Stochastic Processes

Total Page:16

File Type:pdf, Size:1020Kb

Stochastic Processes Stochastic Processes Winter Term 2016-2017 Paolo Di Tella Technische Universit¨atDresden Institut f¨urStochastik Contents 1 Preliminaries 5 1.1 Uniform integrability . .5 1.2 Monotone class theorems . .6 1.3 Conditional expectation and probability . .7 Appendix 1.A Measure and integration theory . .9 2 Introduction to the general theory of stochastic processes 12 2.1 Kolmogorov extension theorem . 12 2.2 Paths of stochastic processes . 17 2.3 Filtrations, stopping times and martingales . 19 2.4 Markov processes . 23 2.5 Processes with independent increments . 30 3 Brownian Motion and stochastic integration 38 3.1 Definition, existence and continuity . 38 3.1.1 Definition of the Brownian motion . 38 3.1.2 Existence of a Brownian motion . 40 3.1.3 Existence of a continuous modification . 40 3.1.4 (Ir)Regularity of paths . 41 3.2 P. L`evyCharacterization of Brownian Motion . 42 3.3 Stochastic integration . 45 3.3.1 Stochastic integral of elementary processes . 46 3.3.2 Extension of the stochastic integral . 48 3.4 Miscellanea . 54 3.4.1 Stochastic integral as a process . 54 3.4.2 A further extension of the stochastic integral . 55 3.4.3 It^o'sformula . 56 4 Poisson Process 58 4.1 Processes of finite variation and stochastic integration . 58 4.2 Poisson Process: definition and characterization . 63 4.3 Independence of Poisson processes . 65 Contents 4 5 Poisson random measures 72 5.1 Random measures . 72 5.2 Definition of Poisson random measure . 74 5.3 Stochastic integration for Poisson random measures . 76 5.4 Compensated Poisson random measures . 78 5.4.1 Stochastic integration for compensated Poisson random measures . 79 5.5 Construction of L´evyprocesses . 81 5.6 The jump measure of a L´evyprocesses . 85 5.7 L´evy{It^oand L´evy{Khintchine decomposition . 90 Bibliography 98 CHAPTER 1 Preliminaries In this chapter we collect some of the results of measure theory needed for this lecture notes. In the appendix we summarize well-known result of measure and integration theory, which are assumed to be known to the reader. 1.1 Uniform integrability 1 1 1 Let (Ω; F ; P) a Probability space and L = L (P) := L (Ω; F ; P). 1 R 1.1.1 Exercise. X 2 L if and only if limN!1 fjX|≥Ng jXjdP = 0. Exercise 1.1.1 justifies the following definition: 1.1.2 Definition. (i) We say that a family K ⊆ L1 is uniformly integrable if supX2K E[jXj1fjX|≥Ng] −! 0 as N ! +1: 1 (ii) A sequence (Xn)n2N ⊆ L is uniformly integrable if K := fX1;:::g is uniformly integrable. If K is dominated in L1, i.e., there exists Y 2 L1 such that jXj ≤ Y , for every X 2 K , then K is uniformly integrable. Clearly, any finite family of integrable random variables is uniformly integrable. However, if a family K is uniformly integrable, this does not mean that it is also dominated in L1. Therefore the following results, for which we refer to Dellacherie & Meyer (1978), Theorem II.21, is a generalization of Lebesgue theorem on dominated convergence (cf. Theorem 1.A.3). 1 1.1.3 Theorem. Let (Xn)n2N be a sequence of random variables in L converging almost surely (or only in probability) to a random variable X. Then the following assertions are equivalent: 1 1 (i) X belongs to L and (Xn)n2N converges in L to X. (ii) The family K := (Xn)n2N is uniformly integrable. 1.2 Monotone class theorems 6 1 1.1.4 Corollary. Let (Xn)n2N ⊆ L be uniformly integrable and converge to X a. s. 1 Then X 2 L and E[Xn] converges to E[X], whenever n ! +1. Proof. Exercise. The following result, known as La Vall´ee{Poussin's Theorem (cf. Dellacherie & Meyer (1978), Theorem II.22), is a characterisation of the uniform integrability 1.1.5 Theorem. A family K of integrable random variables is uniformly integrable if and only if there exists a positive, convex and increasing function G on [0; +1] into G(x) [0; +1) such that: (i) x converges to +1 as x ! +1; (ii) supX2K E[G(jXj)] < +1. Because of La Vall´ee{Poussin's Theorem, we can conclude that a family of random q variables is uniformly integrable if it is q-integrable and bounded in L (P), q > 1. 