Incomplete Cholesky factorization

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In mathematics, Doob's martingale inequality is a result in the study of stochastic processes. It gives a bound on the probability that a stochastic process exceeds any given value over a given interval of time. As the name suggests, the result is usually given in the case that the process is a non-negative martingale, but the result is also valid for non-negative submartingales.

The inequality is due to the American mathematician Joseph L. Doob.

Statement of the inequality

Let X be a submartingale taking non-negative real values, either in discrete or continuous time. That is, for all times s and t with s < t,

E[Xt|s]Xs.

(For a continuous-time submartingale, assume further that the process is càdlàg.) Then, for any constant C > 0 and p ≥ 1,

P[sup0tTXtC]E[XTp]Cp.

In the above, as is conventional, P denotes the probability measure on the sample space Ω of the stochastic process

X:[0,T]×Ω[0,+)

and E denotes the expected value with respect to the probability measure P, i.e. the integral

E[XT]=ΩXT(ω)dP(ω)

in the sense of Lebesgue integration. s denotes the σ-algebra generated by all the random variables Xi with i ≤ s; the collection of such σ-algebras forms a filtration of the probability space.

Further inequalities

There are further (sub)martingale inequalities also due to Doob. With the same assumptions on X as above, let

St=sup0stXs,

and for p ≥ 1 let

Xtp=XtLp(Ω,,P)=(E[|Xt|p])1p.

In this notation, Doob's inequality as stated above reads

P[STC]XTppCp.

The following inequalities also hold: for p = 1,

STpee1(1+XTlogXTp)

and, for p > 1,

XTpSTppp1XTp.

Related inequalities

Doob's inequality for discrete-time martingales implies Kolmogorov's inequality: if X1, X2, ... is a sequence of real-valued independent random variables, each with mean zero, it is clear that

E[X1++Xn+Xn+1|X1,,Xn]=X1++Xn+E[Xn+1|X1,,Xn]=X1++Xn,

so Mn = X1 + ... + Xn is a martingale. Note that Jensen's inequality implies that |Mn| is a nonnegative submartingale if Mn is a martingale. Hence, taking p = 2 in Doob's martingale inequality,

P[max1in|Mi|λ]E[Mn2]λ2,

which is precisely the statement of Kolmogorov's inequality.

Application: Brownian motion

Let B denote canonical one-dimensional Brownian motion. Then

P[sup0tTBtC]exp(C22T).

The proof is just as follows: since the exponential function is monotonically increasing, for any non-negative λ,

{sup0tTBtC}={sup0tTexp(λBt)exp(λC)}.

By Doob's inequality, and since the exponential of Brownian motion is a positive submartingale,

P[sup0tTBtC]=P[sup0tTexp(λBt)exp(λC)]E[exp(λBT)]exp(λC)=exp(12λ2TλC)E[exp(λBt)]=exp(12λ2t)

Since the left-hand side does not depend on λ, choose λ to minimize the right-hand side: λ = C/T gives the desired inequality.

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