Exercise 4. An optional time which is not a stopping time
|
|
- Richard Lambert
- 5 years ago
- Views:
Transcription
1 M5MF6, EXERCICE SET 1 We shall here consider a gien filtered probability space Ω, F, P, spporting a standard rownian motion W t t, with natral filtration F t t. Exercise 1 Proe Proposition 1.1.3, Theorem 1..9, and the examples/exercises in the lectre notes in Sections Answer of exercise 1 See the lectre notes. Exercise An optional time which is not a stopping time Consider the filtration G t t and the random time τ defined by { { {, Ω}, if t 1, 1, if ω, G t : and τ : Ω, if t > 1., if ω /, where is some non-triial sbset of Ω. Show that τ is a G-optional time, bt not a G-stopping time. Exercise 3 Gassian integral Define the process X t t pathwise by X t : φ sd, where φ is a deterministic fnction path. Proe that X is a Gassian process with mean zero and coariance strctre EX s X t s t φ sds. Answer of exercise 3 We first proe that, for any t, X t is a Gassian random ariable with mean zero and ariance φ sds. Itô s lemma yields.1 E e X t φ se e X s ds, for any real nmber. For any sch, define ψ t : E e Xt, so that differentiating both sides of.1 implies t ψ t 1 φ t ψ t, 1 which is easily soled as ψ t exp t φ sds. This proes the claim. The proof of the coariance strctre follows the same steps. Exercise 4 Pinned rownian motion Find a orel fnction ϕ sch that E W t ϕw t, for any s t. Date: Janary 3, 16. 1
2 M5MF6, EXERCICE SET 1 Answer of exercise 4 Fix s < t. We are looking here for a orel fnction ϕ sch that E W t ϕw t ; we can write this eqialently, for any orel sbset R, as dp t dx φxp t dx φxp t, xdx, where P t is the law of the rownian motion at time t, and p t the Gassian density at time t; frthermore, P t dx xp s, xp t s x, ydx dy R pt;, y R sy t p t, ydy. Taking the fnction φy sy/t concldes the proof. sy xp st s/t t, x dx dy Exercise 5 Spremm of rownian motion and Qadratic ariation Let M be a continos local martingale starting at the origin. Then, for all x, >, P sp M t > x, M exp x. t Hint: Fix some x >, and let τ : inf{t : M t x} be the first hitting time of the leel x. For any α R, introdce the process Z t t defined pathwise by Z t : exp αmt τ 1 α M τ t. Use then the optional sampling theorem: a martingale stopped at a stopping time remains a martingale. Answer of exercise 5 Fix some x >, and let τ : inf{t : M t x} be the first hitting time of the leel x. For any α R, introdce the process Z t t defined pathwise by Z t : exp αmt τ 1 α M τ t. Clearly, Z is a continos local martingale by Itô s formla, and satisfies the ineqality Z t expαx almost srely for all t. When α 1, Z is sally called the stochastic exponential of M, and is denoted by EM. It is therefore sqare integrable, and the optional sampling theorem implies EZ EZ 1. Marko s ineqality frther yields, for any >, P sp M t > x, M t P Z exp αx 1 α exp αx + 1 α. Since α is taken randomly, one can optimise oer it, and the maximm on the right-hand side is clearly attained at α x/, from which the reslt follows. Exercise 6 Martingale Representation Theorem will be coered on 5/1/16
3 M5MF6, EXERCICE SET 1 3 Write down the explicit form of the martingale representation theorem for the process M t t defined as i M t ds; ii M t W t ; iii M t W s ds; i M t sinw t ; M t expw t. Answer of exercise 6 i Clearly, M t d; ii Integration by parts immediately gies M t t sd; iii Itô s formla yields M t t + d EM t + d ; i Itô s formla applied to the fnction f : W, t tw yields so that M t tw t W s ds tw t Itô s formla yields t sinw t exp cosw exp t t + 1 t + dw + 1 cosw exp dw. W s ds + s d + sds s d d sd W, W s s d 1 t t s d EM t + Since EM t is clearly nll, the representation follows. sinw exp d 1 t s d sinw exp d W, W i Hint: apply Itô s formla to the fnction t, W t e Wt ft, for some smooth fnction f : [, R. Exercise 7 Martingale Representation Theorem will be coered on 5/1/16 Define the process M by M t : EW 3 T F t, for any t [, T ]. Proe that M t 3 T s + W s dws. Answer of exercise 7 M t E t W 3 T E t [W T W t +W t 3 ] E t [W T W t 3 ]+W 3 t +3W t E t [W T W t ]+3W t E t [W T W t ] W 3 t +3T tw t Applying Itô s lemma then yields dm t 3 W t + T t dw t,
