Lecture 19 Semimartingales
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MAST31801 Mathematical Finance II, Spring 2019. Problem Sheet 8 (4-8.4.2019)
UH|Master program Mathematics and Statistics|MAST31801 Mathematical Finance II, Spring 2019. Problem sheet 8 (4-8.4.2019) 1. Show that a local martingale (Xt : t ≥ 0) in a filtration F, which is bounded from below is a supermartingale. Hint: use localization together with Fatou lemma. 2. A non-negative local martingale Xt ≥ 0 is a martingale if and only if E(Xt) = E(X0) 8t. 3. Recall Ito formula, for f(x; s) 2 C2;1 and a continuous semimartingale Xt with quadratic covariation hXit 1 Z t @2f Z t @f Z t @f f(Xt; t) − f(X0; 0) − 2 (Xs; s)dhXis − (Xs; s)ds = (Xs; s)dXs 2 0 @x 0 @s 0 @x where on the right side we have the Ito integral. We can also understand the Ito integral as limit in probability of Riemann sums X @f n n n n X(tk−1); tk−1 X(tk ^ t) − X(tk−1 ^ t) n n @x tk 2Π among a sequence of partitions Πn with ∆(Πn) ! 0. Recalling that the Brownian motion Wt has quadratic variation hW it = t, write the following Ito integrals explicitely by using Ito formula: R t n (a) 0 Ws dWs, n 2 N. R t (b) 0 exp σWs σdWs R t 2 (c) 0 exp σWs − σ s=2 σdWs R t (d) 0 sin(σWs)dWs R t (e) 0 cos(σWs)dWs 4. These Ito integrals as stochastic processes are semimartingales. Com- pute the quadratic variation of the Ito-integrals above. Hint: recall that the finite variation part of a semimartingale has zero quadratic variation, and the quadratic variation is bilinear. -
CONFORMAL INVARIANCE and 2 D STATISTICAL PHYSICS −
CONFORMAL INVARIANCE AND 2 d STATISTICAL PHYSICS − GREGORY F. LAWLER Abstract. A number of two-dimensional models in statistical physics are con- jectured to have scaling limits at criticality that are in some sense conformally invariant. In the last ten years, the rigorous understanding of such limits has increased significantly. I give an introduction to the models and one of the major new mathematical structures, the Schramm-Loewner Evolution (SLE). 1. Critical Phenomena Critical phenomena in statistical physics refers to the study of systems at or near the point at which a phase transition occurs. There are many models of such phenomena. We will discuss some discrete equilibrium models that are defined on a lattice. These are measures on paths or configurations where configurations are weighted by their energy with a preference for paths of smaller energy. These measures depend on at leastE one parameter. A standard parameter in physics β = c/T where c is a fixed constant, T stands for temperature and the measure given to a configuration is e−βE . Phase transitions occur at critical values of the temperature corresponding to, e.g., the transition from a gaseous to liquid state. We use β for the parameter although for understanding the literature it is useful to know that large values of β correspond to “low temperature” and small values of β correspond to “high temperature”. Small β (high temperature) systems have weaker correlations than large β (low temperature) systems. In a number of models, there is a critical βc such that qualitatively the system has three regimes β<βc (high temperature), β = βc (critical) and β>βc (low temperature). -
Applied Probability
ISSN 1050-5164 (print) ISSN 2168-8737 (online) THE ANNALS of APPLIED PROBABILITY AN OFFICIAL JOURNAL OF THE INSTITUTE OF MATHEMATICAL STATISTICS Articles Optimal control of branching diffusion processes: A finite horizon problem JULIEN CLAISSE 1 Change point detection in network models: Preferential attachment and long range dependence . SHANKAR BHAMIDI,JIMMY JIN AND ANDREW NOBEL 35 Ergodic theory for controlled Markov chains with stationary inputs YUE CHEN,ANA BUŠIC´ AND SEAN MEYN 79 Nash equilibria of threshold type for two-player nonzero-sum games of stopping TIZIANO DE ANGELIS,GIORGIO FERRARI AND JOHN MORIARTY 112 Local inhomogeneous circular law JOHANNES ALT,LÁSZLÓ ERDOS˝ AND TORBEN KRÜGER 148 Diffusion approximations for controlled weakly interacting large finite state systems