A Joint Point Process Model for Information Diffusion and Network Co-Evolution
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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. -
POISSON PROCESSES 1.1. the Rutherford-Chadwick-Ellis
POISSON PROCESSES 1. THE LAW OF SMALL NUMBERS 1.1. The Rutherford-Chadwick-Ellis Experiment. About 90 years ago Ernest Rutherford and his collaborators at the Cavendish Laboratory in Cambridge conducted a series of pathbreaking experiments on radioactive decay. In one of these, a radioactive substance was observed in N = 2608 time intervals of 7.5 seconds each, and the number of decay particles reaching a counter during each period was recorded. The table below shows the number Nk of these time periods in which exactly k decays were observed for k = 0,1,2,...,9. Also shown is N pk where k pk = (3.87) exp 3.87 =k! {− g The parameter value 3.87 was chosen because it is the mean number of decays/period for Rutherford’s data. k Nk N pk k Nk N pk 0 57 54.4 6 273 253.8 1 203 210.5 7 139 140.3 2 383 407.4 8 45 67.9 3 525 525.5 9 27 29.2 4 532 508.4 10 16 17.1 5 408 393.5 ≥ This is typical of what happens in many situations where counts of occurences of some sort are recorded: the Poisson distribution often provides an accurate – sometimes remarkably ac- curate – fit. Why? 1.2. Poisson Approximation to the Binomial Distribution. The ubiquity of the Poisson distri- bution in nature stems in large part from its connection to the Binomial and Hypergeometric distributions. The Binomial-(N ,p) distribution is the distribution of the number of successes in N independent Bernoulli trials, each with success probability p. -
6 Mar 2019 Strict Local Martingales and the Khasminskii Test for Explosions
Strict Local Martingales and the Khasminskii Test for Explosions Aditi Dandapani∗† and Philip Protter‡§ March 7, 2019 Abstract We exhibit sufficient conditions such that components of a multidimen- sional SDE giving rise to a local martingale M are strict local martingales or martingales. We assume that the equations have diffusion coefficients of the form σ(Mt, vt), with vt being a stochastic volatility term. We dedicate this paper to the memory of Larry Shepp 1 Introduction In 2007 P.L. Lions and M. Musiela (2007) gave a sufficient condition for when a unique weak solution of a one dimensional stochastic volatility stochastic differen- tial equation is a strict local martingale. Lions and Musiela also gave a sufficient condition for it to be a martingale. Similar results were obtained by L. Andersen and V. Piterbarg (2007). The techniques depend at one key stage on Feller’s test for explosions, and as such are uniquely applicable to the one dimensional case. Earlier, in 2002, F. Delbaen and H. Shirakawa (2002) gave a seminal result giving arXiv:1903.02383v1 [q-fin.MF] 6 Mar 2019 necessary and sufficient conditions for a solution of a one dimensional stochastic differential equation (without stochastic volatility) to be a strict local martingale or not. This was later extended by A. Mijatovic and M. Urusov (2012) and then by ∗Applied Mathematics Department, Columbia University, New York, NY 10027; email: [email protected]; Currently at Ecole Polytechnique, Palaiseau, France. †Supported in part by NSF grant DMS-1308483 ‡Statistics Department, Columbia University, New York, NY 10027; email: [email protected]. -
Geometric Brownian Motion with Affine Drift and Its Time-Integral
Geometric Brownian motion with affine drift and its time-integral ⋆ a b, c Runhuan Feng , Pingping Jiang ∗, Hans Volkmer aDepartment of Mathematics, University of Illinois at Urbana-Champaign, Illinois, USA bSchool of Management and Economics,The Chinese University of Hong Kong, Shenzhen, Shenzhen, Guangdong, 518172, P.R. China School of Management, University of Science and Technology of China, Hefei, Anhui, 230026, P.R.China cDepartment of Mathematical Sciences, University of Wisconsin–Milwaukee, Wisconsin, USA Abstract The joint distribution of a geometric Brownian motion and its time-integral was derived in a seminal paper by Yor (1992) using Lamperti’s transformation, leading to explicit solutions in terms of modified Bessel functions. In this paper, we revisit this classic result using the simple Laplace transform approach in connection to the Heun differential equation. We extend the methodology to the geometric Brownian motion with affine drift and show that the joint distribution of this process and its time-integral can be determined by a doubly-confluent Heun equation. Furthermore, the joint Laplace transform of the process and its time-integral is derived from the asymptotics of the solutions. In addition, we provide an application by using the results for the asymptotics of the double-confluent Heun equation in pricing Asian options. Numerical results show the accuracy and efficiency of this new method. Keywords: Doubly-confluent Heun equation, geometric Brownian motion with affine drift, Lamperti’s transformation, asymptotics, boundary value problem. ⋆R. Feng is supported by an endowment from the State Farm Companies Foundation. P. Jiang arXiv:2012.09661v1 [q-fin.MF] 17 Dec 2020 is supported by the Postdoctoral Science Foundation of China (No.2020M671853) and the National Natural Science Foundation of China (No. -