4 4 M5MF6, EXERCICE SET 1 which concldes the proof. Exercise 8 t Proe that the process Y : W d is Gassian, and compte its expectation and ariance. t Answer of exercise 8 The integration is defined pathwise as a Riemann integral since the integrand is continos. Since W is Gassian, for any t, the random ariable Y t is clearly Gassian as limit of Riemann sms, and so is the process Y. Clearly EY t, and, for any s t, s E Y s Y t E W d W d s dd s 6 3t s. Consider the process Y defined, for all t, by Exercise 9 Y t : W t W d. Proe that Y is Gassian, and compte its expectation and ariance. Show that it is not an F t -martingale. Answer of exercise 9 The process Y is the sm of two Gassian, bt these are not independent. Howeer, the integral is a Gassian process by definition of sms in L of Riemannn integrals. Clearly ey t and, for any s, t, { } EY s Y t E W t d W d s W t { EW t E W t d W t E d } + E d W d s s t s t s E W t W d t d E W d + s d + s s EW W dd dd s t, which proes that the Gassian process Z is a rownian motion. Howeer, for any s < t, E Z t Z s Fs W t E W t d W W s d t F s W W d, which is clearly non zero almost srely. s Exercise 1 Clark-Ocone Formla Let f be a bonded C 1 fnction on R. Proe that there exists a fnction g : [, 1] R R sch that E fw 1 F t gt, W t, for any t [.1],
5 M5MF6, EXERCICE SET 1 5 and write down an Itô formla for g. Proe finally that the following eqality holds for all t [, 1]: gt, W t EfW 1 + Answer of exercise 1 E f W 1 F s d. It is easy to see that [ ] E fw 1 F t E fw 1 W t + W t F t E f Ŵ1 t + W t Ft gt, W t, where the fnction g is defined as gt, x E fx + Ŵ1 t F t. Note that the process gt, W t t [,1] is clearly a martingale, and hence gt, W t EfW 1 + and the reslt follows. x gs, d EfW 1 + ] E [f + Ŵ1 s F s d, Department of Mathematics, Imperial College London address: a.jacqier@imperial.ac.k
1. Stochastic Processes and filtrations
1. Stochastic Processes and 1. Stoch. pr., A stochastic process (X t ) t T is a collection of random variables on (Ω, F) with values in a measurable space (S, S), i.e., for all t, In our case X t : Ω S
More informationThe Wiener Itô Chaos Expansion
1 The Wiener Itô Chaos Expansion The celebrated Wiener Itô chaos expansion is fundamental in stochastic analysis. In particular, it plays a crucial role in the Malliavin calculus as it is presented in
More informationThe Brauer Manin obstruction
The Braer Manin obstrction Martin Bright 17 April 2008 1 Definitions Let X be a smooth, geometrically irredcible ariety oer a field k. Recall that the defining property of an Azmaya algebra A is that,
More informationApplications of Ito s Formula
CHAPTER 4 Applications of Ito s Formula In this chapter, we discuss several basic theorems in stochastic analysis. Their proofs are good examples of applications of Itô s formula. 1. Lévy s martingale
More informationThe concentration of a drug in blood. Exponential decay. Different realizations. Exponential decay with noise. dc(t) dt.
The concentration of a drug in blood Exponential decay C12 concentration 2 4 6 8 1 C12 concentration 2 4 6 8 1 dc(t) dt = µc(t) C(t) = C()e µt 2 4 6 8 1 12 time in minutes 2 4 6 8 1 12 time in minutes
More informationL 1 -smoothing for the Ornstein-Uhlenbeck semigroup
L -smoothing for the Ornstein-Uhlenbeck semigrop K. Ball, F. Barthe, W. Bednorz, K. Oleszkiewicz and P. Wolff September, 00 Abstract Given a probability density, we estimate the rate of decay of the measre
More informationExercises. T 2T. e ita φ(t)dt.
Exercises. Set #. Construct an example of a sequence of probability measures P n on R which converge weakly to a probability measure P but so that the first moments m,n = xdp n do not converge to m = xdp.
