Doob decomposition theorem

Mathematical theorem in stochastic processes

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 , F , P ) {\displaystyle (\Omega ,{\mathcal {F}},\mathbb {P} )} be a probability space, I = {0, 1, 2, ..., N} with N N {\displaystyle N\in \mathbb {N} } or I = N 0 {\displaystyle I=\mathbb {N} _{0}} a finite or countably infinite index set, ( F n ) n I {\displaystyle ({\mathcal {F}}_{n})_{n\in I}} a filtration of  F {\displaystyle {\mathcal {F}}} , and X = (Xn)nI an adapted stochastic process with E[|Xn|] < ∞ for all nI. Then there exist a martingale M = (Mn)nI and an integrable predictable process A = (An)nI starting with A0 = 0 such that Xn = Mn + An for every nI. Here predictable means that An is F n 1 {\displaystyle {\mathcal {F}}_{n-1}} -measurable for every nI \ {0}. This decomposition is almost surely unique.[2][3][4]

Remark

The theorem is valid word for word also for stochastic processes X taking values in the d-dimensional Euclidean space R d {\displaystyle \mathbb {R} ^{d}} or the complex vector space C d {\displaystyle \mathbb {C} ^{d}} . This follows from the one-dimensional version by considering the components individually.

Proof

Existence

Using conditional expectations, define the processes A and M, for every nI, explicitly by

A n = k = 1 n ( E [ X k | F k 1 ] X k 1 ) {\displaystyle A_{n}=\sum _{k=1}^{n}{\bigl (}\mathbb {E} [X_{k}\,|\,{\mathcal {F}}_{k-1}]-X_{k-1}{\bigr )}}

(1)

and

M n = X 0 + k = 1 n ( X k E [ X k | F k 1 ] ) , {\displaystyle M_{n}=X_{0}+\sum _{k=1}^{n}{\bigl (}X_{k}-\mathbb {E} [X_{k}\,|\,{\mathcal {F}}_{k-1}]{\bigr )},}

(2)

where the sums for n = 0 are empty and defined as zero. Here A adds up the expected increments of X, and M adds up the surprises, i.e., the part of every Xk that is not known one time step before. Due to these definitions, An+1 (if n + 1 ∈ I) and Mn are Fn-measurable because the process X is adapted, E[|An|] < ∞ and E[|Mn|] < ∞ because the process X is integrable, and the decomposition Xn = Mn + An is valid for every nI. The martingale property

E [ M n M n 1 | F n 1 ] = 0 {\displaystyle \mathbb {E} [M_{n}-M_{n-1}\,|\,{\mathcal {F}}_{n-1}]=0}     a.s.

also follows from the above definition (2), for every nI \ {0}.

Uniqueness

To prove uniqueness, let X = M' + A' be an additional decomposition. Then the process Y := MM' = A'A is a martingale, implying that

E [ Y n | F n 1 ] = Y n 1 {\displaystyle \mathbb {E} [Y_{n}\,|\,{\mathcal {F}}_{n-1}]=Y_{n-1}}     a.s.,

and also predictable, implying that

E [ Y n | F n 1 ] = Y n {\displaystyle \mathbb {E} [Y_{n}\,|\,{\mathcal {F}}_{n-1}]=Y_{n}}     a.s.

for any nI \ {0}. Since Y0 = A'0A0 = 0 by the convention about the starting point of the predictable processes, this implies iteratively that Yn = 0 almost surely for all nI, hence the decomposition is almost surely unique.

Corollary

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

Proof

If X is a submartingale, then

E [ X k | F k 1 ] X k 1 {\displaystyle \mathbb {E} [X_{k}\,|\,{\mathcal {F}}_{k-1}]\geq X_{k-1}}     a.s.

for all kI \ {0}, which is equivalent to saying that every term in definition (1) of A is almost surely positive, hence A is almost surely increasing. The equivalence for supermartingales is proved similarly.

Example

Let X = (Xn)n N 0 {\displaystyle \mathbb {N} _{0}} be a sequence in independent, integrable, real-valued random variables. They are adapted to the filtration generated by the sequence, i.e. Fn = σ(X0, . . . , Xn) for all n N 0 {\displaystyle \mathbb {N} _{0}} . By (1) and (2), the Doob decomposition is given by

A n = k = 1 n ( E [ X k ] X k 1 ) , n N 0 , {\displaystyle A_{n}=\sum _{k=1}^{n}{\bigl (}\mathbb {E} [X_{k}]-X_{k-1}{\bigr )},\quad n\in \mathbb {N} _{0},}

and

M n = X 0 + k = 1 n ( X k E [ X k ] ) , n N 0 . {\displaystyle M_{n}=X_{0}+\sum _{k=1}^{n}{\bigl (}X_{k}-\mathbb {E} [X_{k}]{\bigr )},\quad n\in \mathbb {N} _{0}.}