Jump-Diffusion Models for Asset Pricing in Financial Engineering
J.R. Birge and V. Linetsky (Eds.), Handbooks in OR & MS, Vol. 15 Copyright © 2008 Elsevier B.V. All rights reserved DOI: 10.1016/S0927-0507(07)15002-7 Chapter 2 Jump-Diffusion Models for Asset Pricing in Financial Engineering S.G. Kou Department of Industrial Engineering and Operations Research, Columbia University E-mail: [email protected] Abstract In this survey we shall focus on the following issues related to jump-diffusion mod- els for asset pricing in financial engineering. (1) The controversy over tailweight of distributions. (2) Identifying a risk-neutral pricing measure by using the rational ex- pectations equilibrium. (3) Using Laplace transforms to pricing options, including European call/put options, path-dependent options, such as barrier and lookback op- tions. (4) Difficulties associated with the partial integro-differential equations related to barrier-crossing problems. (5) Analytical approximations for finite-horizon Amer- ican options with jump risk. (6) Multivariate jump-diffusion models. 1Introduction There is a large literature on jump-diffusion models in finance, including several excellent books, e.g. the books by Cont and Tankov (2004), Kijima (2002). So a natural question is why another survey article is needed. What we attempt to achieve in this survey chapter is to emphasis some points that have not been well addressed in previous surveys. More precisely we shall focus on the following issues. (1) The controversy over tailweight of distributions. An empirical motiva- tion for using jump-diffusion models comes from the fact that asset return distributions tend to have heavier tails than those of normal dis- tribution. However, it is not clear how heavy the tail distributions are, as some people favor power-type distributions, others exponential-type distributions. -
1 the Ito Integral
Derivative Securities, Fall 2010 Mathematics in Finance Program Courant Institute of Mathematical Sciences, NYU Jonathan Goodman http://www.math.nyu.edu/faculty/goodman/teaching/DerivSec10/resources.html Week 6 1 The Ito integral The Black Scholes reasoning asks us to apply calculus, stochastic calculus, to expressions involving differentials of Brownian motion and other diffusion pro- cesses. To do this, we define the Ito integral with respect to Brownian motion and a general diffusion. Things discussed briefly and vaguely here are discussed in more detail and at greater length in Stochastic calculus. Suppose Xt is a diffusion process that satisfies (18) and (19) from week 5. Suppose that ft is another stochastic process that is adapted to the same filtration F. The Ito integral is Z t Yt = fs dXs : (1) 0 You could call this the \indefinite integral" because we care how the answer depends on t. In particular, the Ito integral is one of the ways to construct a new stochastic process, Yt, from old ones ft and Xt. It is not possible to define (1) unless ft is adapted. If ft is allowed to depend 0 on future values Xt0 (t > t), then the integral may not make sense or it may not have the properties we expect. The essential technical idea in the definition of (1) is that dXs is in the future of s. If we think that dXs = Xs+ds − Xs, then we must take ds > 0 (but infinitely close to zero). This implies that if Xt is a martingale, then Yt also is a martingale. -
Rescaling Marked Point Processes