1.2 Monotone class theorems Monotone class theorems are of different kinds and they are present in the literature in several formulations. We consider only one formulation for sets and one for functions. We refer to Sharpe (1988) and He, Wang & Yan (1992). We start with a monotone class theorem for systems of sets in the same form as He, Wang & Yan (1992), Theorem 1.2. We say that a class K of subsets of Ω is a monotone class if for every monotone sequence (An)n2N ⊆ K such that An " A or An # A as n ! +1, A 2 K . 1.2.1 Theorem (Monotone class theorem for sets). Let F be an algebra and K a monotone class of sets of Ω such that F ⊆ K . Then σ(F ) ⊆ K . For the formulation of the monotone class theorem for classes of functions we refer to Sharpe (1988), Appendix A0. Let (Ω; F ) be a measurable space. We denote by B := B(Ω; R) the set of bounded measurable functions on (Ω; F ) into (R; B(R)). If K is a linear subspace of B we say that it is a monotone vector space if 1 = 1Ω 2 K and if it is monotonically closed, that is, if (fn)n2N ⊆ K is such that 0 ≤ fn ≤ fn+1, for all n 2 N and f 2 B is such that f = limn!+1 fn, then f 2 K . We observe that the limit f belongs to B if and only if (fn)n2N is uniformly bounded. A set C ⊆ B is called a multiplicative class if it is closed with respect to the multiplication of two elements, meaning that if h and g belong to C , then also their product hg does. 1.2.2 Theorem (Monotone class theorem for functions). Let K be a monotone vector space and C a multiplicative class such that C ⊆ K and σ(C ) = F . Then K = B. Let (Ω; F ) be a measurable space and µ a measure on it. Given a system T of numerical functions on (Ω; F ), we denote by Span(T ) its linear hull. Now we fix q in q q (L (µ);k·kq) q [1; +1). If T ⊆ L (µ) we denote by T the closure of T in (L (µ); k · kq). q q A system T ⊆ L (µ) of functions is called total in (L (µ); k · kq) if its linear hull is q (L (µ);k·kq) dense, that is, Span(T ) = Lq(µ). If µ is a finite measure, then the inclusions q p q p L (µ) ⊆ L (µ), q ≥ p, hold and L (µ) is a total system in (L ; k · kp). In particular, L1(µ) is an example of total system in Lq(µ), for every q 2 [1; +1). As an application of Theorem 1.2.2, we want to establish a general lemma stating sufficient conditions for 1.3 Conditional expectation and probability 7 a system T ⊆ Lq(µ) of bounded functions to be total in Lq(µ), for q 2 [1; +1). We recall that we use the notation B := B(Ω; R) to denote the space of bounded measurable functions on (Ω; F ) into (R; B(R)). q q 1.2.3 Lemma. Let T ⊆ L (µ) be a subset of B. Then T is total in L (µ) if the following conditions are satisfied: (i) T is stable under multiplication; (ii) σ(T ) = F ; (iii) There exists a sequence (hn)n2N ⊆ Span(T ) such that hn ≥ 0 and hn " 1 pointwise as n ! +1. q Proof. First, we consider the case in which µ is a finite measure. In this case B ⊆ L (µ) q q (L (µ);k·kq) and it is dense in (L (µ); k · kq). We define H := Span(T ) and then K := H \ B. Clearly, K is a closed linear space and T ⊆ K . By assumption, hn " 1 pointwise as n ! +1 and by the finiteness of µ, 1 2 Lq(µ). From the theorem of q Lebesgue on dominated convergence (cf. Theorem 1.A.3) hn converges to 1 in L (µ) and so 1 2 K . Moreover, K is closed under monotone convergence of uniformly bounded nonnegative functions, as a consequence of the finiteness of µ and of Theorem 1.A.3. Consequently, K is a monotone class and by Theorem 1.2.2, we get K = B. Hence q B ⊆ H and since B is dense and H is closed, this yields L (µ) = H . Now we consider q q the case of a general measure µ. For f 2 L (µ) we put dµn := jhnj dµ, n ≥ 1, where (hn)n2N is as in the assumptions of the lemma. Obviously, µn is a finite measure for q q q every n. Moreover, with notation in (A.1) below, µn(jfj ) = µ(jfhnj ) ≤ µ(jfj ) < +1 q and hence f 2 L (µn). We choose a sequence ("n)n2N such that "n > 0 and "n # 0 as n ! +1. By the previous step, there exists a sequence (gn)n2N ⊆ Span(T ) such that Z Z q q q jf hn − gn hnj dµ = jf − gnj jhnj dµ < "n ; n ≥ 1: Ω Ω The system T is stable under multiplication so gnhn 2 Span(T ).
