The goal is to obtain sharper/more explicit bounds for the upcrossing number of Brownian motion compared to the naive bound given by Doob’s upcrossing inequality.
Notation:
- For $b > a$, we set $\nu_{0}(a, b) = 0$ and write, for all $i \in \mathbb Z_+$,
$$\tau_i(a, b) := \inf \{t \geq \nu_{i-1}(a, b) | W_t = a\}$$
$$\nu_i(a, b) := \inf \{t \geq \tau_i(a, b)| W_t = b\}$$
We shall assume the Brownian motion starts at $c \in \mathbb R$.
We have
$$U(a, b) = \sum_{i = 1}^\infty \mathbf 1(\nu_i (a, b) \leq 1),$$
so that
$$\mathbb E[U(a, b)] = \sum_{i = 1}^\infty \mathbb P(\nu_i (a, b) \leq 1),$$
But, writing $M$ for the supremum over $[0, 1]$ of a Brownian motion starting at $0$, we have by iterated use of the reflection principle,
$$\mathbb P(\nu_i (a, b) \leq 1) = \mathbb P (M \geq |c-a| + (2i-1)(b - a)).$$
Recalling that $M \overset{d}{=} |B_1|$, we get the exact series expression
$$\mathbb E[U(a, b)] = \sum_{i = 1}^\infty \mathbb P (|B_1| \geq |c-a| + (2i-1)(b - a)).$$
We can obtain useful bounds from this expression. Indeed, by a simple Chebyshev inequality,
$$\mathbb E[U(a, b)] \leq \sum_{i = 1}^\infty \frac{1}{(b-a)^2(2i-1)^2},$$
so that
$$\mathbb E[U(a, b)] \leq \frac{\pi^2}{8(b-a)^2},$$
which is already more effective than Doob’s inequality once $b-a$ is large.