withsimultaneousjumps.........AMARJIT BUDHIRAJA AND ERIC FRIEDLANDER 204 Duality and fixation in -Wright–Fisher processes with frequency-dependent selection ADRIÁN GONZÁLEZ CASANOVA AND DARIO SPANÒ 250 CombinatorialLévyprocesses.......................................HARRY CRANE 285 Eigenvalue versus perimeter in a shape theorem for self-interacting random walks MAREK BISKUP AND EVIATAR B. PROCACCIA 340 Volatility and arbitrage E. ROBERT FERNHOLZ,IOANNIS KARATZAS AND JOHANNES RUF 378 A Skorokhod map on measure-valued paths with applications to priority queues RAMI ATAR,ANUP BISWAS,HAYA KASPI AND KAV I TA RAMANAN 418 BSDEs with mean reflection . PHILIPPE BRIAND,ROMUALD ELIE AND YING HU 482 Limit theorems for integrated local empirical characteristic exponents from noisy high-frequency data with application to volatility and jump activity estimation JEAN JACOD AND VIKTOR TODOROV 511 Disorder and wetting transition: The pinned harmonic crystal indimensionthreeorlarger.....GIAMBATTISTA GIACOMIN AND HUBERT LACOIN 577 Law of large numbers for the largest component in a hyperbolic model ofcomplexnetworks..........NIKOLAOS FOUNTOULAKIS AND TOBIAS MÜLLER 607 Vol. -
Superprocesses and Mckean-Vlasov Equations with Creation of Mass
Sup erpro cesses and McKean-Vlasov equations with creation of mass L. Overb eck Department of Statistics, University of California, Berkeley, 367, Evans Hall Berkeley, CA 94720, y U.S.A. Abstract Weak solutions of McKean-Vlasov equations with creation of mass are given in terms of sup erpro cesses. The solutions can b e approxi- mated by a sequence of non-interacting sup erpro cesses or by the mean- eld of multityp e sup erpro cesses with mean- eld interaction. The lat- ter approximation is asso ciated with a propagation of chaos statement for weakly interacting multityp e sup erpro cesses. Running title: Sup erpro cesses and McKean-Vlasov equations . 1 Intro duction Sup erpro cesses are useful in solving nonlinear partial di erential equation of 1+ the typ e f = f , 2 0; 1], cf. [Dy]. Wenowchange the p oint of view and showhowtheyprovide sto chastic solutions of nonlinear partial di erential Supp orted byanFellowship of the Deutsche Forschungsgemeinschaft. y On leave from the Universitat Bonn, Institut fur Angewandte Mathematik, Wegelerstr. 6, 53115 Bonn, Germany. 1 equation of McKean-Vlasovtyp e, i.e. wewant to nd weak solutions of d d 2 X X @ @ @ + d x; + bx; : 1.1 = a x; t i t t t t t ij t @t @x @x @x i j i i=1 i;j =1 d Aweak solution = 2 C [0;T];MIR satis es s Z 2 t X X @ @ a f = f + f + d f + b f ds: s ij s t 0 i s s @x @x @x 0 i j i Equation 1.1 generalizes McKean-Vlasov equations of twodi erenttyp es. -
A Stochastic Processes and Martingales
A Stochastic Processes and Martingales A.1 Stochastic Processes Let I be either IINorIR+.Astochastic process on I with state space E is a family of E-valued random variables X = {Xt : t ∈ I}. We only consider examples where E is a Polish space. Suppose for the moment that I =IR+. A stochastic process is called cadlag if its paths t → Xt are right-continuous (a.s.) and its left limits exist at all points. In this book we assume that every stochastic process is cadlag. We say a process is continuous if its paths are continuous. The above conditions are meant to hold with probability 1 and not to hold pathwise. A.2 Filtration and Stopping Times The information available at time t is expressed by a σ-subalgebra Ft ⊂F.An {F ∈ } increasing family of σ-algebras t : t I is called a filtration.IfI =IR+, F F F we call a filtration right-continuous if t+ := s>t s = t. If not stated otherwise, we assume that all filtrations in this book are right-continuous. In many books it is also assumed that the filtration is complete, i.e., F0 contains all IIP-null sets. We do not assume this here because we want to be able to change the measure in Chapter 4. Because the changed measure and IIP will be singular, it would not be possible to extend the new measure to the whole σ-algebra F. A stochastic process X is called Ft-adapted if Xt is Ft-measurable for all t. If it is clear which filtration is used, we just call the process adapted.The {F X } natural filtration t is the smallest right-continuous filtration such that X is adapted. -
