The *martingale representation theorem* states that any martingale adapted with respect to a Brownian motion can be expressed as a stochastic integral with respect to the same Brownian motion.

Theorem 1LetBbe a standard Brownian motion defined on a probability space and be its natural filtration.Then, every –local martingale

Mcan be written as

for a predictable,B-integrable, process .

As stochastic integration preserves the local martingale property for continuous processes, this result characterizes the space of all local martingales starting from 0 defined with respect to the filtration generated by a Brownian motion as being precisely the set of stochastic integrals with respect to that Brownian motion. Equivalently, Brownian motion has the *predictable representation property*. This result is often used in mathematical finance as the statement that the Black-Scholes model is *complete*. That is, any contingent claim can be exactly replicated by trading in the underlying stock. This does involve some rather large and somewhat unrealistic assumptions on the behaviour of financial markets and ability to trade continuously without incurring additional costs. However, in this post, I will be concerned only with the mathematical statement and proof of the representation theorem.

In more generality, the martingale representation theorem can be stated for a d-dimensional Brownian motion as follows.

Theorem 2Let be a d-dimensional Brownian motion defined on the filtered probability space , and suppose that is the natural filtration generated byBand .Then, every -local martingale

Mcan be expressed as

(1)

for predictable processes satisfying , almost surely, for each .

As Brownian motion has quadratic variation , the condition that is finite is equivalent to stating that is B^{i}-integrable. Taking the quadratic covariation of (1) with and using the identity for gives

By Lebesgue’s theorem, this shows that is given by the derivative

for almost every *t*.

Proving the representation theorem involves showing that, for all integrable random variables *Z*, there exist predictable and -integrable processes satisfying

(2) |

(almost surely), for each time . As long as this can be shown to hold for a suitably large set of random variables, the representation theorem will follow.

I now give an argument showing that (2) is indeed satisfied for certain *B*-measurable random variables. Equation (2) can be verified directly for random variables of the form

(3) |

for deterministic processes satisfying (for now, *i* denotes the square root of -1) and -measurable variable *U*. In particular, for a sequence of times and , taking gives

As are normal with zero mean and variance independently of , the expectation can be written out as

This is continuous and, setting , Ito’s lemma gives

so, taking shows that (2) is satisfied for all random variables of the form (3).

Alternatively, it can be shown that (2) holds for all random variables of the form , for a bounded measurable function and time *T*. For times , is, by definition, joint normal with covariance matrix independently of . This allows us to write out for all as a function of ,

From this, it can be seen that *f* is twice continuously differentiable, so Ito’s formula can be applied,

(4) |

Here the subscripts *t* and *i* represent the partial derivatives of with respect to time and respectively. The final term on the right-hand-side of (4) is a continuous FV process, all the other terms being local martingales. As continuous FV local martingales are constant, this allows us to break (4) up into the following two equations,

The first of these is the Kolmogorov backward equation, and the second shows that does indeed satisfy the representation property (2) with integrands . It should be clear that this argument is quite general, and applies to any continuous martingale which is Markov with twice continuously differentiable transition densities. In fact, it is not difficult to extend the argument to variables of the form

for times , -measurable variable *U* and bounded measurable function . However, I will not do this here, as *Z* of the form (3) is already enough to prove the martingale representation theorem for Brownian motion.

From here, it is possible to extend (2) to all bounded measurable random variables, by taking limits and applying the monotone class theorem. Ito’s isometry can be used to show that -convergence of the random variables implies convergence of the integrands . However, in the proof given here, I will instead make use of the following more general result, applying to all continuous local martingales. Given a continuous local martingale *N*, every other local martingale can be expressed as an integral with respect to *N* plus an `orthogonal’ term. This is a useful result in its own right. In finance, it has applications to models of incomplete markets in which it is not possible to exactly replicate all contingent claims by trading in the underlying stock. Instead, it is only possible to replicate them up to an orthogonal (i.e., unhedgeable) term.

Lemma 3LetNbe a continuous local martingale andMbe any other local martingale. Then, there exists anN-integrable process and local martingaleLsuch that

and [L,N]=0.

*Proof:* The lemma reduces to the statement that there is an *N*-integrable process satisfying . Then, defining gives

as required.

First, the FV process [*M*,*N*] is absolutely continuous with respect to [*N*]. That is, if is a bounded process satisfying , then (almost surely). This follows from the Kunita-Watanabe inequality,

This implies that there exists a predictable process with . It needs to be shown that is *N*-integrable. That is, is almost-surely finite for each time *t*. This is, again, a consequence of the Kunita-Watanabe inequality. For any constant *K*,

Cancelling the term from the right hand side, squaring, and taking the limit gives

which is finite, as required. ⬜

This has the following d-dimensional generalization.

Lemma 4Let be continuous local martingales with covariations for . Then, every local martingaleMcan be expressed as

for -integrable processes and local martingaleLsatisfying .

*Proof:* By Lemma 3, there are -integrable processes such that satisfy . Setting and using the condition that for gives

⬜

The martingale representation theorem follows immediately from applying the following to Lemma 4, so that the orthogonal term *L* is constant.