More informationVerona Course April Lecture 1. Review of probability
Verona Course April 215. Lecture 1. Review of probability Viorel Barbu Al.I. Cuza University of Iaşi and the Romanian Academy A probability space is a triple (Ω, F, P) where Ω is an abstract set, F is
More informationI forgot to mention last time: in the Ito formula for two standard processes, putting
I forgot to mention last time: in the Ito formula for two standard processes, putting dx t = a t dt + b t db t dy t = α t dt + β t db t, and taking f(x, y = xy, one has f x = y, f y = x, and f xx = f yy
More informationMATH2715: Statistical Methods
MATH275: Statistical Methods Exercises III (based on lectres 5-6, work week 4, hand in lectre Mon 23 Oct) ALL qestions cont towards the continos assessment for this modle. Q. If X has a niform distribtion
More informationRemarks on strongly convex stochastic processes
Aeqat. Math. 86 (01), 91 98 c The Athor(s) 01. This article is pblished with open access at Springerlink.com 0001-9054/1/010091-8 pblished online November 7, 01 DOI 10.1007/s00010-01-016-9 Aeqationes Mathematicae
More informationSolution for Problem 7.1. We argue by contradiction. If the limit were not infinite, then since τ M (ω) is nondecreasing we would have
362 Problem Hints and Solutions sup g n (ω, t) g(ω, t) sup g(ω, s) g(ω, t) µ n (ω). t T s,t: s t 1/n By the uniform continuity of t g(ω, t) on [, T], one has for each ω that µ n (ω) as n. Two applications
More informationPROBABILITY: LIMIT THEOREMS II, SPRING HOMEWORK PROBLEMS
PROBABILITY: LIMIT THEOREMS II, SPRING 15. HOMEWORK PROBLEMS PROF. YURI BAKHTIN Instructions. You are allowed to work on solutions in groups, but you are required to write up solutions on your own. Please
More informationVectors in Rn un. This definition of norm is an extension of the Pythagorean Theorem. Consider the vector u = (5, 8) in R 2
MATH 307 Vectors in Rn Dr. Neal, WKU Matrices of dimension 1 n can be thoght of as coordinates, or ectors, in n- dimensional space R n. We can perform special calclations on these ectors. In particlar,
More informationSolutions to the Exercises in Stochastic Analysis
Solutions to the Exercises in Stochastic Analysis Lecturer: Xue-Mei Li 1 Problem Sheet 1 In these solution I avoid using conditional expectations. But do try to give alternative proofs once we learnt conditional
More informationn E(X t T n = lim X s Tn = X s
Stochastic Calculus Example sheet - Lent 15 Michael Tehranchi Problem 1. Let X be a local martingale. Prove that X is a uniformly integrable martingale if and only X is of class D. Solution 1. If If direction:
More informationSpring, 2008 CIS 610. Advanced Geometric Methods in Computer Science Jean Gallier Homework 1, Corrected Version
Spring, 008 CIS 610 Adanced Geometric Methods in Compter Science Jean Gallier Homework 1, Corrected Version Febrary 18, 008; De March 5, 008 A problems are for practice only, and shold not be trned in.
More informationPart II. Martingale measres and their constrctions 1. The \First" and the \Second" fndamental theorems show clearly how \mar tingale measres" are impo
Albert N. Shiryaev (Stelov Mathematical Institte and Moscow State University) ESSENTIALS of the ARBITRAGE THEORY Part I. Basic notions and theorems of the \Arbitrage Theory" Part II. Martingale measres
More information1 The space of linear transformations from R n to R m :
Math 540 Spring 20 Notes #4 Higher deriaties, Taylor s theorem The space of linear transformations from R n to R m We hae discssed linear transformations mapping R n to R m We can add sch linear transformations
More informationLecture 21 Representations of Martingales
Lecture 21: Representations of Martingales 1 of 11 Course: Theory of Probability II Term: Spring 215 Instructor: Gordan Zitkovic Lecture 21 Representations of Martingales Right-continuous inverses Let
More informationStochastic Integration and Continuous Time Models
Chapter 3 Stochastic Integration and Continuous Time Models 3.1 Brownian Motion The single most important continuous time process in the construction of financial models is the Brownian motion process.
More informationThe Cameron-Martin-Girsanov (CMG) Theorem
The Cameron-Martin-Girsanov (CMG) Theorem There are many versions of the CMG Theorem. In some sense, there are many CMG Theorems. The first version appeared in ] in 944. Here we present a standard version,
More informationRestricted cycle factors and arc-decompositions of digraphs. J. Bang-Jensen and C. J. Casselgren
Restricted cycle factors and arc-decompositions of digraphs J. Bang-Jensen and C. J. Casselgren REPORT No. 0, 0/04, spring ISSN 0-467X ISRN IML-R- -0-/4- -SE+spring Restricted cycle factors and arc-decompositions
More informationMath 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation:
Math 263 Assignment #3 Soltions 1. A fnction z f(x, ) is called harmonic if it satisfies Laplace s eqation: 2 + 2 z 2 0 Determine whether or not the following are harmonic. (a) z x 2 + 2. We se the one-variable
More informationMixed Type Second-order Duality for a Nondifferentiable Continuous Programming Problem
heoretical Mathematics & Applications, vol.3, no.1, 13, 13-144 SSN: 179-9687 (print), 179-979 (online) Scienpress Ltd, 13 Mied ype Second-order Dality for a Nondifferentiable Continos Programming Problem.