Recommended publications
  • Stochastic Differential Equations
    Stochastic Differential Equations Stefan Geiss November 25, 2020 2 Contents 1 Introduction 5 1.0.1 Wolfgang D¨oblin . .6 1.0.2 Kiyoshi It^o . .7 2 Stochastic processes in continuous time 9 2.1 Some definitions . .9 2.2 Two basic examples of stochastic processes . 15 2.3 Gaussian processes . 17 2.4 Brownian motion . 31 2.5 Stopping and optional times . 36 2.6 A short excursion to Markov processes . 41 3 Stochastic integration 43 3.1 Definition of the stochastic integral . 44 3.2 It^o'sformula . 64 3.3 Proof of Ito^'s formula in a simple case . 76 3.4 For extended reading . 80 3.4.1 Local time . 80 3.4.2 Three-dimensional Brownian motion is transient . 83 4 Stochastic differential equations 87 4.1 What is a stochastic differential equation? . 87 4.2 Strong Uniqueness of SDE's . 90 4.3 Existence of strong solutions of SDE's . 94 4.4 Theorems of L´evyand Girsanov . 98 4.5 Solutions of SDE's by a transformation of drift . 103 4.6 Weak solutions . 105 4.7 The Cox-Ingersoll-Ross SDE . 108 3 4 CONTENTS 4.8 The martingale representation theorem . 116 5 BSDEs 121 5.1 Introduction . 121 5.2 Setting . 122 5.3 A priori estimate . 123 Chapter 1 Introduction One goal of the lecture is to study stochastic differential equations (SDE's). So let us start with a (hopefully) motivating example: Assume that Xt is the share price of a company at time t ≥ 0 where we assume without loss of generality that X0 := 1.
    [Show full text]
  • Completely Random Measures and Related Models
    CRMs Sinead Williamson Background Completely random measures and related L´evyprocesses Completely models random measures Applications Normalized Sinead Williamson random measures Neutral-to-the- right processes Computational and Biological Learning Laboratory Exchangeable University of Cambridge matrices January 20, 2011 Outline CRMs Sinead Williamson 1 Background Background L´evyprocesses Completely 2 L´evyprocesses random measures Applications 3 Completely random measures Normalized random measures Neutral-to-the- right processes 4 Applications Exchangeable matrices Normalized random measures Neutral-to-the-right processes Exchangeable matrices A little measure theory CRMs Sinead Williamson Set: e.g. Integers, real numbers, people called James. Background May be finite, countably infinite, or uncountably infinite. L´evyprocesses Completely Algebra: Class T of subsets of a set T s.t. random measures 1 T 2 T . 2 If A 2 T , then Ac 2 T . Applications K Normalized 3 If A1;:::; AK 2 T , then [ Ak = A1 [ A2 [ ::: AK 2 T random k=1 measures (closed under finite unions). Neutral-to-the- right K processes 4 If A1;:::; AK 2 T , then \k=1Ak = A1 \ A2 \ ::: AK 2 T Exchangeable matrices (closed under finite intersections). σ-Algebra: Algebra that is closed under countably infinite unions and intersections. A little measure theory CRMs Sinead Williamson Background L´evyprocesses Measurable space: Combination (T ; T ) of a set and a Completely σ-algebra on that set. random measures Measure: Function µ between a σ-field and the positive Applications reals (+ 1) s.t. Normalized random measures 1 µ(;) = 0. Neutral-to-the- right 2 For all countable collections of disjoint sets processes P Exchangeable A1; A2; · · · 2 T , µ([k Ak ) = µ(Ak ).