Lemma 5Let be a d-dimensional Brownian motion defined on the filtered probability space , and suppose that is the natural filtration generated byBand .

Then, any local martingaleLsatisfying for eachiis constant.

*Proof:* By localization, it is enough to consider the case where *L* is a cadlag martingale and, replacing *L* by if necessary, we can assume that . Consider a bounded random variable *Z* satisfying (2). Then, is a bounded martingale with covariation . So, LM is a local martingale. As *M* is bounded and *L* is a martingale, *LM* will be of class (D), so is a proper martingale. Then,

For any fixed time *t*, consider the set *S* of bounded random variables *Z* satisfying . As shown above, this includes all *Z* of the form (3), which generate the sigma-algebra given by *B*. Also, dominated convergence implies that *S* is closed under taking limits of uniformly bounded sequences of variables. So, by the monotone class theorem, *S* contains all bounded random variables measurable with respect to and *B*. In particular, if the filtration is generated by and *B* then is in *S*, giving,

and (almost surely), as required. ⬜

Hi can I have the source of this Martingale Representation Theorem ?

Sorry, what are you asking for? You want a source file, as in a pdf/tex file? Or do you mean a reference for the theorem?

Thank you for your reply, I think a reference for the theorem will be help.

It’s a standard result which most textbooks should cover. Checking the ones I have to hand, they all mention it. Revuz & Yor, Continuous Martingales and Brownian Motion (Chapter V, Prop 3.2); Protter, Stochastic Integration and Differential Equations (Chapter IV, Theorem 43); Kallenberg, Foundations of Modern Probability (Chapter 18, Theorem 18.10); Rogers & Williams Diffusions, Markov Processes and Martingales (Chapter IV, Theorem 36.1).

That is really helpful! Thank you very much!

I wonder if \xi can be taken such that it has left limits a.s.? Are there any examples where this is not possible?

Hi. No, that’s not possible in general. Any square integrable function can appear as the integrand, and it is uniquely defined almost everywhere. Eg, you could have .

Hello George,

as you know, we can’t claim that a Poisson process is continuous a.s.

We know that it is only continuous in probability. But all the books just mention it. I was wondering if the proof that the process cannot be continuous a.s. is difficult.

Thank you.

Alex.

Poisson processes are integer valued and are not constant. That is enough to conclude that they can’t be almost surely continuous.

this holds for all local martingales, not just continuous ones?

Yes. But — if {

F}_{t}_{t≥0}is a filtration generated by a Brownian motion then allF-local martingales are continuous anyway. This fact does have further consequences beyond martingale representation. For example, it implies that all_{t}F-stopping times are predictable, and all right-continuous adapted processes are predictable._{t}Does (2) hold for all integrable variables? The proofs just apply “certain” random variables and variables with the representation F(B_T). What are the minimal conditions for this to be true?

Given an integrable Z, we can define a uniformly integrable martingale which we can apply Theorem to to show (2) holds.

Note that this argument is not circular – we never needed to show (2) holds for all integrable random variables to prove Theorem 2, just for the ones of the special exponential form given by (3).

Sorry, typo.

which we can apply Theorem 2 to to show (2) holds. *

Hi. Thanks for the post. One of the key points in the Martingale Representation Theorem seems to be that the Filtration to which a given martingale is adapted is the natural filtration of the Brownian Motion on a measurable space. In several applications, this particular condition may be hard to verify. For example, the compensated Poisson process is a martingale, but not adapted to the Brownian Filtration. [This somehow limits the general applicability of this theorem]. Is there some constructive procedure to determine whether the given filtration of the martingale, is in fact the natural Brownian Filtration ?

Why is in Lemma 3?

This was under the condition that . Integrate with respect to this, or use the fact that it implies almost everywhere under the measure.

Hi! There is any sufficient condition in Lemma 3 concerning and that implies ? Which means: there exists a “proper” version of Radon-Nikodym theorem for martingales? Intuition would suggest that should be (at least) “absolutely continuous” with respect to . If we think in a vector measures language this would mean that predictable such that , then , but maybe this is not sufficient.

Thanks,

Alex

I’m not sure what the sufficient condition would be. Consider the case where M and N are independent standard Brownian motions. Then, taking quadratic variations, if we have and, hence . However, L is not 0.

Are there any martingale representation theorem for manifold valued martingales?

Good morning George,

Thank you for your beautiful blog! I would be interested in the following statement you made: “It should be clear that this argument is quite general, and applies to any continuous martingale which is Markov with twice continuously differentiable transition densities”. Do you have a reference for this, some book/paper where this is proven? Thanks

Hi Hurgudurgu,

I have seen similar statements before in various books & papers. Nothing that I can recall precisely right now, but I think that it is quite well known that sufficiently “nice” strong Markov martingales satisfy the representation property. If I remember any references, I will come back here. Probably googling the relevant terms would get something, although probably not the exact conditions stated here.

Thanks

George