More informationPROBABILITY: LIMIT THEOREMS II, SPRING HOMEWORK PROBLEMS
PROBABILITY: LIMIT THEOREMS II, SPRING 218. HOMEWORK PROBLEMS PROF. YURI BAKHTIN Instructions. You are allowed to work on solutions in groups, but you are required to write up solutions on your own. Please
More informationThe multidimensional Ito Integral and the multidimensional Ito Formula. Eric Mu ller June 1, 2015 Seminar on Stochastic Geometry and its applications
The multidimensional Ito Integral and the multidimensional Ito Formula Eric Mu ller June 1, 215 Seminar on Stochastic Geometry and its applications page 2 Seminar on Stochastic Geometry and its applications
More informationON THE PERFORMANCE OF LOW
Monografías Matemáticas García de Galdeano, 77 86 (6) ON THE PERFORMANCE OF LOW STORAGE ADDITIVE RUNGE-KUTTA METHODS Inmaclada Higeras and Teo Roldán Abstract. Gien a differential system that inoles terms
More informationGraphs and Networks Lecture 5. PageRank. Lecturer: Daniel A. Spielman September 20, 2007
Graphs and Networks Lectre 5 PageRank Lectrer: Daniel A. Spielman September 20, 2007 5.1 Intro to PageRank PageRank, the algorithm reportedly sed by Google, assigns a nmerical rank to eery web page. More
More informationDigital Image Processing. Lecture 8 (Enhancement in the Frequency domain) Bu-Ali Sina University Computer Engineering Dep.
Digital Image Processing Lectre 8 Enhancement in the Freqenc domain B-Ali Sina Uniersit Compter Engineering Dep. Fall 009 Image Enhancement In The Freqenc Domain Otline Jean Baptiste Joseph Forier The
More informationA Concise Course on Stochastic Partial Differential Equations
A Concise Course on Stochastic Partial Differential Equations Michael Röckner Reference: C. Prevot, M. Röckner: Springer LN in Math. 1905, Berlin (2007) And see the references therein for the original
More informationStochastic Processes II/ Wahrscheinlichkeitstheorie III. Lecture Notes
BMS Basic Course Stochastic Processes II/ Wahrscheinlichkeitstheorie III Michael Scheutzow Lecture Notes Technische Universität Berlin Sommersemester 218 preliminary version October 12th 218 Contents
More informationFormulas for stopped diffusion processes with stopping times based on drawdowns and drawups
Stochastic Processes and their Applications 119 (009) 563 578 www.elsevier.com/locate/spa Formlas for stopped diffsion processes with stopping times based on drawdowns and drawps Libor Pospisil, Jan Vecer,
More informationQuestion 1. The correct answers are: (a) (2) (b) (1) (c) (2) (d) (3) (e) (2) (f) (1) (g) (2) (h) (1)
Question 1 The correct answers are: a 2 b 1 c 2 d 3 e 2 f 1 g 2 h 1 Question 2 a Any probability measure Q equivalent to P on F 2 can be described by Q[{x 1, x 2 }] := q x1 q x1,x 2, 1 where q x1, q x1,x
More informationBrownian Motion. 1 Definition Brownian Motion Wiener measure... 3
Brownian Motion Contents 1 Definition 2 1.1 Brownian Motion................................. 2 1.2 Wiener measure.................................. 3 2 Construction 4 2.1 Gaussian process.................................