    [Show full text]
  • A University of Sussex Phd Thesis Available Online Via Sussex
    A University of Sussex PhD thesis Available online via Sussex Research Online: http://sro.sussex.ac.uk/ This thesis is protected by copyright which belongs to the author. This thesis cannot be reproduced or quoted extensively from without first obtaining permission in writing from the Author The content must not be changed in any way or sold commercially in any format or medium without the formal permission of the Author When referring to this work, full bibliographic details including the author, title, awarding institution and date of the thesis must be given Please visit Sussex Research Online for more information and further details NON-STATIONARY PROCESSES AND THEIR APPLICATION TO FINANCIAL HIGH-FREQUENCY DATA Mailan Trinh A thesis submitted for the degree of Doctor of Philosophy University of Sussex March 2018 UNIVERSITY OF SUSSEX MAILAN TRINH A THESIS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY NON-STATIONARY PROCESSES AND THEIR APPLICATION TO FINANCIAL HIGH-FREQUENCY DATA SUMMARY The thesis is devoted to non-stationary point process models as generalizations of the standard homogeneous Poisson process. The work can be divided in two parts. In the first part, we introduce a fractional non-homogeneous Poisson process (FNPP) by applying a random time change to the standard Poisson process. We character- ize the FNPP by deriving its non-local governing equation. We further compute moments and covariance of the process and discuss the distribution of the arrival times. Moreover, we give both finite-dimensional and functional limit theorems for the FNPP and the corresponding fractional non-homogeneous compound Poisson process. The limit theorems are derived by using martingale methods, regular vari- ation properties and Anscombe's theorem.
    [Show full text]
  • STOCHASTIC COMPARISONS and AGING PROPERTIES of an EXTENDED GAMMA PROCESS Zeina Al Masry, Sophie Mercier, Ghislain Verdier
    STOCHASTIC COMPARISONS AND AGING PROPERTIES OF AN EXTENDED GAMMA PROCESS Zeina Al Masry, Sophie Mercier, Ghislain Verdier To cite this version: Zeina Al Masry, Sophie Mercier, Ghislain Verdier. STOCHASTIC COMPARISONS AND AGING PROPERTIES OF AN EXTENDED GAMMA PROCESS. Journal of Applied Probability, Cambridge University press, 2021, 58 (1), pp.140-163. 10.1017/jpr.2020.74. hal-02894591 HAL Id: hal-02894591 https://hal.archives-ouvertes.fr/hal-02894591 Submitted on 9 Jul 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Applied Probability Trust (4 July 2020) STOCHASTIC COMPARISONS AND AGING PROPERTIES OF AN EXTENDED GAMMA PROCESS ZEINA AL MASRY,∗ FEMTO-ST, Univ. Bourgogne Franche-Comt´e,CNRS, ENSMM SOPHIE MERCIER & GHISLAIN VERDIER,∗∗ Universite de Pau et des Pays de l'Adour, E2S UPPA, CNRS, LMAP, Pau, France Abstract Extended gamma processes have been seen to be a flexible extension of standard gamma processes in the recent reliability literature, for cumulative deterioration modeling purpose. The probabilistic properties of the standard gamma process have been well explored since the 1970's, whereas those of its extension remain largely unexplored. In particular, stochastic comparisons between degradation levels modeled by standard gamma processes and aging properties for the corresponding level-crossing times are nowadays well understood.
