Schilder's theorem

Schilder's theorem

In mathematics, Schilder's theorem is a result in the large deviations theory of stochastic processes. Roughly speaking, Schilder's theorem gives an estimate for the probability that a (scaled-down) sample path of Brownian motion will stray far from the mean path (which is constant with value 0). This statement is made precise using rate functions. Schilder's theorem is generalized by the Freidlin-Wentzell theorem for Itō diffusions.

tatement of the theorem

Let "B" be a standard Brownian motion in "d"-dimensional Euclidean space R"d" starting at the origin, 0 ∈ R"d"; let W denote the law of "B", i.e. classical Wiener measure. For "ε" > 0, let W"ε" denote the law of the rescaled process (√"ε")"B". Then, on the Banach space "C"0 = "C"0( [0, "T"] ; R"d") with the supremum norm ||·||∞, the probability measures W"ε" satisfy the large deviations principle with good rate function "I" : "C"0 → R ∪ {+∞} given by

:I(omega) = frac{1}{2} int_{0}^{T} | dot{omega}(t) |^{2} , mathrm{d} t

if "ω" is absolutely continuous, and "I"("ω") = +∞ otherwise. In other words, for every open set "G" ⊆ "C"0 and every closed set "F" ⊆ "C"0,

:limsup_{varepsilon downarrow 0} varepsilon log mathbf{W}_{varepsilon} (F) leq - inf_{omega in F} I(omega)

and

:liminf_{varepsilon downarrow 0} varepsilon log mathbf{W}_{varepsilon} (G) geq - inf_{omega in G} I(omega).

Example

Taking "ε" = 1 ⁄ "c"2, one can use Schilder's theorem to obtain estimates for the probability that a standard Brownian motion "B" strays further than "c" from its starting point over the time interval [0, "T"] , i.e. the probability

:mathbf{W} (C_{0} setminus mathbf{B}_{c} (0; | cdot |_{infty})) equiv mathbf{P} ig [ | B |_{infty} > c ig] ,

as "c" tends to infinity. Here B"c"(0; ||·||∞) denotes the open ball of radius "c" about the zero function in "C"0, taken with respect to the supremum norm. First note that

:| B |_{infty} > c iff sqrt{varepsilon} B in A := ig{ omega in C_{0} ig| | omega(t) | > 1 mbox{ for some } t in [0, T] ig}.

Since the rate function is continuous on "A", Schilder's theorem yields

:lim_{c o infty} frac{1}{c^{2 log mathbf{P} ig [ | B |_{infty} > c ig] ::= lim_{varepsilon o 0} epsilon mathbf{P} ig [ sqrt{varepsilon} B in A ig] ::= - inf left{ left. frac{1}{2} int_{0}^{T} | dot{omega}(t) |^{2} , mathrm{d} t ight| omega in A ight}::= - frac{1}{2} int_{0}^{T} frac{1}{T^{2 , mathrm{d} t::= - frac{1}{2 T},

making use of the fact that the infimum over paths in the collection "A" is attained for "ω"("t") = "t" ⁄ "T". This result can be heuristically interpreted as saying that, for large "c" and/or large "T"

:frac{1}{c^{2 log mathbf{P} ig [ | B |_{infty} > c ig] approx - frac{1}{2 T},

or, in other words,

:mathbf{P} ig [ | B |_{infty} > c ig] approx exp left( - frac{c^{2{2 T} ight).

In fact, the above probability can be estimated more precisely as follows: for "B" a standard Brownian motion in R"n", and any "T", "c" and "ε" > 0, it holds that

:mathbf{P} left [ sup_{0 leq t leq T} ig| sqrt{varepsilon} B_{t} ig| geq c ight] leq 4 n exp left( - frac{c^{2{2 n T varepsilon} ight).

References

* cite book
last= Dembo
first = Amir
coauthors = Zeitouni, Ofer
title = Large deviations techniques and applications
series = Applications of Mathematics (New York) 38
edition = Second edition
publisher = Springer-Verlag
location = New York
year = 1998
pages = xvi+396
isbn = 0-387-98406-2
MathSciNet|id=1619036 (See theorem 5.2)


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