1 Rescaling Marked Point Processes David Vere-Jones1, Victoria University of Wellington Frederic Paik Schoenberg2, University of California, Los Angeles Abstract In 1971, Meyer showed how one could use the compensator to rescale a multivari- ate point process, forming independent Poisson processes with intensity one. Meyer’s result has been generalized to multi-dimensional point processes. Here, we explore gen- eralization of Meyer’s theorem to the case of marked point processes, where the mark space may be quite general. Assuming simplicity and the existence of a conditional intensity, we show that a marked point process can be transformed into a compound Poisson process with unit total rate and a fixed mark distribution. ** Key words: residual analysis, random time change, Meyer’s theorem, model evaluation, intensity, compensator, Poisson process. ** 1 Department of Mathematics, Victoria University of Wellington, P.O. Box 196, Welling- ton, New Zealand. [email protected] 2 Department of Statistics, 8142 Math-Science Building, University of California, Los Angeles, 90095-1554. [email protected] Vere-Jones and Schoenberg. Rescaling Marked Point Processes 2 1 Introduction. Before other matters, both authors would like express their appreciation to Daryl for his stimulating and forgiving company, and to wish him a long and fruitful continuation of his mathematical, musical, woodworking, and many other activities. In particular, it is a real pleasure for the first author to acknowledge his gratitude to Daryl for his hard work, good humour, generosity and continuing friendship throughout the development of (innumerable draft versions and now even two editions of) their joint text on point processes. -
Lecture 26 : Poisson Point Processes
Lecture 26 : Poisson Point Processes STAT205 Lecturer: Jim Pitman Scribe: Ben Hough <[email protected]> In this lecture, we consider a measure space (S; S; µ), where µ is a σ-finite measure (i.e. S may be written as a disjoint union of sets of finite µ-measure). 26.1 The Poisson Point Process Definition 26.1 A Poisson Point Process (P.P.P.) with intensity µ is a collection of random variables N(A; !), A 2 S, ! 2 Ω defined on a probability space (Ω; F; P) such that: 1. N(·; !) is a counting measure on (S; S) for each ! 2 Ω. 2. N(A; ·) is Poisson with mean µ(A): − P e µ(A)(µ(A))k (N(A) = k) = k! all A 2 S. 3. If A1, A2, ... are disjoint sets then N(A1; ·), N(A2; ·), ... are independent random variables. Theorem 26.2 P.P.P.'s exist. Proof Sketch: It's not enough to quote Kolmogorov's Extension Theorem. The only convincing argument is to give an explicit constuction from sequences of independent random variables. We begin by considering the case µ(S) < 1. P µ(A) 1. Take X1, X2, ... to be i.i.d. random variables so that (Xi 2 A) = µ(S) . 2. Take N(S) to be a Poisson random variable with mean µ(S), independent of the Xi's. Assume all random varibles are defined on the same probability space (Ω; F; P). N(S) 3. Define N(A) = i=1 1(Xi2A), for all A 2 S. P 1 Now verify that this N(A; !) is a P.P.P. -
A Stochastic Lomax Diffusion Process: Statistical Inference and Application
mathematics Article A Stochastic Lomax Diffusion Process: Statistical Inference and Application Ahmed Nafidi 1,†, Ilyasse Makroz 1,*,† and Ramón Gutiérrez Sánchez 2,† 1 Department of Mathematics and Informatics, National School of Applied Sciences, Hassan First University of Settat, LAMSAD, Avenue de l’université, Berrechid BP 280, Morocco; ahmed.nafi[email protected] 2 Department of Statistics and Operational Research, Facultad de Ciencias, Campus de Fuentenueva, University of Granada, 18071 Granada, Spain; [email protected] * Correspondence: [email protected] † These authors contributed equally to this work. Abstract: In this paper, we discuss a new stochastic diffusion process in which the trend function is proportional to the Lomax density function. This distribution arises naturally in the studies of the frequency of extremely rare events. We first consider the probabilistic characteristics of the proposed model, including its analytic expression as the unique solution to a stochastic differential equation, the transition probability density function together with the conditional and unconditional trend functions. Then, we present a method to address the problem of parameter estimation using maximum likelihood with discrete sampling. This estimation requires the solution of a non-linear equation, which is achieved via the simulated annealing method. Finally, we apply the proposed model to a real-world example concerning adolescent fertility rate in Morocco. Keywords: stochastic differential equation; lomax distribution; trend functions; statistical inference; simulated annealing; adolescent fertility rate Citation: Nafidi, A.; Makroz, I.; 1. Introduction Gutiérrez-Sánchez, R. A Stochastic Stochastic diffusion models are used to analyze the evolution of phenomena in multi- Lomax Diffusion Process: Statistical ple fields of science, including biology, finance, energy consumption and physics. -
A Guide to Brownian Motion and Related Stochastic Processes
