Probability Theory 2 - MA 539

MATH 202B - Problem Set 5

ADVANCED PROBABILITY: SOLUTIONS TO SHEET 1

Real Analysis Math 131AH Rudin, Chapter #1. Dominique Abdi

4. We accept without proofs that the following functions are differentiable: (e x ) = e x, sin x = cos x, cos x = sin x, log (x) = 1 sin x

MAT 571 REAL ANALYSIS II LECTURE NOTES. Contents. 2. Product measures Iterated integrals Complete products Differentiation 17

Lecture 12. F o s, (1.1) F t := s>t

Jump Processes. Richard F. Bass

n E(X t T n = lim X s Tn = X s

Math 127C, Spring 2006 Final Exam Solutions. x 2 ), g(y 1, y 2 ) = ( y 1 y 2, y1 2 + y2) 2. (g f) (0) = g (f(0))f (0).

MA8109 Stochastic Processes in Systems Theory Autumn 2013

Applications of Ito s Formula

Math 5051 Measure Theory and Functional Analysis I Homework Assignment 2

h(x) lim H(x) = lim Since h is nondecreasing then h(x) 0 for all x, and if h is discontinuous at a point x then H(x) > 0. Denote

Question 1. The correct answers are: (a) (2) (b) (1) (c) (2) (d) (3) (e) (2) (f) (1) (g) (2) (h) (1)

Part III Stochastic Calculus and Applications

MATH 104: INTRODUCTORY ANALYSIS SPRING 2008/09 PROBLEM SET 8 SOLUTIONS

STOCHASTIC CALCULUS JASON MILLER AND VITTORIA SILVESTRI

u( x) = g( y) ds y ( 1 ) U solves u = 0 in U; u = 0 on U. ( 3)

Solutions Final Exam May. 14, 2014

4th Preparation Sheet - Solutions

MATH 409 Advanced Calculus I Lecture 10: Continuity. Properties of continuous functions.

Part III Advanced Probability

Filtrations, Markov Processes and Martingales. Lectures on Lévy Processes and Stochastic Calculus, Braunschweig, Lecture 3: The Lévy-Itô Decomposition

Feller Processes and Semigroups

Problem set 1, Real Analysis I, Spring, 2015.

Weak convergence. Amsterdam, 13 November Leiden University. Limit theorems. Shota Gugushvili. Generalities. Criteria

Nash Type Inequalities for Fractional Powers of Non-Negative Self-adjoint Operators. ( Wroclaw 2006) P.Maheux (Orléans. France)

OPTIMAL STOPPING OF A BROWNIAN BRIDGE

Continuity. Chapter 4

Wiener Measure and Brownian Motion

Theory of PDE Homework 2

Lecture 3. Econ August 12

Continuity. Chapter 4

An essay on the general theory of stochastic processes

MAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9

Midterm 1. Every element of the set of functions is continuous

Exercises. T 2T. e ita φ(t)dt.

Stochastic integration. P.J.C. Spreij

MATH 56A SPRING 2008 STOCHASTIC PROCESSES 197

Carefully tear this page off the rest of your exam. UNIVERSITY OF TORONTO SCARBOROUGH MATA37H3 : Calculus for Mathematical Sciences II

Probability Theory. Richard F. Bass

Exercises Measure Theoretic Probability

1 Solution to Problem 2.1

Brownian Motion and Conditional Probability

HOMEWORK ASSIGNMENT 5

Economics 204 Fall 2011 Problem Set 2 Suggested Solutions

MATH 425, FINAL EXAM SOLUTIONS

An idea how to solve some of the problems. diverges the same must hold for the original series. T 1 p T 1 p + 1 p 1 = 1. dt = lim

MATH 5616H INTRODUCTION TO ANALYSIS II SAMPLE FINAL EXAM: SOLUTIONS

MATH34032 Mid-term Test 10.00am 10.50am, 26th March 2010 Answer all six question [20% of the total mark for this course]

BEST TESTS. Abstract. We will discuss the Neymann-Pearson theorem and certain best test where the power function is optimized.

