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📐 Advanced Quantitative Stochastic Calculus & Non-Markovian Microstructure Suite

Author: Ramprasad Atluri
Affiliation: Quantitative Research & Advanced Econometric Architectures
License: MIT License


1. Merton Compound Poisson Jump-Diffusion Model

The underlying asset price $S_t$ satisfies the jump-diffusion stochastic differential equation (SDE):

dStSt−=(μ−λκ)dt+σdWt+(Y−1)dNt\frac{dS_t}{S_{t-}} = (\mu - \lambda \kappa) dt + \sigma dW_t + (Y - 1) dN_t

Where:

  • $W_t$ is a standard standard Brownian motion on $(\Omega, \mathcal{F}, (\mathcal{F}_t), \mathbb{P})$.
  • $N_t$ is a homogeneous Poisson counting process with constant intensity $\lambda > 0$, independent of $W_t$.
  • $Y$ is a log-normal jump size distribution: $\ln Y \sim \mathcal{N}(\gamma, \delta^2)$.
  • $\kappa = \mathbb{E}[Y - 1] = \exp\left(\gamma + \frac{1}{2} \delta^2\right) - 1$ is the expected relative jump percentage, ensuring the compensated process is a $\mathbb{Q}$-martingale.

2. Fractional Brownian Motion & Detrended Fluctuation Analysis (DFA)

The fractional Brownian motion (fBM) $B_H(t)$ with Hurst index $H \in (0, 1)$ possesses covariance structure:

E[BH(t)BH(s)]=12(∣t∣2H+∣s∣2H−∣t−s∣2H)\mathbb{E}[B_H(t) B_H(s)] = \frac{1}{2} \left( |t|^{2H} + |s|^{2H} - |t - s|^{2H} \right)

Fractional Integration Properties:

  • $H > 1/2$: Non-Markovian long-range dependence, $\sum_{k=1}^\infty \gamma(k) = \infty$, exhibiting directional persistence.
  • $H = 1/2$: Classical Brownian motion with independent increments.
  • $H < 1/2$: Anti-persistent, negative autocorrelation, anomalous sub-diffusion.

The Detrended Fluctuation Analysis computes root-mean-square fluctuation $F(s)$ over window length $s$:

F(s)=1N∑k=1N(X(k)−pv(k))2∼sHF(s) = \sqrt{\frac{1}{N} \sum_{k=1}^N \left( X(k) - p_v(k) \right)^2} \sim s^H


3. Hawkes Self-Exciting Point Process

The conditional intensity function $\lambda(t)$ of high-frequency orderbook arrival events satisfies:

λ(t)=μ+∫0tαe−β(t−s)dN(s)=μ+∑ti<tαe−β(t−ti)\lambda(t) = \mu + \int_0^t \alpha e^{-\beta (t - s)} dN(s) = \mu + \sum_{t_i < t} \alpha e^{-\beta(t - t_i)}

Subcriticality Condition:

The spectral radius of the transition kernel satisfies the subcritical stability criterion:

η=αβ<1.0\eta = \frac{\alpha}{\beta} < 1.0

The total log-likelihood over interval $[0, T]$ is evaluated via exact recursion:

ln⁡L=∑i=1Nln⁡λ(ti)−μT−αβ∑i=1N(1−e−β(T−ti))\ln \mathcal{L} = \sum_{i=1}^N \ln \lambda(t_i) - \mu T - \frac{\alpha}{\beta} \sum_{i=1}^N \left( 1 - e^{-\beta(T - t_i)} \right)


4. Optimal Stopping via Longstaff-Schwartz LSM Dynamic Programming

Resolves the backward Snell envelope for early-exercise American contingent claims:

V(St,t)=max⁡{h(St), e−rΔtEQ[V(St+1,t+1)∣Ft]}V(S_t, t) = \max\left\{ h(S_t), \, e^{-r \Delta t} \mathbb{E}^\mathbb{Q} \left[ V(S_{t+1}, t+1) \mid \mathcal{F}_t \right] \right\}

The conditional continuation value $C(S_t) = \mathbb{E}^\mathbb{Q}[e^{-r \Delta t} V_{t+1} \mid S_t]$ is projected onto an orthogonal basis of weighted Laguerre polynomials ${L_k(x)}_{k=0}^M$:

C(St)≈∑k=0MβkLk(St),β=(X⊤X)−1X⊤YC(S_t) \approx \sum_{k=0}^M \beta_k L_k(S_t), \quad \boldsymbol{\beta} = (\mathbf{X}^\top \mathbf{X})^{-1} \mathbf{X}^\top \mathbf{Y}

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