Derivatives of Self-Intersection Local Times
Derivatives of self-intersection local times Jay Rosen? Department of Mathematics College of Staten Island, CUNY Staten Island, NY 10314 e-mail: [email protected] Summary. We show that the renormalized self-intersection local time γt(x) for both the Brownian motion and symmetric stable process in R1 is differentiable in 0 the spatial variable and that γt(0) can be characterized as the continuous process of zero quadratic variation in the decomposition of a natural Dirichlet process. This Dirichlet process is the potential of a random Schwartz distribution. Analogous results for fractional derivatives of self-intersection local times in R1 and R2 are also discussed. 1 Introduction In their study of the intrinsic Brownian local time sheet and stochastic area integrals for Brownian motion, [14, 15, 16], Rogers and Walsh were led to analyze the functional Z t A(t, Bt) = 1[0,∞)(Bt − Bs) ds (1) 0 where Bt is a 1-dimensional Brownian motion. They showed that A(t, Bt) is not a semimartingale, and in fact showed that Z t Bs A(t, Bt) − Ls dBs (2) 0 x has finite non-zero 4/3-variation. Here Ls is the local time at x, which is x R s formally Ls = 0 δ(Br − x) dr, where δ(x) is Dirac’s ‘δ-function’. A formal d d2 0 application of Ito’s lemma, using dx 1[0,∞)(x) = δ(x) and dx2 1[0,∞)(x) = δ (x), yields Z t 1 Z t Z s Bs 0 A(t, Bt) − Ls dBs = t + δ (Bs − Br) dr ds (3) 0 2 0 0 ? This research was supported, in part, by grants from the National Science Foun- dation and PSC-CUNY. -
Semimartingale Properties of a Generalized Fractional Brownian Motion and Its Mixtures with Applications in finance
Semimartingale properties of a generalized fractional Brownian motion and its mixtures with applications in finance TOMOYUKI ICHIBA, GUODONG PANG, AND MURAD S. TAQQU ABSTRACT. We study the semimartingale properties for the generalized fractional Brownian motion (GFBM) introduced by Pang and Taqqu (2019) and discuss the applications of the GFBM and its mixtures to financial models, including stock price and rough volatility. The GFBM is self-similar and has non-stationary increments, whose Hurst index H 2 (0; 1) is determined by two parameters. We identify the region of these two parameter values where the GFBM is a semimartingale. Specifically, in one region resulting in H 2 (1=2; 1), it is in fact a process of finite variation and differentiable, and in another region also resulting in H 2 (1=2; 1) it is not a semimartingale. For regions resulting in H 2 (0; 1=2] except the Brownian motion case, the GFBM is also not a semimartingale. We also establish p-variation results of the GFBM, which are used to provide an alternative proof of the non-semimartingale property when H < 1=2. We then study the semimartingale properties of the mixed process made up of an independent Brownian motion and a GFBM with a Hurst parameter H 2 (1=2; 1), and derive the associated equivalent Brownian measure. We use the GFBM and its mixture with a BM to study financial asset models. The first application involves stock price models with long range dependence that generalize those using shot noise processes and FBMs. When the GFBM is a process of finite variation (resulting in H 2 (1=2; 1)), the mixed GFBM process as a stock price model is a Brownian motion with a random drift of finite variation. -
Skorohod Stochastic Integration with Respect to Non-Adapted Processes on Wiener Space Nicolas Privault