More informationChange of Variables. (f T) JT. f = U
Change of Variables 4-5-8 The change of ariables formla for mltiple integrals is like -sbstittion for single-ariable integrals. I ll gie the general change of ariables formla first, and consider specific
More informationStochastic Integration and Stochastic Differential Equations: a gentle introduction
Stochastic Integration and Stochastic Differential Equations: a gentle introduction Oleg Makhnin New Mexico Tech Dept. of Mathematics October 26, 27 Intro: why Stochastic? Brownian Motion/ Wiener process
More informationStochastic Differential Equations
CHAPTER 1 Stochastic Differential Equations Consider a stochastic process X t satisfying dx t = bt, X t,w t dt + σt, X t,w t dw t. 1.1 Question. 1 Can we obtain the existence and uniqueness theorem for
More informationStochastic Calculus (Lecture #3)
Stochastic Calculus (Lecture #3) Siegfried Hörmann Université libre de Bruxelles (ULB) Spring 2014 Outline of the course 1. Stochastic processes in continuous time. 2. Brownian motion. 3. Itô integral:
More informationStochastic Differential Equations
Chapter 5 Stochastic Differential Equations We would like to introduce stochastic ODE s without going first through the machinery of stochastic integrals. 5.1 Itô Integrals and Itô Differential Equations
More informationLecture 22 Girsanov s Theorem
Lecture 22: Girsanov s Theorem of 8 Course: Theory of Probability II Term: Spring 25 Instructor: Gordan Zitkovic Lecture 22 Girsanov s Theorem An example Consider a finite Gaussian random walk X n = n
More informationCIMPA SCHOOL, 2007 Jump Processes and Applications to Finance Monique Jeanblanc
CIMPA SCHOOL, 27 Jump Processes and Applications to Finance Monique Jeanblanc 1 Jump Processes I. Poisson Processes II. Lévy Processes III. Jump-Diffusion Processes IV. Point Processes 2 I. Poisson Processes
More informationarxiv: v1 [math.co] 25 Sep 2016
arxi:1609.077891 [math.co] 25 Sep 2016 Total domination polynomial of graphs from primary sbgraphs Saeid Alikhani and Nasrin Jafari September 27, 2016 Department of Mathematics, Yazd Uniersity, 89195-741,
More informationBernardo D Auria Stochastic Processes /12. Notes. March 29 th, 2012
1 Stochastic Calculus Notes March 9 th, 1 In 19, Bachelier proposed for the Paris stock exchange a model for the fluctuations affecting the price X(t) of an asset that was given by the Brownian motion.
More informationCharacterizations of probability distributions via bivariate regression of record values
Metrika (2008) 68:51 64 DOI 10.1007/s00184-007-0142-7 Characterizations of probability distribtions via bivariate regression of record vales George P. Yanev M. Ahsanllah M. I. Beg Received: 4 October 2006
More informationMalliavin Calculus: Analysis on Gaussian spaces
Malliavin Calculus: Analysis on Gaussian spaces Josef Teichmann ETH Zürich Oxford 2011 Isonormal Gaussian process A Gaussian space is a (complete) probability space together with a Hilbert space of centered
More informationLECTURE 2: LOCAL TIME FOR BROWNIAN MOTION
LECTURE 2: LOCAL TIME FOR BROWNIAN MOTION We will define local time for one-dimensional Brownian motion, and deduce some of its properties. We will then use the generalized Ray-Knight theorem proved in
More informationGeneralized Gaussian Bridges of Prediction-Invertible Processes
Generalized Gaussian Bridges of Prediction-Invertible Processes Tommi Sottinen 1 and Adil Yazigi University of Vaasa, Finland Modern Stochastics: Theory and Applications III September 1, 212, Kyiv, Ukraine
More informationAn Overview of the Martingale Representation Theorem
An Overview of the Martingale Representation Theorem Nuno Azevedo CEMAPRE - ISEG - UTL nazevedo@iseg.utl.pt September 3, 21 Nuno Azevedo (CEMAPRE - ISEG - UTL) LXDS Seminar September 3, 21 1 / 25 Background
More informationBernardo D Auria Stochastic Processes /10. Notes. Abril 13 th, 2010
1 Stochastic Calculus Notes Abril 13 th, 1 As we have seen in previous lessons, the stochastic integral with respect to the Brownian motion shows a behavior different from the classical Riemann-Stieltjes
More informationMath 4A03: Practice problems on Multivariable Calculus
Mat 4A0: Practice problems on Mltiariable Calcls Problem Consider te mapping f, ) : R R defined by fx, y) e y + x, e x y) x, y) R a) Is it possible to express x, y) as a differentiable fnction of, ) near
More informationStochastic Calculus February 11, / 33
Martingale Transform M n martingale with respect to F n, n =, 1, 2,... σ n F n (σ M) n = n 1 i= σ i(m i+1 M i ) is a Martingale E[(σ M) n F n 1 ] n 1 = E[ σ i (M i+1 M i ) F n 1 ] i= n 2 = σ i (M i+1 M
More informationAn Introduction to Malliavin calculus and its applications
An Introduction to Malliavin calculus and its applications Lecture 3: Clark-Ocone formula David Nualart Department of Mathematics Kansas University University of Wyoming Summer School 214 David Nualart
