Doob decomposition theorem: Difference between revisions

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Template:Short description In the theory of stochastic processes in discrete time, a part of the mathematical theory of probability, the Doob decomposition theorem gives a unique decomposition of every adapted and integrable stochastic process as the sum of a martingale and a predictable process (or "drift") starting at zero. The theorem was proved by and is named for Joseph L. Doob.[1]

The analogous theorem in the continuous-time case is the Doob–Meyer decomposition theorem.

Statement

Let (Ω,,) be a probability space, Template:Math with N or I=0 a finite or countably infinite index set, (n)nI a filtration of , and Template:Math an adapted stochastic process with Template:Math for all Template:Math. Then there exist a martingale Template:Math and an integrable predictable process Template:Math starting with Template:Math such that Template:Math for every Template:Math. Here predictable means that Template:Math is n1-measurable for every Template:Math. This decomposition is almost surely unique.[2][3][4]

Remark

The theorem is valid word for word also for stochastic processes Template:Math taking values in the Template:Math-dimensional Euclidean space d or the complex vector space d. This follows from the one-dimensional version by considering the components individually.

Proof

Existence

Using conditional expectations, define the processes Template:Math and Template:Math, for every Template:Math, explicitly by

Template:NumBlk

and

Template:NumBlk

where the sums for Template:Math are empty and defined as zero. Here Template:Math adds up the expected increments of Template:Math, and Template:Math adds up the surprises, i.e., the part of every Template:Math that is not known one time step before. Due to these definitions, Template:Math (if Template:Math) and Template:Math are Template:Math-measurable because the process Template:Math is adapted, Template:Math and Template:Math because the process Template:Math is integrable, and the decomposition Template:Math is valid for every Template:Math. The martingale property

𝔼[MnMn1|n1]=0    a.s.

also follows from the above definition (Template:EquationNote), for every Template:Math}.

Uniqueness

To prove uniqueness, let Template:Math be an additional decomposition. Then the process Template:Math is a martingale, implying that

𝔼[Yn|n1]=Yn1    a.s.,

and also predictable, implying that

𝔼[Yn|n1]=Yn    a.s.

for any Template:Math}. Since Template:Math by the convention about the starting point of the predictable processes, this implies iteratively that Template:Math almost surely for all Template:Math, hence the decomposition is almost surely unique.

Corollary

A real-valued stochastic process Template:Math is a submartingale if and only if it has a Doob decomposition into a martingale Template:Math and an integrable predictable process Template:Math that is almost surely increasing.[5] It is a supermartingale, if and only if Template:Math is almost surely decreasing.

Proof

If Template:Math is a submartingale, then

𝔼[Xk|k1]Xk1    a.s.

for all Template:Math}, which is equivalent to saying that every term in definition (Template:EquationNote) of Template:Math is almost surely positive, hence Template:Math is almost surely increasing. The equivalence for supermartingales is proved similarly.

Example

Let Template:Math be a sequence in independent, integrable, real-valued random variables. They are adapted to the filtration generated by the sequence, i.e. Template:Math for all Template:Math. By (Template:EquationNote) and (Template:EquationNote), the Doob decomposition is given by

An=k=1n(𝔼[Xk]Xk1),n0,

and

Mn=X0+k=1n(Xk𝔼[Xk]),n0.

If the random variables of the original sequence Template:Math have mean zero, this simplifies to

An=k=0n1Xk    and    Mn=k=0nXk,n0,

hence both processes are (possibly time-inhomogeneous) random walks. If the sequence Template:Math consists of symmetric random variables taking the values Template:Math and Template:Math, then Template:Math is bounded, but the martingale Template:Math and the predictable process Template:Math are unbounded simple random walks (and not uniformly integrable), and Doob's optional stopping theorem might not be applicable to the martingale Template:Math unless the stopping time has a finite expectation.

Application

In mathematical finance, the Doob decomposition theorem can be used to determine the largest optimal exercise time of an American option.[6][7] Let Template:Math denote the non-negative, discounted payoffs of an American option in a Template:Math-period financial market model, adapted to a filtration Template:Math, and let Template:Math denote an equivalent martingale measure. Let Template:Math denote the Snell envelope of Template:Math with respect to . The Snell envelope is the smallest Template:Math-supermartingale dominating Template:Math[8] and in a complete financial market it represents the minimal amount of capital necessary to hedge the American option up to maturity.[9] Let Template:Math denote the Doob decomposition with respect to of the Snell envelope Template:Math into a martingale Template:Math and a decreasing predictable process Template:Math with Template:Math. Then the largest stopping time to exercise the American option in an optimal way[10][11] is

τmax:={Nif AN=0,min{n{0,,N1}An+1<0}if AN<0.

Since Template:Math is predictable, the event Template:Math} is in Template:Math for every Template:Math}, hence Template:Math is indeed a stopping time. It gives the last moment before the discounted value of the American option will drop in expectation; up to time Template:Math the discounted value process Template:Math is a martingale with respect to .

Generalization

The Doob decomposition theorem can be generalized from probability spaces to σ-finite measure spaces.[12]

Citations

Template:Reflist

References

Template:Stochastic processes