    [Show full text]
  • Lecture Notes
    Lecture Notes Lars Peter Hansen October 8, 2007 2 Contents 1 Approximation Results 5 1.1 One way to Build a Stochastic Process . 5 1.2 Stationary Stochastic Process . 6 1.3 Invariant Events and the Law of Large Numbers . 6 1.4 Another Way to Build a Stochastic Process . 8 1.4.1 Stationarity . 8 1.4.2 Limiting behavior . 9 1.4.3 Ergodicity . 10 1.5 Building Nonstationary Processes . 10 1.6 Martingale Approximation . 11 3 4 CONTENTS Chapter 1 Approximation Results 1.1 One way to Build a Stochastic Process • Consider a probability space (Ω, F, P r) where Ω is a set of sample points, F is an event collection (sigma algebra) and P r assigns proba- bilities to events . • Introduce a function S :Ω → Ω such that for any event Λ, S−1(Λ) = {ω ∈ Ω: S(ω) ∈ Λ} is an event. • Introduce a (Borel measurable) measurement function x :Ω → Rn. x is a random vector. • Construct a stochastic process {Xt : t = 1, 2, ...} via the formula: t Xt(ω) = X[S (ω)] or t Xt = X ◦ S . Example 1.1.1. Let Ω be a collection of infinite sequences of real numbers. Specifically, ω = (r0, r1, ...), S(ω) = (r1, r2, ...) and x(ω) = r0. Then Xt(ω) = rt. 5 6 CHAPTER 1. APPROXIMATION RESULTS 1.2 Stationary Stochastic Process Definition 1.2.1. The transformation S is measure-preserving if: P r(Λ) = P r{S−1(Λ)} for all Λ ∈ F. Proposition 1.2.2. When S is measure-preserving, the process {Xt : t = 1, 2, ...} has identical distributions for every t.
    [Show full text]
  • Arbitrage Free Approximations to Candidate Volatility Surface Quotations
    Journal of Risk and Financial Management Article Arbitrage Free Approximations to Candidate Volatility Surface Quotations Dilip B. Madan 1,* and Wim Schoutens 2,* 1 Robert H. Smith School of Business, University of Maryland, College Park, MD 20742, USA 2 Department of Mathematics, KU Leuven, 3000 Leuven, Belgium * Correspondence: [email protected] (D.B.M.); [email protected] (W.S.) Received: 19 February 2019; Accepted: 10 April 2019; Published: 21 April 2019 Abstract: It is argued that the growth in the breadth of option strikes traded after the financial crisis of 2008 poses difficulties for the use of Fourier inversion methodologies in volatility surface calibration. Continuous time Markov chain approximations are proposed as an alternative. They are shown to be adequate, competitive, and stable though slow for the moment. Further research can be devoted to speed enhancements. The Markov chain approximation is general and not constrained to processes with independent increments. Calibrations are illustrated for data on 2695 options across 28 maturities for SPY as at 8 February 2018. Keywords: bilateral gamma; fast Fourier transform; sato process; matrix exponentials JEL Classification: G10; G12; G13 1. Introduction A variety of arbitrage free models for approximating quoted option prices have been available for some time. The quotations are typically in terms of (Black and Scholes 1973; Merton 1973) implied volatilities for the traded strikes and maturities. Consequently, the set of such quotations is now popularly referred to as the volatility surface. Some of the models are nonparametric with the Dupire(1994) local volatility model being a popular example. The local volatility model is specified in terms of a deterministic function s(K, T) that expresses the local volatility for the stock if the stock were to be at level K at time T.
    [Show full text]
  • Portfolio Optimization and Option Pricing Under Defaultable Lévy
    Universit`adegli Studi di Padova Dipartimento di Matematica Scuola di Dottorato in Scienze Matematiche Indirizzo Matematica Computazionale XXVI◦ ciclo Portfolio optimization and option pricing under defaultable L´evy driven models Direttore della scuola: Ch.mo Prof. Paolo Dai Pra Coordinatore dell’indirizzo: Ch.ma Prof.ssa. Michela Redivo Zaglia Supervisore: Ch.mo Prof. Tiziano Vargiolu Universit`adegli Studi di Padova Corelatori: Ch.mo Prof. Agostino Capponi Ch.mo Prof. Andrea Pascucci Johns Hopkins University Universit`adegli Studi di Bologna Dottorando: Stefano Pagliarani To Carolina and to my family “An old man, who had spent his life looking for a winning formula (martingale), spent the last days of his life putting it into practice, and his last pennies to see it fail. The martingale is as elusive as the soul.” Alexandre Dumas Mille et un fantˆomes, 1849 Acknowledgements First and foremost, I would like to thank my supervisor Prof. Tiziano Vargiolu and my co-advisors Prof. Agostino Capponi and Prof. Andrea Pascucci, for coauthoring with me all the material appearing in this thesis. In particular, thank you to Tiziano Vargiolu for supporting me scientifically and finan- cially throughout my research and all the activities related to it. Thank you to Agostino Capponi for inviting me twice to work with him at Purdue University, and for his hospital- ity and kindness during my double stay in West Lafayette. Thank you to Andrea Pascucci for wisely leading me throughout my research during the last four years, and for giving me the chance to collaborate with him side by side, thus sharing with me his knowledge and his experience.