More informationImage and Multidimensional Signal Processing
Image and Mltidimensional Signal Processing Professor William Hoff Dept of Electrical Engineering &Compter Science http://inside.mines.ed/~whoff/ Forier Transform Part : D discrete transforms 2 Overview
More informationProblem 1. Construct a filtered probability space on which a Brownian motion W and an adapted process X are defined and such that
Stochatic Calculu Example heet 4 - Lent 5 Michael Tehranchi Problem. Contruct a filtered probability pace on which a Brownian motion W and an adapted proce X are defined and uch that dx t = X t t dt +
More informationOn the Total Duration of Negative Surplus of a Risk Process with Two-step Premium Function
Aailable at http://pame/pages/398asp ISSN: 93-9466 Vol, Isse (December 7), pp 7 (Preiosly, Vol, No ) Applications an Applie Mathematics (AAM): An International Jornal Abstract On the Total Dration of Negatie
More informationA MODEL FOR THE LONG-TERM OPTIMAL CAPACITY LEVEL OF AN INVESTMENT PROJECT
A MODEL FOR HE LONG-ERM OPIMAL CAPACIY LEVEL OF AN INVESMEN PROJEC ARNE LØKKA AND MIHAIL ZERVOS Abstract. We consider an investment project that produces a single commodity. he project s operation yields
More informationON THE STRUCTURE OF GAUSSIAN RANDOM VARIABLES
ON THE STRUCTURE OF GAUSSIAN RANDOM VARIABLES CIPRIAN A. TUDOR We study when a given Gaussian random variable on a given probability space Ω, F,P) is equal almost surely to β 1 where β is a Brownian motion
More informationON THE PATHWISE UNIQUENESS OF SOLUTIONS OF STOCHASTIC DIFFERENTIAL EQUATIONS
PORTUGALIAE MATHEMATICA Vol. 55 Fasc. 4 1998 ON THE PATHWISE UNIQUENESS OF SOLUTIONS OF STOCHASTIC DIFFERENTIAL EQUATIONS C. Sonoc Abstract: A sufficient condition for uniqueness of solutions of ordinary
More informationOn pathwise stochastic integration
On pathwise stochastic integration Rafa l Marcin Lochowski Afican Institute for Mathematical Sciences, Warsaw School of Economics UWC seminar Rafa l Marcin Lochowski (AIMS, WSE) On pathwise stochastic
More informationMA8109 Stochastic Processes in Systems Theory Autumn 2013
Norwegian University of Science and Technology Department of Mathematical Sciences MA819 Stochastic Processes in Systems Theory Autumn 213 1 MA819 Exam 23, problem 3b This is a linear equation of the form
More information13 The martingale problem
19-3-2012 Notations Ω complete metric space of all continuous functions from [0, + ) to R d endowed with the distance d(ω 1, ω 2 ) = k=1 ω 1 ω 2 C([0,k];H) 2 k (1 + ω 1 ω 2 C([0,k];H) ), ω 1, ω 2 Ω. F
More informationB8.3 Mathematical Models for Financial Derivatives. Hilary Term Solution Sheet 2
B8.3 Mathematical Models for Financial Derivatives Hilary Term 18 Solution Sheet In the following W t ) t denotes a standard Brownian motion and t > denotes time. A partition π of the interval, t is a
More informationMathematical Methods for Neurosciences. ENS - Master MVA Paris 6 - Master Maths-Bio ( )
Mathematical Methods for Neurosciences. ENS - Master MVA Paris 6 - Master Maths-Bio (2014-2015) Etienne Tanré - Olivier Faugeras INRIA - Team Tosca November 26th, 2014 E. Tanré (INRIA - Team Tosca) Mathematical
More informationMEAN VALUE ESTIMATES OF z Ω(n) WHEN z 2.
MEAN VALUE ESTIMATES OF z Ωn WHEN z 2 KIM, SUNGJIN 1 Introdction Let n i m pei i be the prime factorization of n We denote Ωn by i m e i Then, for any fixed complex nmber z, we obtain a completely mltiplicative
More informationSelected Exercises on Expectations and Some Probability Inequalities
Selected Exercises on Expectations and Some Probability Inequalities # If E(X 2 ) = and E X a > 0, then P( X λa) ( λ) 2 a 2 for 0 < λ
More informationBranching Processes II: Convergence of critical branching to Feller s CSB
Chapter 4 Branching Processes II: Convergence of critical branching to Feller s CSB Figure 4.1: Feller 4.1 Birth and Death Processes 4.1.1 Linear birth and death processes Branching processes can be studied
More informationECON3120/4120 Mathematics 2, spring 2009
University of Oslo Department of Economics Arne Strøm ECON3/4 Mathematics, spring 9 Problem soltions for Seminar 4, 6 Febrary 9 (For practical reasons some of the soltions may inclde problem parts that
More informationSibuya s Measure of Local Dependence
Versão formatada segndo a reista Estadistica 5/dez/8 Sibya s Measre of Local Dependence SUMAIA ABDEL LATIF () PEDRO ALBERTO MORETTIN () () School of Arts, Science and Hmanities Uniersity of São Palo, Ra
More informationPartial Differential Equations with Applications to Finance Seminar 1: Proving and applying Dynkin s formula
Partial Differential Equations with Applications to Finance Seminar 1: Proving and applying Dynkin s formula Group 4: Bertan Yilmaz, Richard Oti-Aboagye and Di Liu May, 15 Chapter 1 Proving Dynkin s formula