Skorohod stochastic integration with respect to non-adapted processes on Wiener space Nicolas Privault Equipe d'Analyse et Probabilit´es,Universit´ed'Evry-Val d'Essonne Boulevard des Coquibus, 91025 Evry Cedex, France e-mail: [email protected] Abstract We define a Skorohod type anticipative stochastic integral that extends the It^ointegral not only with respect to the Wiener process, but also with respect to a wide class of stochastic processes satisfying certain homogeneity and smoothness conditions, without requirements relative to filtrations such as adaptedness. Using this integral, a change of variable formula that extends the classical and Skorohod It^oformulas is obtained. Key words: It^ocalculus, Malliavin calculus, Skorohod integral. Mathematics Subject Classification (1991): 60H05, 60H07. 1 Introduction The Skorohod integral, defined by creation on Fock space, is an extension of the It^o integral with respect to the Wiener or Poisson processes, depending on the probabilis- tic interpretation chosen for the Fock space. This means that it coincides with the It^ointegral on square-integrable adapted processes. It can also extend the stochastic integral with respect to certain normal martingales, cf. [10], but it always acts with respect to the underlying process relative to a given probabilistic interpretation. The Skorohod integral is also linked to the Stratonovich, forward and backward integrals, and allows to extend the It^oformula to a class of Skorohod integral processes which contains non-adapted processes that have a certain structure. In this paper we introduce an extended Skorohod stochastic integral on Wiener space that can act with respect to processes other than Brownian motion. -
Local Time and Tanaka Formula for G-Brownian Motion
Local time and Tanaka formula for the G-Brownian motion∗ Qian LIN 1,2† 1School of Mathematics, Shandong University, Jinan 250100, China; 2 Laboratoire de Math´ematiques, CNRS UMR 6205, Universit´ede Bretagne Occidentale, 6, avenue Victor Le Gorgeu, CS 93837, 29238 Brest cedex 3, France. Abstract In this paper, we study the notion of local time and obtain the Tanaka formula for the G-Brownian motion. Moreover, the joint continuity of the local time of the G- Brownian motion is obtained and its quadratic variation is proven. As an application, we generalize Itˆo’s formula with respect to the G-Brownian motion to convex functions. Keywords: G-expectation; G-Brownian motion; local time; Tanaka formula; quadratic variation. 1 Introduction The objective of the present paper is to study the local time as well as the Tanaka formula for the G-Brownian motion. Motivated by uncertainty problems, risk measures and superhedging in finance, Peng has introduced a new notion of nonlinear expectation, the so-called G-expectation (see [10], [12], [13], [15], [16]), which is associated with the following nonlinear heat equation 2 ∂u(t,x) ∂ u(t,x) R arXiv:0912.1515v3 [math.PR] 20 Oct 2012 = G( 2 ), (t,x) [0, ) , ∂t ∂x ∈ ∞ × u(0,x)= ϕ(x), where, for given parameters 0 σ σ, the sublinear function G is defined as follows: ≤ ≤ 1 G(α)= (σ2α+ σ2α−), α R. 2 − ∈ The G-expectation represents a special case of general nonlinear expectations Eˆ whose importance stems from the fact that they are related to risk measures ρ in finance by ∗Corresponding address: Institute of Mathematical Economics, Bielefeld University, Postfach 100131, 33501 Bielefeld, Germany †Email address: [email protected] 1 the relation Eˆ[X] = ρ( X), where X runs the class of contingent claims. -
Deep Optimal Stopping
Journal of Machine Learning Research 20 (2019) 1-25 Submitted 4/18; Revised 1/19; Published 4/19 Deep Optimal Stopping Sebastian Becker [email protected] Zenai AG, 8045 Zurich, Switzerland Patrick Cheridito [email protected] RiskLab, Department of Mathematics ETH Zurich, 8092 Zurich, Switzerland Arnulf Jentzen [email protected] SAM, Department of Mathematics ETH Zurich, 8092 Zurich, Switzerland Editor: Jon McAuliffe Abstract In this paper we develop a deep learning method for optimal stopping problems which directly learns the optimal stopping rule from Monte Carlo samples. As such, it is broadly applicable in situations where the underlying randomness can efficiently be simulated. We test the approach on three problems: the pricing of a Bermudan max-call option, the pricing of a callable multi barrier reverse convertible and the problem of optimally stopping a fractional Brownian motion. In all three cases it produces very accurate results in high- dimensional