First work with the filtration , which records the Brownian motion and whether default has occurred. On all subsequent defaultable stock prices vanish. On , the memoryless property of the exponential distribution gives survival from to with conditional probability . The residual survival event is independent of the future independent increments of the Brownian motion. Thus, for deterministic ,
Also , so this is a true martingale, with no localization needed. Its natural filtration is contained in ; applying the tower property of conditional expectation to the displayed identity yields the requested natural-filtration martingale property:
The printed convention keeps the stock alive at . It is a left-continuous convention at that one random time. Replacing it by gives the usual càdlàg zero-recovery default model; since at each fixed , the fixed-time martingale calculations above are unchanged.
A martingale with the specified terminal value must equal its conditional expectation. If , default has already occurred and the terminal European call option payoff is zero. If , put . Conditional on survival to ,
where has the standard normal distribution; the conditional probability of this survival is . The conditional expectation of the payoff in the enlarged filtration used in part (c) is consequently
This expression is already measurable with respect to the natural filtration of , so the tower property of conditional expectation gives the same value there. The survival factor cancels the compensating growth factor:
The separate zero branch avoids division by zero. At it gives the required payoff, using ; integrability follows from .
For fixed maturity , define and . The stochastic Fubini theorem and the moving lower endpoint give
The factor is the integral over one of the two triangles in the square . Applying the Itô formula to , its quadratic-variation correction cancels that factor:
Set , the reciprocal of the continuous-time bank account. The Itô product rule then gives
If , then on this finite horizon. The Novikov condition holds, so this stochastic exponential is a true martingale, not merely a local martingale. The discounted price is therefore
The authoritative PDF discounts to in this part. The TeX transcription's upper endpoint would include future short rates and is incorrect here.
Under the usual no-arbitrage interpretation from part (a), let be an equivalent martingale measure for the strictly positive numéraire . Then is a martingale. Define the discounted European call option payoff . Because and , we have . The conditional Jensen inequality therefore gives
For the middle step, the strike is fixed conditionally on ; alternatively use . Thus is a submartingale. Risk-neutral valuation in units of gives , with the usual fixed initial prices. Consequently
The source's word “increasing” means nondecreasing: a European call option can have zero payoff at successive maturities, so strict increase is not guaranteed. Integrability is understood in the claim class for which the stated replication prices exist.
Backward induction makes every adapted and integrable: the conditional expectation of an integrable random variable is integrable, and . The Snell envelope recursion directly gives , so is a supermartingale.
If is a submartingale, iterating its defining inequality gives . Starting at and applying the tower property of conditional expectation backwards shows
This last conditional expectation is a true martingale. The conclusions are
In the second case waiting until attains the optimal stopping value. It is not generally true that : that further equality holds when itself is a martingale.
Apply the Itô formula to . The backward equation cancels its drift, leaving
Bounded and make this Itô integral square-integrable on the finite horizon; in addition itself is bounded. Hence is a true martingale, not just a local martingale, and . Taking conditional expectations gives
The stock is understood to be adapted to the stated Brownian filtration, with its initial value fixed there. This is the Feynman-Kac formula in the zero-potential, zero-drift case.
The positive density process is the stochastic exponential
Since is bounded, the Novikov condition holds; is a true martingale with and . Thus it defines the stated equivalent probability measure. The positive sign in the exponent means that the Girsanov theorem gives
Under this change of measure, applying the Itô formula to produces precisely the drift in its backward equation, which vanishes:
Bounded and make a true martingale under . Its terminal value is . Consequently
The sign can also be checked before changing measure: under the original measure , while the quadratic covariation term in is , exactly cancelling its drift.
Relative to a probability space and a filtration , the real stochastic process is a martingale if it is adapted, each is an integrable random variable, and
Here adapted means is -measurable, and integrability means . By the tower property of conditional expectation, the equivalent multi-step condition is for all . The filtration is part of the definition; specifying only the marginal means is insufficient.
The discrete-time Doob L2 maximal inequality states that a square-integrable martingale satisfies
Equivalently, the Lp norm of the maximum at is at most . The same assertion holds for a nonnegative square-integrable submartingale. No assumption is required; for a bound in terms of fluctuations from the initial value, apply it to .
