Basics on large deviations
In this chapter we introduce some general theorems on large deviations which
will be frequently used in this book. In most of the cases, the state space we deal
with is the real line. Indeed, a substantial portion of the discussion is limited to the
random variables taking non-negative values. Sometimes, the underlying stochastic
processes are sub-additive (see Section 1.3). Unlike most textbooks on this subject,
we put more attention on the tail probability
P{Yn λ}
than the probability of the form
P{Yn A}.
The unique structure of the models we deal with in this book requires some non-
conventional treatments. The topics we chose in this chapter reflect this demand.
As a consequence, most theorems introduced in Section 1.2 and in Section 1.3 are
non-standard and are not usually seen in the textbooks on large deviations.
1.1. artner-Ellis theorem
In the area of large deviations, we are concerned about asymptotic computation
of small probabilities on an exponential scale. The general form of large deviation
can be roughly described as
P{Yn A} exp{−bnI(A)} (n ∞)
for a random sequence {Yn}, a positive sequence {bn} with bn ∞, and a coeffi-
cient I(A) 0. In the application, we are often concerned with the probability that
the random variable(s) takes large values. Since the remarkable works by Donsker
and Varadhan (and others) in the 1970s and 1980s, this area has developed into a
relatively complete system. There have been several standard approaches in dealing
with large deviation problems. Perhaps the most useful tool is the G¨artner-Ellis
We have no intention to state the large deviation theory in its full generality.
Let {Yn} be a sequence of real random variables and let {bn} be a positive sequence
such that bn −→ ∞.
Assumption 1.1.1. For each θ R, the logarithmic moment generating function
Λ(θ), defined as the limit
(1.1.1) Λ(θ) = lim
log E exp θbnYn θ R
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