Couplings and Poisson laws in total variation #
General total-variation facts used by the source (inventory item B15, source lines 1693–1696,
2115–2120 and 2392–2398), all in the paper's probability convention paperTVDist:
- the coupling bound
d_TV(L(X), L(Y)) ≤ P(X ≠ Y)and its monotone formd_TV(L(X), L(Y)) ≤ E[Y - X]forℕ-valuedX ≤ Y; d_TV(Po(a), Po(b)) ≤ 1 - exp (-|a - b|) ≤ |a - b|;- continuity of the Poisson law in its parameter, and the replacement of the Poisson parameter along a sequence when the parameters are asymptotically equal;
- the Poisson zero-mass bound
|P(N = 0) - exp (-a)| ≤ d_TV(L(N), Po(a)).
Coupling bound. Two random variables on the same probability space have laws whose
normalized total variation distance is at most the probability that they differ. The
disagreement event need not be measurable; Measure.real is then its outer measure.
Monotone coupling bound. If X ≤ Y almost surely are ℕ-valued random variables and
Y - X is integrable, then d_TV(L(X), L(Y)) ≤ E[Y - X]. This is the mechanism used for the
truncation in Lemma lem:truncate(i), source lines 1692–1693.
The Poisson law with rate zero is the Dirac mass at zero.
d_TV(Po(a), Po(b)) ≤ 1 - exp (-(b - a)) for a ≤ b, via the coupling X versus
X + Y with independent X ~ Po(a) and Y ~ Po(b - a).
d_TV(Po(a), Po(b)) ≤ 1 - exp (-|a - b|).
Poisson laws in total variation. d_TV(Po(a), Po(b)) ≤ |a - b|, as used at source
lines 1695 and 2115.
If the Poisson parameters are asymptotically equal, the Poisson laws merge in total variation.
Convergence of the Poisson parameter implies convergence of the Poisson laws in total variation.
Continuity of the Poisson law in its parameter, for normalized total variation.
Triangle inequality along a filter: total-variation convergence passes through an intermediate family of finite measures.
Replacing the Poisson parameter: if d_TV(L_n, Po(a_n)) → 0 and a_n - b_n → 0, then
d_TV(L_n, Po(b_n)) → 0 (source lines 2112–2119).
The Poisson zero mass is controlled by total variation:
|μ{0} - exp (-a)| ≤ d_TV(μ, Po(a)) (source lines 2392–2397).