Fix . Since is a martingale,
Every finite vector consisting of and past values has a multivariate normal distribution. Therefore uncorrelated jointly normal variables are independent, so the increment is independent of every finite vector of past values. A Monotone class theorem then extends this to independence from . This is the independent increments of a Gaussian martingale.
Define the deterministic function . The independent increments from part (i) show that is increasing and that is a martingale. Mean-square continuity follows from path continuity and the Gaussian laws, so is continuous.
The Itô formula also says that is a local martingale. Their difference is therefore a continuous finite-variation process that is also a local martingale. By the theorem that a continuous finite-variation local martingale is constant, and because the difference starts at zero,
for all almost surely.
The assertion is false. Let and define . This is a centered continuous Gaussian process. Its natural filtration satisfies for every , and hence, for ,
with positive probability. Thus is not a martingale and does not belong to the stated martingale class.
The assertion is true. The Dambis-Dubins-Schwarz theorem, with an independent continuation of the Brownian motion if is bounded, represents
Because is deterministic, every finite vector is a finite vector of a Brownian motion at deterministic times and therefore has a multivariate normal distribution. Hence is a Gaussian process. This is the deterministic quadratic variation characterizes a Gaussian continuous local martingale result.
The function is a harmonic function on the annulus . The Itô formula therefore makes a bounded martingale. The optional sampling theorem for a supermartingale gives
where . Solving this linear equation yields the planar Brownian annulus hitting probability
No such function exists. Continuity on the compact closed unit disk makes bounded near the origin. The removable singularity for a bounded harmonic function extends harmonically across the origin. The extended function is continuous on the closed disk and vanishes on its boundary, so the maximum principle for harmonic functions, applied to both and , forces throughout the disk. This contradicts .

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