If the random variables of the original sequence X have mean zero, this simplifies to

A n = k = 0 n 1 X k {\displaystyle A_{n}=-\sum _{k=0}^{n-1}X_{k}}     and     M n = k = 0 n X k , n N 0 , {\displaystyle M_{n}=\sum _{k=0}^{n}X_{k},\quad n\in \mathbb {N} _{0},}

hence both processes are (possibly time-inhomogeneous) random walks. If the sequence X = (Xn)n N 0 {\displaystyle \mathbb {N} _{0}} consists of symmetric random variables taking the values +1 and −1, then X is bounded, but the martingale M and the predictable process A are unbounded simple random walks (and not uniformly integrable), and Doob's optional stopping theorem might not be applicable to the martingale M 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 X = (X0, X1, . . . , XN) denote the non-negative, discounted payoffs of an American option in a N-period financial market model, adapted to a filtration (F0, F1, . . . , FN), and let Q {\displaystyle \mathbb {Q} } denote an equivalent martingale measure. Let U = (U0, U1, . . . , UN) denote the Snell envelope of X with respect to Q {\displaystyle \mathbb {Q} } . The Snell envelope is the smallest Q {\displaystyle \mathbb {Q} } -supermartingale dominating X[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 U = M + A denote the Doob decomposition with respect to Q {\displaystyle \mathbb {Q} } of the Snell envelope U into a martingale M = (M0, M1, . . . , MN) and a decreasing predictable process A = (A0, A1, . . . , AN) with A0 = 0. Then the largest stopping time to exercise the American option in an optimal way[10][11] is

τ max := { N if  A N = 0 , min { n { 0 , , N 1 } A n + 1 < 0 } if  A N < 0. {\displaystyle \tau _{\text{max}}:={\begin{cases}N&{\text{if }}A_{N}=0,\\\min\{n\in \{0,\dots ,N-1\}\mid A_{n+1}<0\}&{\text{if }}A_{N}<0.\end{cases}}}

Since A is predictable, the event {τmax = n} = {An = 0, An+1 < 0} is in Fn for every n ∈ {0, 1, . . . , N − 1}, hence τmax 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 τmax the discounted value process U is a martingale with respect to Q {\displaystyle \mathbb {Q} } .

Generalization

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

Citations

  1. ^ Doob (1953), see (Doob 1990, pp. 296−298)
  2. ^ Durrett (2010)
  3. ^ (Föllmer & Schied 2011, Proposition 6.1)
  4. ^ (Williams 1991, Section 12.11, part (a) of the Theorem)
  5. ^ (Williams 1991, Section 12.11, part (b) of the Theorem)
  6. ^ (Lamberton & Lapeyre 2008, Chapter 2: Optimal stopping problem and American options)
  7. ^ (Föllmer & Schied 2011, Chapter 6: American contingent claims)
  8. ^ (Föllmer & Schied 2011, Proposition 6.10)
  9. ^ (Föllmer & Schied 2011, Theorem 6.11)
  10. ^ (Lamberton & Lapeyre 2008, Proposition 2.3.2)
  11. ^ (Föllmer & Schied 2011, Theorem 6.21)
  12. ^ (Schilling 2005, Problem 23.11)

References

  • Doob, Joseph L. (1953), Stochastic Processes, New York: Wiley, ISBN 978-0-471-21813-5, MR 0058896, Zbl 0053.26802
  • Doob, Joseph L. (1990), Stochastic Processes (Wiley Classics Library ed.), New York: John Wiley & Sons, Inc., ISBN 0-471-52369-0, MR 1038526, Zbl 0696.60003
  • Durrett, Rick (2010), Probability: Theory and Examples, Cambridge Series in Statistical and Probabilistic Mathematics (4. ed.), Cambridge University Press, ISBN 978-0-521-76539-8, MR 2722836, Zbl 1202.60001
  • Föllmer, Hans; Schied, Alexander (2011), Stochastic Finance: An Introduction in Discrete Time, De Gruyter graduate (3. rev. and extend ed.), Berlin, New York: De Gruyter, ISBN 978-3-11-021804-6, MR 2779313, Zbl 1213.91006
  • Lamberton, Damien; Lapeyre, Bernard (2008), Introduction to Stochastic Calculus Applied to Finance, Chapman & Hall/CRC financial mathematics series (2. ed.), Boca Raton, FL: Chapman & Hall/CRC, ISBN 978-1-58488-626-6, MR 2362458, Zbl 1167.60001
  • Schilling, René L. (2005), Measures, Integrals and Martingales, Cambridge: Cambridge University Press, ISBN 978-0-52185-015-5, MR 2200059, Zbl 1084.28001
  • Williams, David (1991), Probability with Martingales, Cambridge University Press, ISBN 0-521-40605-6, MR 1155402, Zbl 0722.60001
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