🎲Mathematical Probability Theory Unit 11 – Stochastic Processes

Stochastic processes are mathematical models that describe random systems evolving over time or space. They're essential in fields like finance, physics, and biology, helping us understand and predict complex phenomena with inherent uncertainty. This unit covers key concepts like state spaces, sample paths, and stationarity. We'll explore various types of stochastic processes, including Markov chains, Poisson processes, and Brownian motion, and their applications in real-world scenarios.

Key Concepts and Definitions

  • Stochastic process is a collection of random variables indexed by time or space representing the evolution of a random system
  • State space is the set of all possible values that a stochastic process can take at any given time or position
  • Sample path (or realization) refers to a single possible outcome or trajectory of a stochastic process over time or space
  • Stationarity implies that the statistical properties of a stochastic process do not change over time (time-invariant)
    • Strict stationarity requires the joint probability distribution to be invariant under time shifts
    • Weak stationarity (or covariance stationarity) only requires the mean and covariance to be time-invariant
  • Ergodicity is a property where the statistical properties of a stochastic process can be inferred from a single, sufficiently long realization
  • Martingale is a stochastic process whose expected value at any future time, given the current state, is equal to its current value
    • Submartingales have expected future values greater than or equal to the current value
    • Supermartingales have expected future values less than or equal to the current value

Types of Stochastic Processes

  • Discrete-time processes have random variables indexed by discrete time steps (integers) while continuous-time processes have random variables indexed by a continuous time parameter (real numbers)
  • Markov processes are memoryless stochastic processes where the future state depends only on the current state, not on the past states
    • Markov chains are discrete-time Markov processes with a countable state space
    • Continuous-time Markov chains have a countable state space but continuous time parameter
  • Gaussian processes are stochastic processes where any finite collection of random variables has a multivariate normal distribution
    • Brownian motion (or Wiener process) is a continuous-time Gaussian process with independent increments
  • Poisson processes model the occurrence of rare events in continuous time with a constant average rate
  • Renewal processes generalize Poisson processes by allowing the inter-arrival times between events to have any distribution (not necessarily exponential)
  • Birth-death processes are continuous-time Markov chains used to model population dynamics with birth and death rates

Probability Spaces and Random Variables

  • Probability space (Ω,F,P)(\Omega, \mathcal{F}, P) consists of a sample space Ω\Omega (set of all possible outcomes), a σ\sigma-algebra F\mathcal{F} of events (subsets of Ω\Omega), and a probability measure PP assigning probabilities to events
  • Random variable XX is a measurable function from the sample space Ω\Omega to the real numbers R\mathbb{R}, assigning a numerical value to each outcome
    • Discrete random variables take countable values (integers) while continuous random variables take uncountable values (real numbers)
  • Probability distribution of a random variable XX is a function that assigns probabilities to the possible values or ranges of values that XX can take
    • Probability mass function (PMF) for discrete random variables: P(X=x)P(X = x)
    • Probability density function (PDF) for continuous random variables: fX(x)f_X(x) such that P(aXb)=abfX(x)dxP(a \leq X \leq b) = \int_a^b f_X(x) dx
  • Expected value (or mean) of a random variable XX is the average value it takes, denoted by E[X]\mathbb{E}[X]
    • For discrete XX: E[X]=xxP(X=x)\mathbb{E}[X] = \sum_x x P(X = x)
    • For continuous XX: E[X]=xfX(x)dx\mathbb{E}[X] = \int_{-\infty}^{\infty} x f_X(x) dx
  • Variance of a random variable XX measures its spread around the mean, denoted by Var(X)=E[(XE[X])2]\text{Var}(X) = \mathbb{E}[(X - \mathbb{E}[X])^2]

Markov Chains

  • Markov chain is a discrete-time stochastic process with the Markov property: the future state depends only on the current state, not on the past states
    • State space SS is the set of possible values the Markov chain can take at each time step (countable)
    • Transition probability pijp_{ij} is the probability of moving from state ii to state jj in one time step: pij=P(Xn+1=jXn=i)p_{ij} = P(X_{n+1} = j | X_n = i)
  • Transition probability matrix P=(pij)P = (p_{ij}) contains all the transition probabilities, with rows summing to 1
  • nn-step transition probability pij(n)p_{ij}^{(n)} is the probability of moving from state ii to state jj in nn time steps, obtained by taking the nn-th power of the transition probability matrix: Pn=(pij(n))P^n = (p_{ij}^{(n)})
  • Stationary distribution π=(π1,π2,)\pi = (\pi_1, \pi_2, \ldots) is a probability distribution over the states that remains unchanged under the transition probabilities: πP=π\pi P = \pi
    • If a Markov chain is irreducible (all states communicate) and aperiodic, it has a unique stationary distribution
  • Absorbing Markov chains have one or more absorbing states that, once entered, cannot be left
    • Fundamental matrix N=(IQ)1N = (I - Q)^{-1} gives the expected number of visits to each transient state before absorption, where QQ is the submatrix of transient-to-transient transition probabilities

