The Stein solution for the Poisson law #
For a rate r > 0 and an event A ⊆ ℕ, steinSolution r A solves the Poisson Stein equation
r f(w + 1) - w f(w) = 1_A(w) - Po(r)(A) for every w : ℕ,
and is bounded by one in absolute value. Writing F = P(Z ≤ w), T = P(Z > w) and
p_w = P(Z = w) for Z ~ Po(r), the explicit numerator is bounded by F T, and
F T ≤ r p_w follows from the head bound (r - w) F ≤ r p_w and the tail bound
(w + 1 - r) T ≤ r p_w, both consequences of the recursion (k + 1) p_{k+1} = r p_k.
This is the analytic input to the Arratia–Goldstein–Gordon Chen–Stein bound
(Proposition prop:AGG of the source); it is the crude Stein factor ‖f‖ ≤ 1 and not the
sharper factors of AGG89.
Head bound: (r - w) P(Z ≤ w) ≤ r P(Z = w) for Z ~ Po(r).
P(Z ≤ w) P(Z > w) ≤ r P(Z = w) for Z ~ Po(r).
The numerator of the Stein solution is bounded by P(Z ≤ w) P(Z > w).
The Stein solution of r f(w+1) - w f(w) = 1_A(w) - Po(r)(A), normalized by f 0 = 0.
Equations
- One or more equations did not get rendered due to their size.
- PoissonDeclumping.ChenStein.steinSolution r A 0 = 0
Instances For
The Stein solution is bounded by one.
The Stein equation: r f(w+1) - w f(w) = 1_A(w) - Po(r)(A) for every w : ℕ.
Increments of the Stein solution are bounded by two.
Stein identity for the Poisson law: E[r f(Z+1) - Z f(Z)] = 0 for Z ~ Po(r) and any
bounded f. (Not needed for the Chen–Stein bound itself, which only uses the Stein equation
pointwise.)