Chapter Summary

Chapter 13 Summary: Introduction to Stochastic Processes

Key Points

  • 1.

    A stochastic process {X(t):t∈T}\{X(t) : t \in \mathcal{T}\} is a family of random variables indexed by time. It is fully characterized by its finite-dimensional distributions (fdds), which must satisfy Kolmogorov's consistency conditions.

  • 2.

    Strict-sense stationarity (SSS) requires all fdds to be time-shift invariant. Wide-sense stationarity (WSS) requires only constant mean and lag-dependent autocorrelation β€” a much weaker and more practical condition.

  • 3.

    For Gaussian processes, WSS implies SSS (Lemma 43), because Gaussian distributions are fully determined by their first two moments.

  • 4.

    The autocorrelation rXX(Ο„)r_{XX}(\tau) of a WSS process satisfies: rXX(0)=r_{XX}(0) = average power, rXX(Ο„)=rXXβˆ—(βˆ’Ο„)r_{XX}(\tau) = r_{XX}^*(-\tau) (Hermitian symmetry), ∣rXX(Ο„)βˆ£β‰€rXX(0)|r_{XX}(\tau)| \leq r_{XX}(0) (maximum at origin), and non-negative definiteness.

  • 5.

    The cross-correlation rXY(Ο„)r_{XY}(\tau) measures the linear dependence between two jointly WSS processes. For an LTI system, rYX[k]=(hβˆ—rXX)[k]r_{YX}[k] = (h * r_{XX})[k].

  • 6.

    Ergodicity ensures that time averages converge to ensemble averages. The sufficient condition for mean-ergodicity is cXX(Ο„)β†’0c_{XX}(\tau) \to 0 as βˆ£Ο„βˆ£β†’βˆž|\tau| \to \infty.

  • 7.

    These second-order tools β€” autocorrelation, cross-correlation, and the WSS/ergodicity framework β€” are the foundation for the power spectral density (Chapter 14), LTI system analysis (Chapter 15), and mean-square calculus (Chapter 16).

Looking Ahead

In Chapter 14, we introduce the power spectral density β€” the Fourier transform of the autocorrelation β€” which transforms the correlation-domain analysis of this chapter into the frequency domain. The Wiener-Khintchine theorem establishes the fundamental link, and the frequency-domain viewpoint enables the design of optimal filters (matched filter, Wiener filter) in Chapter 15.