Poisson Processes

  • Poisson process is a continuous-time stochastic process that models the occurrence of rare events with a constant average rate λ>0\lambda > 0
    • Inter-arrival times between events are independent and exponentially distributed with mean 1/λ1/\lambda
    • Number of events in any interval of length tt follows a Poisson distribution with mean λt\lambda t: P(N(t)=k)=(λt)keλtk!P(N(t) = k) = \frac{(\lambda t)^k e^{-\lambda t}}{k!}
  • Superposition of independent Poisson processes with rates λ1,λ2,,λn\lambda_1, \lambda_2, \ldots, \lambda_n is also a Poisson process with rate λ=i=1nλi\lambda = \sum_{i=1}^n \lambda_i
  • Thinning (or splitting) a Poisson process with rate λ\lambda into two independent Poisson processes with rates pλp\lambda and (1p)λ(1-p)\lambda, where 0<p<10 < p < 1, is done by assigning each event to the first process with probability pp and to the second process with probability 1p1-p
  • Non-homogeneous Poisson process has a time-varying rate function λ(t)\lambda(t), with the expected number of events in an interval [a,b][a, b] given by abλ(t)dt\int_a^b \lambda(t) dt
  • Compound Poisson process associates a random variable (mark) with each event in a Poisson process, representing the event's magnitude or cost

Brownian Motion

  • Brownian motion (or Wiener process) is a continuous-time stochastic process {B(t),t0}\{B(t), t \geq 0\} with the following properties:
    • B(0)=0B(0) = 0 (starts at the origin)
    • Independent increments: for any t1<t2t3<t4t_1 < t_2 \leq t_3 < t_4, B(t4)B(t3)B(t_4) - B(t_3) is independent of B(t2)B(t1)B(t_2) - B(t_1)
    • Stationary increments: for any s<ts < t, B(t)B(s)B(t) - B(s) has a normal distribution with mean 0 and variance tst-s
    • Sample paths are continuous almost surely (with probability 1)
  • Standard Brownian motion has unit variance per unit time, while a general Brownian motion can have any constant variance σ2\sigma^2 per unit time
  • Brownian bridge is a Brownian motion conditioned to start and end at specified values, often used to model random processes with fixed endpoints
  • Geometric Brownian motion is a stochastic process {S(t),t0}\{S(t), t \geq 0\} where the logarithm of S(t)S(t) follows a Brownian motion with drift: dlogS(t)=μdt+σdB(t)d\log S(t) = \mu dt + \sigma dB(t)
    • Used to model stock prices in the Black-Scholes option pricing model
  • Fractional Brownian motion is a generalization of Brownian motion with correlated increments, characterized by the Hurst parameter H(0,1)H \in (0, 1)
    • For H=1/2H = 1/2, it reduces to standard Brownian motion
    • For H>1/2H > 1/2, increments are positively correlated (persistent)
    • For H<1/2H < 1/2, increments are negatively correlated (anti-persistent)

Applications in Real-World Scenarios

  • Finance: modeling stock prices, option pricing, portfolio optimization, risk management
    • Geometric Brownian motion for stock price dynamics (Black-Scholes model)
    • Stochastic volatility models (Heston model) for time-varying volatility
    • Lévy processes for modeling jumps and heavy-tailed distributions in asset returns
  • Queueing theory: analyzing waiting lines and service systems in operations research
    • M/M/1 queue: Poisson arrivals, exponential service times, single server
    • M/M/c queue: Poisson arrivals, exponential service times, cc parallel servers
    • M/G/1 queue: Poisson arrivals, general service time distribution, single server
  • Reliability engineering: modeling the failure and repair of complex systems
    • Alternating renewal process for a system with exponential failure and repair times
    • Non-homogeneous Poisson process for modeling time-varying failure rates (bathtub curve)
  • Epidemiology: modeling the spread of infectious diseases in a population
    • SIR (Susceptible-Infected-Recovered) model as a continuous-time Markov chain
    • Branching processes for modeling the early stages of an epidemic
  • Machine learning: Gaussian processes for regression and classification
    • Kriging (Gaussian process regression) for spatial interpolation and surrogate modeling
    • Gaussian process classification for binary or multi-class classification problems

Advanced Topics and Extensions

  • Martingales and their applications in stochastic calculus and financial mathematics
    • Doob's optional stopping theorem for the expected value of a stopped martingale
    • Azuma-Hoeffding inequality for concentration bounds on martingales with bounded differences
  • Stochastic differential equations (SDEs) for modeling continuous-time stochastic processes driven by Brownian motion
    • Itô's lemma for computing the differential of a function of a stochastic process
    • Girsanov's theorem for changing the probability measure of an SDE
    • Feynman-Kac formula for solving certain partial differential equations using SDEs
  • Lévy processes as generalizations of Brownian motion with jumps
    • Poisson process, compound Poisson process, and gamma process as examples of Lévy processes
    • Lévy-Khintchine formula for the characteristic function of a Lévy process
    • Subordinators as increasing Lévy processes used for time-changing other stochastic processes
  • Stochastic calculus for jump processes and its applications
    • Itô's formula for jump processes, extending Itô's lemma to include jump terms
    • Stochastic differential equations driven by Lévy processes
    • Applications in finance (jump-diffusion models) and insurance mathematics (risk processes)
  • Measure-valued processes and their applications in population genetics and statistical physics
    • Fleming-Viot process for modeling allele frequencies in a population under genetic drift and mutation
    • Dawson-Watanabe process (or super-process) for modeling branching populations with spatial structure
    • Interacting particle systems (voter model, contact process) for modeling the spread of opinions or infections on a lattice


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AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.