If $\tau$, $\rho$ are stopping times, then it is easily seen that $\tau+\rho$ is also a stopping time. However $\tau-\rho$ and $\tau\rho$ are not necessarily stopping times as it requires a "peak into the future", but I am not sure why this is so and would appreciate any feedback to facilitate my understanding.
For the difference case, I think it not as if $(X,\mathscr{F})$ is a measurable space and $f, \space g \space :(X,\mathscr{F})\rightarrow([0,\infty),\mathscr{B}([0,\infty))$ are measurable maps then if for some $x\in X$, $f(x)-g(x)<0$ then I say it does not make sense that $f-g$ is measurable as it maps some elements outside of $[0,\infty)$, and $(f-g)^{-1}(\mathscr{B}([0,\infty)))$ is not a sub $\sigma$-algebra of $\mathscr{F}$. Is my reasoning correct?
So in the case of stooping time, $\tau$ we have the added requirement that $1_{\{\tau\leq t\}}$ be adapted to the given filtration. So my question is why does the difference of stopping times require a "peak into the future"? I have the same qualms about the product case.
However in the case of the reciprocal, I think I see why, as if we take $t=1/2$, then $\{1/\tau\leq2\}=\{\tau\geq2\}\in\mathscr{F}_2$ and we have no way on knowing if the event is in $\mathscr{F}_{1/2}$
So any comments and answers would be really appreciated.
Let $(\mathcal{F}_t)_{t \geq 0}$ be a filtration and $\tau$ an $\mathcal{F}_t$-stopping time, i.e. $\{\tau \leq t\} \in \mathcal{F}_t$ for all $t \geq 0.$
For a fixed constant $c >0$ the mapping $\varrho(\omega) := c$ defines an $\mathcal{F}_t$-stopping time. Then $\tau-\varrho = \tau-c$ is, in general, not a $\mathcal{F}_t$-stopping time since
$$\{\tau-\varrho \leq t\} = \{\tau \leq t+c\}$$
is in $\mathcal{F}_{t+c}$ but not necessarily in $\mathcal{F}_t$. A similar thing happens if we consider $\varrho \cdot \tau$ and $\varrho:=c >1$.