    [Show full text]
  • Some Theory for the Analysis of Random Fields Diplomarbeit
    Philipp Pluch Some Theory for the Analysis of Random Fields With Applications to Geostatistics Diplomarbeit zur Erlangung des akademischen Grades Diplom-Ingenieur Studium der Technischen Mathematik Universit¨at Klagenfurt Fakult¨at fur¨ Wirtschaftswissenschaften und Informatik Begutachter: O.Univ.-Prof.Dr. Jurgen¨ Pilz Institut fur¨ Mathematik September 2004 To my parents, Verena and all my friends Ehrenw¨ortliche Erkl¨arung Ich erkl¨are ehrenw¨ortlich, dass ich die vorliegende Schrift verfasst und die mit ihr unmittelbar verbundenen Arbeiten selbst durchgefuhrt¨ habe. Die in der Schrift verwendete Literatur sowie das Ausmaß der mir im gesamten Arbeitsvorgang gew¨ahrten Unterstutzung¨ sind ausnahmslos angegeben. Die Schrift ist noch keiner anderen Prufungsb¨ eh¨orde vorgelegt worden. St. Urban, 29 September 2004 Preface I remember when I first was at our univeristy - I walked inside this large corridor called ’Aula’ and had no idea what I should do, didn’t know what I should study, I had interest in Psychology or Media Studies, and now I’m sitting in my office at the university, five years later, writing my final lines for my master degree theses in mathematics. A long and also hard but so beautiful way was gone, I remember at the beginning, the first mathematic courses in discrete mathematics, how difficult that was for me, the abstract thinking, my first exams and now I have finished them all, I mastered them. I have to thank so many people and I will do so now. First I have to thank my parents, who always believed in me, who gave me financial support and who had to fight with my mood when I was working hard.
    [Show full text]
  • Completely Random Measures
    Pacific Journal of Mathematics COMPLETELY RANDOM MEASURES JOHN FRANK CHARLES KINGMAN Vol. 21, No. 1 November 1967 PACIFIC JOURNAL OF MATHEMATICS Vol. 21, No. 1, 1967 COMPLETELY RANDOM MEASURES J. F. C. KlNGMAN The theory of stochastic processes is concerned with random functions defined on some parameter set. This paper is con- cerned with the case, which occurs naturally in some practical situations, in which the parameter set is a ^-algebra of subsets of some space, and the random functions are all measures on this space. Among all such random measures are distinguished some which are called completely random, which have the property that the values they take on disjoint subsets are independent. A representation theorem is proved for all completely random measures satisfying a weak finiteness condi- tion, and as a consequence it is shown that all such measures are necessarily purely atomic. 1. Stochastic processes X(t) whose realisation are nondecreasing functions of a real parameter t occur in a number of applications of probability theory. For instance, the number of events of a point process in the interval (0, t), the 'load function' of a queue input [2], the amount of water entering a reservoir in time t, and the local time process in a Markov chain ([8], [7] §14), are all processes of this type. In many applications the function X(t) enters as a convenient way of representing a measure on the real line, the Stieltjes measure Φ defined as the unique Borel measure for which (1) Φ(a, b] = X(b + ) - X(a + ), (-co <α< b< oo).