Vol. 0 (0000) A guide to Brownian motion and related stochastic processes Jim Pitman and Marc Yor Dept. Statistics, University of California, 367 Evans Hall # 3860, Berkeley, CA 94720-3860, USA e-mail: [email protected] Abstract: This is a guide to the mathematical theory of Brownian mo- tion and related stochastic processes, with indications of how this theory is related to other branches of mathematics, most notably the classical the- ory of partial differential equations associated with the Laplace and heat operators, and various generalizations thereof. As a typical reader, we have in mind a student, familiar with the basic concepts of probability based on measure theory, at the level of the graduate texts of Billingsley [43] and Durrett [106], and who wants a broader perspective on the theory of Brow- nian motion and related stochastic processes than can be found in these texts. Keywords and phrases: Markov process, random walk, martingale, Gaus- sian process, L´evy process, diffusion. AMS 2000 subject classifications: Primary 60J65. Contents 1 Introduction................................. 3 1.1 History ................................ 3 1.2 Definitions............................... 4 2 BM as a limit of random walks . 5 3 BMasaGaussianprocess......................... 7 3.1 Elementarytransformations . 8 3.2 Quadratic variation . 8 3.3 Paley-Wiener integrals . 8 3.4 Brownianbridges........................... 10 3.5 FinestructureofBrownianpaths . 10 arXiv:1802.09679v1 [math.PR] 27 Feb 2018 3.6 Generalizations . 10 3.6.1 FractionalBM ........................ 10 3.6.2 L´evy’s BM . 11 3.6.3 Browniansheets ....................... 11 3.7 References............................... 11 4 BMasaMarkovprocess.......................... 12 4.1 Markovprocessesandtheirsemigroups. 12 4.2 ThestrongMarkovproperty. 14 4.3 Generators ............................. -
A Course in Interacting Particle Systems
A Course in Interacting Particle Systems J.M. Swart January 14, 2020 arXiv:1703.10007v2 [math.PR] 13 Jan 2020 2 Contents 1 Introduction 7 1.1 General set-up . .7 1.2 The voter model . .9 1.3 The contact process . 11 1.4 Ising and Potts models . 14 1.5 Phase transitions . 17 1.6 Variations on the voter model . 20 1.7 Further models . 22 2 Continuous-time Markov chains 27 2.1 Poisson point sets . 27 2.2 Transition probabilities and generators . 30 2.3 Poisson construction of Markov processes . 31 2.4 Examples of Poisson representations . 33 3 The mean-field limit 35 3.1 Processes on the complete graph . 35 3.2 The mean-field limit of the Ising model . 36 3.3 Analysis of the mean-field model . 38 3.4 Functions of Markov processes . 42 3.5 The mean-field contact process . 47 3.6 The mean-field voter model . 49 3.7 Exercises . 51 4 Construction and ergodicity 53 4.1 Introduction . 53 4.2 Feller processes . 54 4.3 Poisson construction . 63 4.4 Generator construction . 72 4.5 Ergodicity . 79 4.6 Application to the Ising model . 81 4.7 Further results . 85 5 Monotonicity 89 5.1 The stochastic order . 89 5.2 The upper and lower invariant laws . 94 5.3 The contact process . 97 5.4 Other examples . 100 3 4 CONTENTS 5.5 Exercises . 101 6 Duality 105 6.1 Introduction . 105 6.2 Additive systems duality . 106 6.3 Cancellative systems duality . 113 6.4 Other dualities . -
Point Processes, Temporal
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CiteSeerX Point processes, temporal David R. Brillinger, Peter M. Guttorp & Frederic Paik Schoenberg Volume 3, pp 1577–1581 in Encyclopedia of Environmetrics (ISBN 0471 899976) Edited by Abdel H. El-Shaarawi and Walter W. Piegorsch John Wiley & Sons, Ltd, Chichester, 2002 is an encyclopedic account of the theory of the Point processes, temporal subject. A temporal point process is a random process whose Examples realizations consist of the times fjg, j 2 , j D 0, š1, š2,... of isolated events scattered in time. A Examples of point processes abound in the point process is also known as a counting process or environment; we have already mentioned times a random scatter. The times may correspond to events of floods. There are also times of earthquakes, of several types. fires, deaths, accidents, hurricanes, storms (hale, Figure 1 presents an example of temporal point ice, thunder), volcanic eruptions, lightning strikes, process data. The figure actually provides three dif- tornadoes, power outages, chemical spills (see ferent ways of representing the timing of floods Meteorological extremes; Natural disasters). on the Amazon River near Manaus, Brazil, dur- ing the period 1892–1992 (see Hydrological ex- tremes)[7]. Questions The formal use of the concept of point process has a long history going back at least to the life tables The questions that scientists ask involving point of Graunt [14]. Physicists contributed many ideas in process data include the following. Is a point pro- the first half of the twentieth century; see, for ex- cess associated with another process? Is the associ- ample, [23].