REAL ANALYSIS I HOMEWORK 4

Advanced Calculus I Chapter 2 & 3 Homework Solutions October 30, Prove that f has a limit at 2 and x + 2 find it. f(x) = 2x2 + 3x 2 x + 2

Brownian Motion. Chapter Definition of Brownian motion

Laplace s Equation. Chapter Mean Value Formulas

Math 328 Course Notes

A Barrier Version of the Russian Option

Backward Stochastic Differential Equations with Infinite Time Horizon

Lecture Notes on Metric Spaces

Ch3 Operations on one random variable-expectation

Transcription:

ETHZ, Spring 17 D-MATH Prof Dr Martin Larsson Coordinator A Sepúlveda Brownian Motion and Stochastic Calculus Exercise sheet 6 Please hand in your solutions during exercise class or in your assistant s box in HG E65 no latter than April 7th Exercise 61 Let (B t t be a Brownian motion and define the process (M t t by M t sup s t B s Show that for any fixed t Law M t B t B t Law M t (1 That is, show that the random variables have the same density functions Solution 61 For any g : R R bounded Borel measurable function, we know that E g( B t 1 g( x e x /(t dx g(x πt πt e x /(t dx ( Thus, we see that the probability density function of B t on R is given by the function x 1 x πt e x /(t From Corollary 55 of the script, we know that the probability density function of the joint law of (B t, M t where M t : sup s t B s is given by the function (x, y (y x πt 3 e (y x /(t 1 {y, x y} (3 Take any g : R R bounded Borel measurable function We deduce from (3 that E g(m t B t (y x g(y x e (y x /(t dx dy πt 3 y, y x By a change of variable u : y x v : y we get that E g(m t B t g(u (u + v e (u+v /(t du dv (4 πt3 u, v By another change of variable n : u and m : u + v and as x e cx / dx e cx / c, we get that E g(m t B t g(n πt 3 m e m /(t dm dn n g(n πt e n /(t dn (5 Law Comparing ( with (5 yields that M t B t B t Now, from (3, we deduce for any g : R R bounded Borel measurable function that E g(m t y, y x g(y (y x πt 3 e (y x /(t dx dy Updated: March 8, 17 1 / 7

Brownian Motion and Stochastic Calculus, Spring 17 By a change of variable u : y and v : y x we get that E g(m t g(u (u + v e (u+v /(t du dv (6 πt3 u, v Comparing (4 with (6 yields M t B t Law M t Updated: March 8, 17 / 7

Brownian Motion and Stochastic Calculus, Spring 17 Exercise 6 Let (B t t be a Brownian motion and denote by G t : σ(b u, u t, t Define R f(x f(x and R t f(x 1 f(y exp ( 1t (y πt x + exp ( 1t (y + x dy, t > Let us consider the process (X t t by X t : B t Show that E f(x t+h G t Rh f(x t P -as for f bb(r and t, h Solution 6 Fix any t, h and f bb(r The case where h is trivial, therefore, let h > From the lecture (cf Example 3 in Section 3 in the lecture notes, we know that Brownian motion is a Markov process with transition semigroup given by R f(x f(x and 1 R h f(x πh Therefore, we get for f(x : f( x bb(r that R E f(x t+h Gt Rh f(bt 1 πh (y x f(y exp ( dy when h >, f bb(r h 1 πh R f(y exp ( (y B t dy h f(y exp ( (y B t dy h f( y exp ( (y B t dy (7 h, + 1 πh (, By a change of variables and by observing that {} is a null set, we deduce from (7 that E f(x t+h 1 Gt f(y exp ( (y B t dy πh, h + 1 f(y exp ( (y + B t dy (8 πh h R h f(b t, By symmetry of the expression in (8, we see that E f(x t+h Gt Rh f( B t and thus E f(x t+h Gt Rh f(x t Updated: March 8, 17 3 / 7

Brownian Motion and Stochastic Calculus, Spring 17 Exercise 63 Let (B t t be a Brownian motion For any a > consider the stopping times T a : inf { t > Bt a }, Show that the Laplace transform of T a has value: E exp( µt a exp ( a µ, µ > and show that P T a < 1 Hint: Consider the martingale M λ t ( exp λb t λ t Solution 63 We know that for any λ R, the process M λ : (M λ t t defined by M λ t exp (λb t λ t is a continuous F t -martingale, where we denote by (F t t the filtration generated by B Moreover, for any n N, T a n is a bounded stopping time Thus, applying the stopping theorem (ie Serie 6 Exercise 1 we get E F M λ 1 P -as By taking expectations, we get that M λ T a n Now, on the event {T a < } we have exp (λb Ta n λ (T a n E MT λ a n 1 ( n exp (λb Ta λ T a e λa exp λ T a On the event {T a } we have B t a for any t and thus we get for any λ > that exp (λb Ta n λ (T a n exp (λb n λ n n We conclude that for any λ > exp (λb Ta n λ (T a n Observe that for any n N we have exp ( n e λa exp λ T a 1 {Ta< } P -as (9 (λb Ta n λ (T a n e λa Thus, we deduce from (9, by applying dominated convergence theorem, that for any λ > 1 E ( MT λ n a n e λa E exp λ T a 1 {Ta< } and so, for any λ > ( e λa E exp λ T a 1 {Ta< } 1 (1 Take any positive, decreasing sequence (λ n n N converging to We deduce from (1 and the monotone convergence theorem that P T a < ( lim n eλna E exp λ n T a 1 {Ta< } 1 Updated: March 8, 17 4 / 7