Use the natural filtration and define . The increments are centered, independent, and square integrable, so their conditional expectations given the past are zero. Thus is a square-integrable martingale with . Independence gives
Applying the Doob L2 maximal inequality yields
This includes , when every centered increment vanishes almost surely.
For the converse in the characterization of a martingale by stopped expectations, fix and . Define the bounded stopping time
Indeed, its only nontrivial sublevel event is . Applying the assumed stopped-expectation equality to and to the deterministic stopping time gives
This holds for every . Since is adapted and both variables are integrable, the defining test-event property of conditional expectation yields
Together with the given adaptation and integrability, this is exactly the martingale property.
For the forward implication, let be a martingale and let the stopping time satisfy for a deterministic integer . The stopped variable is integrable because it uses only finitely many integrable values. The pathwise identity
expresses it through martingale increments. Since , each summand has expectation zero by conditional expectation. Consequently
This proves the bounded-time case of the optional stopping theorem directly; no assumptions about an unbounded stopping time are being used.
The mean increment is , so is a martingale. Applying the bounded optional stopping theorem at gives
The terminal sums are bounded by the exit-state bounds from (b), while increases to the integrable stopping time . The dominated convergence theorem on the left and the monotone convergence theorem on the right therefore prove
This is also Wald's equation here. In fact, the stopped identity already implies from , giving another direct finite-expectation justification.
The Martingale convergence theorem in its -bounded form says that a martingale with has an integrable limit and
The norm bound on the limit follows from Fatou lemma. Boundedness in by itself does not imply convergence in L1. The uniformly integrable martingale convergence theorem gives the stronger conclusion: if is uniformly integrable, then both almost surely and in L1 norm, and . Conversely, convergence in L1 implies uniform integrability.
For the distinction, the fair-coin doubling martingale has expectation one for every but converges almost surely to zero. Its L1 norm remains one, so its convergence is not in L1 norm. These two formulations specify exactly which hypothesis is needed in part (d).
For , the Lp martingale convergence theorem states that a martingale with has a limit such that
Moreover, and . To see why matters, the Doob Lp maximal inequality gives an integrable dominating variable . The Martingale convergence theorem first supplies the almost-sure limit, then the dominated convergence theorem supplies convergence in the Lp norm. This maximal estimate is unavailable at in the required form.
Work on as a probability space, with Lebesgue measure of total mass one. Let be the filtration generated by the level- half-open dyadic cells together with the separate null cell . Define the dyadic slope martingale by
The endpoint may be assigned any value, since it is a null set for Lebesgue measure. The two child slopes average to their parent slope, by telescoping the two increments. Therefore almost everywhere, so this is a martingale. The Lipschitz condition gives everywhere except possibly at the freely chosen endpoint, where we take zero.
Apply the Lp martingale convergence theorem with . Its limit has almost everywhere and in L1 norm as well, by Cauchy-Schwarz inequality. Choose a measurable representative of and set it to zero on any exceptional null set; it is then a bounded measurable function on the entire interval.
Set . Telescoping at the grid points shows that is the linear interpolation of on the dyadic grid. The Lipschitz condition gives . Also
The two uniform limits coincide, giving the absolutely continuous function representation
The chosen bound holds for every after the null-set modification; the integral identity holds for every simultaneously.
Let , , and . The function is harmonic away from the origin: its radial Laplacian in dimension three is
The Itô formula therefore makes a local martingale, bounded between and , hence a true martingale. The annulus exit time is finite almost surely. For instance, exit from the containing open ball is finite because from every point in the open ball a sufficiently large Gaussian vector increment has a uniform positive probability of leaving it in unit time; iterate the geometric tail bound from a uniform escape probability.
The optional stopping theorem at , followed by the dominated convergence theorem, gives . By continuity, there is no radial overshoot and the two exit spheres cannot be hit simultaneously. Writing gives
All harmonicity and boundedness statements apply only in the annulus, which stays away from the singularity at zero.