Contraction principle (large deviations theory)

In mathematics — specifically, in large deviations theory — the contraction principle is a theorem that states how a large deviation principle on one space "pushes forward" to a large deviation principle on another space via a continuous function.

Statement of the theorem

Let X and Y be Hausdorff topological spaces and let (μ_ε)_ε>0 be a family of probability measures on X that satisfies the large deviation principle with rate function I : X → [0, +∞]. Let T : X → Y be a continuous function, and let ν_ε = T_∗(μ_ε) be the push-forward measure of μ_ε by T, i.e., for each measurable set/event E ⊆ Y, ν_ε(E) = μ_ε(T⁻¹(E)). Let

$J(y):=\inf {\big \{}I(x){\big |}x\in X{\mbox{ and }}T(x)=y{\big \}},$

with the convention that the infimum of I over the empty set ∅ is +∞. Then:

• J : Y → [0, +∞] is a rate function on Y,
• J is a good rate function on Y if I is a good rate function on X, and
• (ν_ε)_ε>0 satisfies the large deviation principle on Y with rate function J.

References

• Dembo, Amir (1998). Large deviations techniques and applications. Applications of Mathematics (New York) 38 (Second edition ed.). New York: Springer-Verlag. pp. xvi+396. ISBN 0-387-98406-2. MR 1619036. {{cite book}}: |edition= has extra text (help); Unknown parameter |coauthors= ignored (|author= suggested) (help) (See chapter 4.2.1)
• den Hollander, Frank (2000). Large deviations. Fields Institute Monographs 14. Providence, RI: American Mathematical Society. pp. x+143. ISBN 0-8218-1989-5. MR 1739680.