Brownian Motion and Stochastic Calculus, Spring 17 which proves the first part Thus, as we now know that P T a < 1 we get from (1 that for any λ > ( e λa E exp λ T a 1 (11 Fix any µ > For λ : µ, (11 yields the desired result Updated: March 8, 17 5 / 7

Brownian Motion and Stochastic Calculus, Spring 17 Exercise 64 Let (F n n N be a decreasing sequence of sub-σ-fields of F (ie F n+1 F n F, n N and let (X n n N be a backward submartingale, ie E X n <, X n is F n -measurable and EX n F n+1 X n+1 P -as for every n N (a Show that for any n m, N, M >, E X n 1 { Xn M} E Xm E N M E Xn (b Show that lim n EX n > implies that the sequence (X n n N is uniformly integrable Hint: use a to conclude that (X n n N is uniformly integrable Solution 64 (a For any n m, N, M >, by the backward submartingale property, using that the set { X n > M} F n, we obtain that E X n 1 { Xn M} E Xn E Xn 1 { Xn<M} E X n E Xm 1 { Xn<M} E X n E Xm + E Xm 1 { Xn M} E X m X n + E Xm 1 { Xn M, X m N} + E X m 1 { Xn M,< X m<n} + E Xm 1 { Xn M, X m } E X m X n + E Xm 1 { Xn M, X m N} + E Xm 1 { Xn M,< X m<n} E X m E N M E X n 1 { Xn M} E X m E N M E X n 1 { Xn } E X m E N M E Xn (b First, as (X n n N is a backward submartingale, we obtain that for any n X + n X n + X n EX F n + X n Thus, as (EX F n n N is uniformly integrable, if we can show that (X n n N is uniformly integrable, we can conclude that also (X + n n N is uniformly integrable which then implies that (X n n N is uniformly integrable Now, (X n n N being uniformly integrable is equivalent having that for any ε > we find M such that sup E X n 1 { Xn M} ε n N Fix any ε > Due to the assumption that lim n EX n >, we can find m N such that for any n m EX m EX n ε/4 Since X n is integrable for every n N we can find M m such that for any M M m max E X n 1 { Xn M} ε/4 n<m As sup E X n 1 { Xn M} max E X n 1 { Xn M} + sup E X n 1 { Xn M} n N n<m n m Updated: March 8, 17 6 / 7

Brownian Motion and Stochastic Calculus, Spring 17 it suffices to find M M m such that sup E X n 1 { Xn M} 3ε/4 n m We first observe that (X n + n N is also a backward submartingale Indeed, due to Jensen s inequality, we obtain that E X n + F n+1 EXn F n+1 + X n+1 + Now, we claim that sup n N EX n < Assume by contradiction that sup n N EX n Then, we can find a subsequence (n k k N such that lim k EX n k sup EXn Using that (X + n n N is also a backward submartingale, we obtain for any k that n N E X n k E X + nk E Xnk E X + E Xnk E X E X nk But as X is integrable and as lim k E X nk > by assumption, we obtain that lim k EX n k E X lim k E X nk < which gives us a contradiction Thus we have proved that sup u N EXu < For any n m, N, M >, by a, by the choice of m and as sup k N EX k <, we obtain that E X n 1 { Xn M} E Xm E N ε/4 + E N X m 1 { Xm N} + M E Xn ε/4 + E N X m 1 { Xm N} + M sup u N E Xu M E Xn Since X u is integrable for any u N we can find N big enough such that second term above is smaller than ε/4 After having chosen N we can find M M m such that that the last term above is smaller than ε/4 Thus, we get for that chosen M that hence we get the result sup E X n 1 { Xn M} 3ε/4 n m Updated: March 8, 17 7 / 7