situations with short computing times. Keywords: optimal stopping, deep learning, Bermudan option, callable multi barrier reverse convertible, fractional Brownian motion 1. Introduction N We consider optimal stopping problems of the form supτ E g(τ; Xτ ), where X = (Xn)n=0 d is an R -valued discrete-time Markov process and the supremum is over all stopping times τ based on observations of X. Formally, this just covers situations where the stopping decision can only be made at finitely many times. But practically all relevant continuous- time stopping problems can be approximated with time-discretized versions. The Markov assumption means no loss of generality. We make it because it simplifies the presentation and many important problems already are in Markovian form. -
Fclts for the Quadratic Variation of a CTRW and for Certain Stochastic Integrals
FCLTs for the Quadratic Variation of a CTRW and for certain stochastic integrals No`eliaViles Cuadros (joint work with Enrico Scalas) Universitat de Barcelona Sevilla, 17 de Septiembre 2013 Damped harmonic oscillator subject to a random force The equation of motion is informally given by x¨(t) + γx_(t) + kx(t) = ξ(t); (1) where x(t) is the position of the oscillating particle with unit mass at time t, γ > 0 is the damping coefficient, k > 0 is the spring constant and ξ(t) represents white L´evynoise. I. M. Sokolov, Harmonic oscillator under L´evynoise: Unexpected properties in the phase space. Phys. Rev. E. Stat. Nonlin Soft Matter Phys 83, 041118 (2011). 2 of 27 The formal solution is Z t x(t) = F (t) + G(t − t0)ξ(t0)dt0; (2) −∞ where G(t) is the Green function for the homogeneous equation. The solution for the velocity component can be written as Z t 0 0 0 v(t) = Fv (t) + Gv (t − t )ξ(t )dt ; (3) −∞ d d where Fv (t) = dt F (t) and Gv (t) = dt G(t). 3 of 27 • Replace the white noise with a sequence of instantaneous shots of random amplitude at random times. • They can be expressed in terms of the formal derivative of compound renewal process, a random walk subordinated to a counting process called continuous-time random walk. A continuous time random walk (CTRW) is a pure jump process given by a sum of i.i.d. random jumps fYi gi2N separated by i.i.d. random waiting times (positive random variables) fJi gi2N. -
Solving Black-Schole Equation Using Standard Fractional Brownian Motion
http://jmr.ccsenet.org Journal of Mathematics Research Vol. 11, No. 2; 2019 Solving Black-Schole Equation Using Standard Fractional Brownian Motion Didier Alain Njamen Njomen1 & Eric Djeutcha2 1 Department of Mathematics and Computer’s Science, Faculty of Science, University of Maroua, Cameroon 2 Department of Mathematics, Higher Teachers’ Training College, University of Maroua, Cameroon Correspondence: Didier Alain Njamen Njomen, Department of Mathematics and Computer’s Science, Faculty of Science, University of Maroua, Po-Box 814, Cameroon. Received: May 2, 2017 Accepted: June 5, 2017 Online Published: March 24, 2019 doi:10.5539/jmr.v11n2p142 URL: https://doi.org/10.5539/jmr.v11n2p142 Abstract In this paper, we emphasize the Black-Scholes equation using standard fractional Brownian motion BH with the hurst index H 2 [0; 1]. N. Ciprian (Necula, C. (2002)) and Bright and Angela (Bright, O., Angela, I., & Chukwunezu (2014)) get the same formula for the evaluation of a Call and Put of a fractional European with the different approaches. We propose a formula by adapting the non-fractional Black-Scholes model using a λH factor to evaluate the european option. The price of the option at time t 2]0; T[ depends on λH(T − t), and the cost of the action S t, but not only from t − T as in the classical model. At the end, we propose the formula giving the implied volatility of sensitivities of the option and indicators of the financial market. Keywords: stock price, black-Scholes model, fractional Brownian motion, options, volatility 1. Introduction Among the first systematic treatments of the option pricing problem has been the pioneering work of Black, Scholes and Merton (see Black, F.