    [Show full text]
  • A Representation Free Quantum Stochastic Calculus
    JOURNAL OF FUNCTIONAL ANALYSIS 104, 149-197 (1992) A Representation Free Quantum Stochastic Calculus L. ACCARDI Centro Matemarico V. Volterra, Diparfimento di Matematica, Universitci di Roma II, Rome, Italy F. FACNOLA Dipartimento di Matematica, Vniversild di Trento, Povo, Italy AND J. QUAEGEBEUR Department of Mathemarics, Universiteit Leuven, Louvain, Belgium Communicated by L. Gross Received January 2; revised March 1, 1991 We develop a representation free stochastic calculus based on three inequalities (semimartingale inequality, scalar forward derivative inequality, scalar conditional variance inequality). We prove that our scheme includes all the previously developed stochastic calculi and some new examples. The abstract theory is applied to prove a Boson Levy martingale representation theorem in bounded form and a general existence, uniqueness, and unitarity theorem for quantum stochastic differential equations. 0 1992 Academic Press. Inc. 0. INTRODUCTION Stochastic calculus is a powerful tool in classical probability theory. Recently various kinds of stochastic calculi have been introduced in quan- tum probability [18, 12, 10,211. The common features of these calculi are: - One starts from a representation of the canonical commutation (or anticommutation) relations (CCR or CAR) over a space of the form L2(R+, dr; X) (where 3? is a given Hilbert space). - One introduces a family of operator valued measures on R,, related to this representation, e.g., expressed in terms of creation or annihilation or number or field operators. 149 0022-1236192 $3.00 Copyright 0 1992 by Academic Press, Inc. All rights of reproduction in any form reserved. 150 QUANTUM STOCHASTIC CALCULUS -- One shows that it is possible to develop a theory of stochastic integration with respect to these operator valued measures sufficiently rich to allow one to solve some nontrivial stochastic differential equations.
    [Show full text]
  • Lecture 18 : Itō Calculus
    Lecture 18 : Itō Calculus 1. Ito's calculus In the previous lecture, we have observed that a sample Brownian path is nowhere differentiable with probability 1. In other words, the differentiation dBt dt does not exist. However, while studying Brownain motions, or when using Brownian motion as a model, the situation of estimating the difference of a function of the type f(Bt) over an infinitesimal time difference occurs quite frequently (suppose that f is a smooth function). To be more precise, we are considering a function f(t; Bt) which depends only on the second variable. Hence there exists an implicit dependence on time since the Brownian motion depends on time. dBt If the differentiation dt existed, then we can easily do this by using chain rule: dB df = t · f 0(B ) dt: dt t We already know that the formula above makes no sense. One possible way to work around this problem is to try to describe the difference df in terms of the difference dBt. In this case, the equation above becomes 0 (1.1) df = f (Bt)dBt: Our new formula at least makes sense, since there is no need to refer to the dBt differentiation dt which does not exist. The only problem is that it does not quite work. Consider the Taylor expansion of f to obtain (∆x)2 (∆x)3 f(x + ∆x) − f(x) = (∆x) · f 0(x) + f 00(x) + f 000(x) + ··· : 2 6 To deduce Equation (1.1) from this formula, we must be able to say that the significant term is the first term (∆x) · f 0(x) and all other terms are of smaller order of magnitude.
    [Show full text]
  • The Ito Integral
    Notes on the Itoˆ Calculus Steven P. Lalley May 15, 2012 1 Continuous-Time Processes: Progressive Measurability 1.1 Progressive Measurability Measurability issues are a bit like plumbing – a bit ugly, and most of the time you would prefer that it remains hidden from view, but sometimes it is unavoidable that you actually have to open it up and work on it. In the theory of continuous–time stochastic processes, measurability problems are usually more subtle than in discrete time, primarily because sets of measures 0 can add up to something significant when you put together uncountably many of them. In stochastic integration there is another issue: we must be sure that any stochastic processes Xt(!) that we try to integrate are jointly measurable in (t; !), so as to ensure that the integrals are themselves random variables (that is, measurable in !). Assume that (Ω; F;P ) is a fixed probability space, and that all random variables are F−measurable. A filtration is an increasing family F := fFtgt2J of sub-σ−algebras of F indexed by t 2 J, where J is an interval, usually J = [0; 1). Recall that a stochastic process fYtgt≥0 is said to be adapted to a filtration if for each t ≥ 0 the random variable Yt is Ft−measurable, and that a filtration is admissible for a Wiener process fWtgt≥0 if for each t > 0 the post-t increment process fWt+s − Wtgs≥0 is independent of Ft. Definition 1. A stochastic process fXtgt≥0 is said to be progressively measurable if for every T ≥ 0 it is, when viewed as a function X(t; !) on the product space ([0;T ])×Ω, measurable relative to the product σ−algebra B[0;T ] × FT .
    [Show full text]