More informationOptimal Mean-Variance Portfolio Selection
Research Report No. 14, 2013, Probab. Statist. Grop Manchester 25 pp Optimal Mean-Variance Portfolio Selection J. L. Pedersen & G. Peskir Assming that the wealth process X is generated self-financially
More informationBrownian motion. Samy Tindel. Purdue University. Probability Theory 2 - MA 539
Brownian motion Samy Tindel Purdue University Probability Theory 2 - MA 539 Mostly taken from Brownian Motion and Stochastic Calculus by I. Karatzas and S. Shreve Samy T. Brownian motion Probability Theory
More informationTHE HOHENBERG-KOHN THEOREM FOR MARKOV SEMIGROUPS
THE HOHENBERG-KOHN THEOREM FOR MARKOV SEMIGROUPS OMAR HIJAB Abstract. At the basis of mch of comptational chemistry is density fnctional theory, as initiated by the Hohenberg-Kohn theorem. The theorem
More informationWeak solutions of mean-field stochastic differential equations
Weak solutions of mean-field stochastic differential equations Juan Li School of Mathematics and Statistics, Shandong University (Weihai), Weihai 26429, China. Email: juanli@sdu.edu.cn Based on joint works
More informationINPUT-OUTPUT APPROACH NUMERICAL EXAMPLES
INPUT-OUTPUT APPROACH NUMERICAL EXAMPLES EXERCISE s consider the linear dnamical sstem of order 2 with transfer fnction with Determine the gain 2 (H) of the inpt-otpt operator H associated with this sstem.
More informationON THE SHAPES OF BILATERAL GAMMA DENSITIES
ON THE SHAPES OF BILATERAL GAMMA DENSITIES UWE KÜCHLER, STEFAN TAPPE Abstract. We investigate the for parameter family of bilateral Gamma distribtions. The goal of this paper is to provide a thorogh treatment
More informationPrandl established a universal velocity profile for flow parallel to the bed given by
EM 0--00 (Part VI) (g) The nderlayers shold be at least three thicknesses of the W 50 stone, bt never less than 0.3 m (Ahrens 98b). The thickness can be calclated sing Eqation VI-5-9 with a coefficient
More informationClases 11-12: Integración estocástica.
Clases 11-12: Integración estocástica. Fórmula de Itô * 3 de octubre de 217 Índice 1. Introduction to Stochastic integrals 1 2. Stochastic integration 2 3. Simulation of stochastic integrals: Euler scheme
More informationChapter 4 Supervised learning:
Chapter 4 Spervised learning: Mltilayer Networks II Madaline Other Feedforward Networks Mltiple adalines of a sort as hidden nodes Weight change follows minimm distrbance principle Adaptive mlti-layer
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 7 9/25/2013
MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.65/15.070J Fall 013 Lecture 7 9/5/013 The Reflection Principle. The Distribution of the Maximum. Brownian motion with drift Content. 1. Quick intro to stopping times.
More informationReduction of over-determined systems of differential equations
Redction of oer-determined systems of differential eqations Maim Zaytse 1) 1, ) and Vyachesla Akkerman 1) Nclear Safety Institte, Rssian Academy of Sciences, Moscow, 115191 Rssia ) Department of Mechanical
More informationFEA Solution Procedure
EA Soltion Procedre (demonstrated with a -D bar element problem) EA Procedre for Static Analysis. Prepare the E model a. discretize (mesh) the strctre b. prescribe loads c. prescribe spports. Perform calclations
More informationTheory and Applications of Stochastic Systems Lecture Exponential Martingale for Random Walk
Instructor: Victor F. Araman December 4, 2003 Theory and Applications of Stochastic Systems Lecture 0 B60.432.0 Exponential Martingale for Random Walk Let (S n : n 0) be a random walk with i.i.d. increments
More informationTheoretical Tutorial Session 2
1 / 36 Theoretical Tutorial Session 2 Xiaoming Song Department of Mathematics Drexel University July 27, 216 Outline 2 / 36 Itô s formula Martingale representation theorem Stochastic differential equations
More informationEquivalence between transition systems. Modal logic and first order logic. In pictures: forth condition. Bisimilation. In pictures: back condition
odal logic and first order logic odal logic: local ie of the strctre ( here can I get by folloing links from here ). First order logic: global ie of the strctre (can see eerything, qantifiers do not follo
More informationTurbulence and boundary layers
Trblence and bondary layers Weather and trblence Big whorls hae little whorls which feed on the elocity; and little whorls hae lesser whorls and so on to iscosity Lewis Fry Richardson Momentm eqations
More informationExam Stochastic Processes 2WB08 - March 10, 2009,
Exam Stochastic Processes WB8 - March, 9, 4.-7. The number of points that can be obtained per exercise is mentioned between square brackets. The maximum number of points is 4. Good luck!!. (a) [ pts.]
