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Compound Poisson Jumps

Updated 31 January 2026
  • Compound Poisson jumps are stochastic processes that sum independent and identically distributed jump sizes occurring at Poisson event times, forming a basic pure-jump Lévy process.
  • They are widely applied in financial modeling, risk theory, and ergodic control, characterized by stationary, independent increments and explicit moment formulations.
  • Recent research employs Bayesian, wavelet, and self-normalization techniques to effectively estimate jump intensities and decompound observed increments.

A compound Poisson jump process is a fundamental stochastic model in which random instantaneous changes (“jumps”) occur at Poisson event times, and each jump has a random size governed by an independent, identically distributed sequence. This framework underlies a large portion of the applied probability literature, including stochastic differential equations, rare-event large deviations, ergodic control, financial modeling, and fractional generalizations. The compound Poisson process serves both as a prototypical example of a pure-jump Lévy process and as a building block in more complex jump-diffusion or time-changed models.

1. Definition and Basic Properties

Let NtN_t be a Poisson process of rate λ>0\lambda>0 and {Yi}i1\{Y_i\}_{i\ge1} an i.i.d. sequence of random variables, independent of NN. The classic compound Poisson process is defined as

Xt=i=1NtYi.X_t = \sum_{i=1}^{N_t} Y_i .

The corresponding infinitesimal generator, moment generating function, and characteristic function are

E[euXt]=exp{λt[E[euY1]1]},E[eiθXt]=exp{λt[E[eiθY1]1]}.\mathbb{E}[e^{u X_t}] = \exp\bigl\{ \lambda t [\mathbb{E}[e^{uY_1}]-1] \bigr\},\quad \mathbb{E}[e^{i\theta X_t}] = \exp\bigl\{ \lambda t [\mathbb{E}[e^{i\theta Y_1}]-1] \bigr\}.

If YiY_i are nonnegative and Lebesgue absolutely continuous with density ff, the process is used to model aggregated random shocks or claims in risk processes, queueing, and insurance applications (Crescenzo et al., 2015).

Key properties:

  • Stationarity and independence of increments: Xt+sXtX_{t+s}-X_t is independent of the filtration up to tt and has the same law as XsX_s.
  • Lévy process: XtX_t is a finite-activity pure-jump Lévy process.
  • Moments: E[Xt]=λtE[Y1]\mathbb{E}[X_t] = \lambda t\,\mathbb{E}[Y_1], Var[Xt]=λtE[Y12]\mathrm{Var}[X_t] = \lambda t\,\mathbb{E}[Y_1^2].

If λ\lambda or the law of YiY_i is state-dependent, a "compound Poisson process with state-dependent rate" arises (Hongler et al., 2016).

2. Master Equations and Fractional Extensions

Consider an SDE with a compound Poisson jump term: dXt=b(Xt)dt+σ(Xt)dWt+dJtdX_t = b(X_{t-})\,dt + \sigma(X_{t-})\,dW_t + dJ_t where Jt=i=1NtZiJ_t=\sum_{i=1}^{N_t} Z_i and WtW_t is Brownian motion. The forward Kolmogorov (Master) equation for the density P(x,t)P(x,t) involves gain–loss terms reflecting the jump structure: Pt=x(bP)+122x2(σ2P)λP(x,t)+φ(y)λP(xy,t)dy.\frac{\partial P}{\partial t} = -\frac{\partial}{\partial x}(bP) + \frac{1}{2}\frac{\partial^2}{\partial x^2}(\sigma^2 P) - \lambda P(x,t) + \int \varphi(y) \lambda P(x-y,t) dy . For special jump distributions, the integro-differential equation can reduce to a higher-order PDE (e.g., Erlang-distributed jumps yield a spatial mm-th order PDE) (Hongler et al., 2016).

Fractional generalizations involve time-changing with inverse subordinators Ef(t)E_f(t), yielding the Generalized Fractional Compound Poisson Process (GFCPP): Yf(t)=i=1N(Ef(t))XiY_f(t) = \sum_{i=1}^{N(E_f(t))} X_i governed by a fractional Kolmogorov–Feller equation with a generalized Caputo–Džrbašjan derivative: Dtfpn(t)=λpn(t)+λk0pnk(t)FX({k}).\mathcal{D}^f_t p_n(t) = -\lambda p_n(t) + \lambda \sum_{k\ge0} p_{n-k}(t) F_X^{*}(\{k\}) . Special cases cover Mittag–Leffler, discrete uniform, geometric, and negative-binomial jump distributions (Gupta et al., 2023).

