Elements of Queueing Theory Ib: Ergodicity and Stochastic IntensityTextbook
Ergodicity and Stochastic Intensity
Background
Chapter 1 of Baccelli and Brémaud's Elements of Queueing Theory has two halves. The first builds
Palm calculus from the Matthes definition of P⁰_N and reaches the Swiss army formula. This
mission is the second: §§1.6, 1.8 and 1.9, which supply the two things the rest of the book runs
on.
Ergodic theory, quoted
§1.6 states, in its own words, "the ergodic theory results to be used later in this book". Five of them, and the book proves none: Birkhoff's pointwise ergodic theorem in discrete (Theorem 1.6.1) and continuous time (Theorem 1.6.4), Kingman's sub-additive ergodic theorem (Theorem 1.6.2), and the extremal characterizations of ergodicity in both settings (Theorems 1.6.3 and 1.6.5) — ergodicity is exactly the impossibility of splitting an invariant probability into two distinct ones.
They are quoted, but they are not decoration. Kingman's theorem is what produces the asymptotic
growth rates of Theorem 2.11.2 and the constant γ(c) on which the saturation rule rests.
Birkhoff's theorem is what makes the time average in PASTA's (3.3.2) a well-defined object, and
what the fluid Loynes theorem invokes for lim_{u→−∞}(A_{u,0} − C_{u,0}) = −∞.
None of the three analytic ones exists in Mathlib. Analysis/InnerProductSpace/MeanErgodic is the
mean (von Neumann, L²) theorem, not almost-everywhere convergence, and there is no sub-additive
ergodic theorem at all. The platform has neither.
Predictability, and why PASTA can be stated
§1.8 introduces the stochastic intensity: a point process N admits the (P, F_t)-intensity
{λ(t)} when E[N(a,b] 1_A] = E[(∫_a^b λ(t)dt) 1_A] for A ∈ F_a. Around it sits the notion of a
predictable process — one measurable with respect to the strict past.
Theorem 1.8.1 is the structural fact that makes predictability usable. For the internal history of a marked point process, every predictable process has the concrete form
Z(t, ω) = v(t, θ_t ω), v(t, ·) F_{0−}-measurable. (1.8.1)
That is why mission IV can take this form as PASTA's hypothesis rather than constructing a predictable σ-field: Theorem 1.8.1 says nothing is lost.
The goal
Theorem 1.8.2 (p.61), §1.8.4, Watanabe's characterization of Poisson processes. For a
history F_t = F_t^N ∨ G and a G-measurable, locally integrable {λ(t)}, if N admits the
F_t-intensity {λ(t)} then N is a G-conditional Poisson process:
E[ e^{iuN(a,b]} | G ∨ F^N_a ] = exp{ (e^{iu} − 1) ∫_a^b λ(t) dt } . (1.8.12)
A stochastic intensity that carries no information beyond G forces the process to be Poisson
conditionally on G, with the compensator as the parameter — and the conditional characteristic
function is the exact Poisson one, not an approximation. With G trivial and λ constant this is
the ordinary Poisson process, which is the equivalence Remark 3.3.1 of Chapter 3 invokes to explain
the name PASTA. The book: "This result plays a role in queueing theory, especially for proving
that some streams in a queueing network are or are not Poissonian."
Palm probability meets stochastic intensity
§1.9 asks whether the stochastic intensity is the same under P and under P⁰_N — whether the
two probabilities describe the same dynamics. Theorem 1.9.1 says yes, on ℝ₊: the same process
{λ(t)} serves both.
Theorem 1.9.2 is Papangelou's theorem, and it is the deepest statement of the section: N
admits a stochastic intensity if and only if P⁰_N ≪ P on F_{0−}, and then
λ(t) = (μ ∘ θ_t)λ with μ the Radon–Nikodým derivative. A dynamic property and a static one turn
out to be the same thing.
Theorem 1.9.3 is Mecke's characterization: N is Poisson exactly when P ≡ P⁰_N on
F_{0−}. The view from a point of the process and the view from a deterministic instant agree on
the strict past precisely when the process has no memory. It follows in one line from the two
theorems before it.
What this mission provides
Four of the five missions in this series import the Chapter 1 substrate; this one adds the two pieces they need from its second half — ergodic theory and the stochastic intensity. Nothing here is on the platform, and Mathlib has filtrations and adapted processes but no predictability in this form, no stochastic intensity, no pointwise ergodic theorem and no Kingman.
Formalization scope
Every result is stated in the book's strength, with the book's standing definitions as binders.
A discrete flow is a bijective, measurable, P⁰-preserving map (p.46); a continuous flow is jointly
measurable in (t, ω) (p.3, clause (a)). A history compatible with the flow satisfies
θ_t F_s = F_{s−t} (p.57), and an F_t-intensity is a non-negative, measurable, locally
integrable, adapted process (p.58). The limits of Theorems 1.6.1, 1.6.2 and 1.6.4 are asserted to
exist; Kingman's constant h̄ lies in ℝ ∪ {−∞} and is identified with
inf_n (1/n) E⁰[h_n], the means being extended reals so that E⁰[h_n] = −∞ is not read as 0.
Theorems 1.6.3, 1.6.5, 1.9.2 and 1.9.3 are equivalences, and Theorem 1.9.2 carries the closed form
λ(t) = (μ ∘ θ_t)λ with μ = dP⁰_N/dP on F_{0−}. The goal's conclusion is the exact conditional
characteristic function (1.8.12); a formalization that only asserted some conditional Poisson law,
or conditioned on G alone, would not be this theorem.