More informationsin xdx = cos x + c We also run into antiderivatives for tan x, cot x, sec x and csc x in the section on Log integrals. They are: cos ax sec ax a
Trig Integrals We already know antiderivatives for sin x, cos x, sec x tan x, csc x, sec x and csc x cot x. They are cos xdx = sin x sin xdx = cos x sec x tan xdx = sec x csc xdx = cot x sec xdx = tan
More information9. Tensor product and Hom
9. Tensor prodct and Hom Starting from two R-modles we can define two other R-modles, namely M R N and Hom R (M, N), that are very mch related. The defining properties of these modles are simple, bt those
More informationCHANNEL SELECTION WITH RAYLEIGH FADING: A MULTI-ARMED BANDIT FRAMEWORK. Wassim Jouini and Christophe Moy
CHANNEL SELECTION WITH RAYLEIGH FADING: A MULTI-ARMED BANDIT FRAMEWORK Wassim Joini and Christophe Moy SUPELEC, IETR, SCEE, Avene de la Bolaie, CS 47601, 5576 Cesson Sévigné, France. INSERM U96 - IFR140-
More information1 Brownian Local Time
1 Brownian Local Time We first begin by defining the space and variables for Brownian local time. Let W t be a standard 1-D Wiener process. We know that for the set, {t : W t = } P (µ{t : W t = } = ) =
More informationA Theory of Markovian Time Inconsistent Stochastic Control in Discrete Time
A Theory of Markovian Time Inconsistent Stochastic Control in Discrete Time Tomas Björk Department of Finance, Stockholm School of Economics tomas.bjork@hhs.se Agatha Mrgoci Department of Economics Aarhs
More informationMS&E 321 Spring Stochastic Systems June 1, 2013 Prof. Peter W. Glynn Page 1 of 7
MS&E 321 Spring 12-13 Stochastic Systems June 1, 213 Prof. Peter W. Glynn Page 1 of 7 Section 9: Renewal Theory Contents 9.1 Renewal Equations..................................... 1 9.2 Solving the Renewal
More informationProperties of an infinite dimensional EDS system : the Muller s ratchet
Properties of an infinite dimensional EDS system : the Muller s ratchet LATP June 5, 2011 A ratchet source : wikipedia Plan 1 Introduction : The model of Haigh 2 3 Hypothesis (Biological) : The population
More informationEssentials of optimal control theory in ECON 4140
Essentials of optimal control theory in ECON 4140 Things yo need to know (and a detail yo need not care abot). A few words abot dynamic optimization in general. Dynamic optimization can be thoght of as
More informationConnectivity and Menger s theorems
Connectiity and Menger s theorems We hae seen a measre of connectiity that is based on inlnerability to deletions (be it tcs or edges). There is another reasonable measre of connectiity based on the mltiplicity
More informationSufficient Optimality Condition for a Risk-Sensitive Control Problem for Backward Stochastic Differential Equations and an Application
Jornal of Nmerical Mathematics and Stochastics, 9(1) : 48-6, 17 http://www.jnmas.org/jnmas9-4.pdf JNM@S Eclidean Press, LLC Online: ISSN 151-3 Sfficient Optimality Condition for a Risk-Sensitive Control
More informationComplexity of the Cover Polynomial
Complexity of the Coer Polynomial Marks Bläser and Holger Dell Comptational Complexity Grop Saarland Uniersity, Germany {mblaeser,hdell}@cs.ni-sb.de Abstract. The coer polynomial introdced by Chng and
More informationWe automate the bivariate change-of-variables technique for bivariate continuous random variables with
INFORMS Jornal on Compting Vol. 4, No., Winter 0, pp. 9 ISSN 09-9856 (print) ISSN 56-558 (online) http://dx.doi.org/0.87/ijoc.046 0 INFORMS Atomating Biariate Transformations Jeff X. Yang, John H. Drew,
More informationDYNAMICAL LOWER BOUNDS FOR 1D DIRAC OPERATORS. 1. Introduction We consider discrete, resp. continuous, Dirac operators
DYNAMICAL LOWER BOUNDS FOR D DIRAC OPERATORS ROBERTO A. PRADO AND CÉSAR R. DE OLIVEIRA Abstract. Qantm dynamical lower bonds for continos and discrete one-dimensional Dirac operators are established in
More information