3. Estimation and Decompounding

The decompounding problem asks for the recovery of intensity λ\lambda and jump law ff from discretely observed increments.

  • Bayesian Approach: Latent count augmentation and Markov Chain Monte Carlo are used for nonparametric νk=λpk\nu_k = \lambda p_k estimation (Gugushvili et al., 2019).
  • Wavelet Methods: Adaptive wavelet thresholding estimates convolution powers of the observed mixture density, and inversion formulas reconstruct ff, achieving minimax rates under certain sampling regimes (Duval, 2012).
  • Self-normalization for SDEs: For ergodic diffusions with Poisson jumps, iterative jump-removal based on self-normalized Euler residuals and the Jarque–Bera statistic provides tuning-free, efficient estimators for the diffusion parameters, adapting to unknown volatility (Masuda et al., 2018).

4. Functional Analysis and Limit Theorems

Key results on distribution tails, functionals, and performance in heavy-tailed or high-intensity regimes include:

  • Uniform Large Deviations: For compound Poisson processes with regularly varying jumps (P[J>x]L(x)xα\mathbb{P}[J>x] \sim L(x) x^{-\alpha}), the tail of the supremum and functionals such as time to ruin exhibit asymptotics driven by the jump tail, robust uniformly in near-critical vanishing drift (Kamphorst et al., 2015).
  • Ornstein–Uhlenbeck with Compound Poisson Jumps: Passage times, ruin probabilities, and undershoots are characterized using partial eigenfunctions and contour integration, with explicit Laplace transform formulas and sharp asymptotics (Rønn-Nielsen, 2016).
  • Central Limit and Law of Large Numbers: For finite mean and variance, X(t)/tμ=λEYX(t)/t \to \mu = \lambda \mathbb{E} Y a.s., and the fluctuations are asymptotically Gaussian; in high-intensity limits, scaling yields convergence to Brownian motion (Cinque et al., 10 Apr 2025).

5. Applied and Generalized Settings

Compound Poisson jumps are core in models for finance, control, and beyond:

  • Time-Changed Lévy Models in Finance: Option pricing under time-changed Brownian motion with compound Poisson jumps (e.g., variance gamma, normal inverse Gaussian) leads to explicit and quasi-explicit formulas, tractable via conditioning and static hedging arguments (Ivanov et al., 2020).
  • Ergodic Control: Stochastic control of jump–diffusion systems with compound Poisson noise is fully characterized by the ergodic HJB equation, with pathwise optimality and fine value function regularity under Lyapunov-type structural assumptions (Arapostathis et al., 2019).
  • Prediction Problems: For Gaussian Volterra processes perturbed by compound Poisson jumps, full conditional distributions and prediction laws follow by leveraging independence and additive decomposition, yielding explicit future-forecast statistics (Almani et al., 2023).
  • Co-integrated Multivariate Models: Cointegration of dependent Poisson processes induces spread pricing frameworks in energy and commodities, with explicit dependence captured by self-decomposable random variables (Petroni et al., 2015).

6. Rare-Event Simulation and Extreme-Value Regimes

In heavy-tailed settings, rare events frequently result from one or several large jumps:

  • Sample-Path Large Deviations: Precise asymptotic rates for rare events are available via the sample-path large deviations principle, identifying the minimal “big-jump” structure required for a given rare event (Chen et al., 2017).
  • Strongly Efficient Estimators: Importance sampling strategies that specifically bias toward rare multiple-jump realizations admit provably bounded relative error and are effective across rare-event regimes, including insurance ruin, option barriers, and queue overflows (Chen et al., 2017).

7. Special Constructions and Bell Polynomial Expansions

Time-randomization and iteration yield further classes:

  • CPP with Poisson Subordinator: If a CPP is evaluated at Poisson times, closed-form distribution representations result in mixtures characterized by Bell polynomials. Exponential and normal jump cases furnish explicit formulas for densities, moments, and characteristic exponents. The so-called “iterated Poisson process” exhibits convergence to a Poisson process under appropriate scaling (Crescenzo et al., 2015).
  • Skellam-Type and Multivariate Compound Poisson: The Skellam process and its generalizations—sums of signed jumps at Poisson times—admit exact CPP representations and clean characterizations of limiting/Gaussian behavior and discrete-time approximations (Cinque et al., 10 Apr 2025).

References:

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