I am working on the following problem
Given the solution to the Geometric Brownian Motion $$S_t=S(0)\exp\Big[(\mu-\frac{1}{2}\sigma^2)t+\sigma B_t\Big]$$ Where $\{B_t:t\geq 0\}$ is a Brownian motion.
a) Show that for $\mu>\frac{1}{2}\sigma^2$, we have that $S(t)\rightarrow\infty$ as $t\rightarrow\infty$.
b) Show that for $\mu<\frac{1}{2}\sigma^2$, we have that $S(t)\rightarrow 0$ as $t\rightarrow\infty$.
I know multiple things that will probably help me in finding the solution, but I'm not able to connect the dots. For question a), we know that the term in the exponent can be split into an exponent with a strictly positive term, and an exponent with the Brownian Motion.
I can't figure out why the exponent with the Brownian motion would go to infinity in question a), but not in question b). In other words, I cannot see why we would have that $$S(0)\exp\Big[ct+\sigma B_t\Big]\rightarrow\infty ,\quad c>0$$But also $$S(0)\exp\Big[dt+\sigma B_t\Big]\rightarrow\infty ,\quad d<0$$ What is the convergence behavior of Brownian Motion in the exponent?
Moreover, we know that the definition of convergence in probability of some sequence $(X_n)$ is that $$\forall\epsilon>0:\mathbb{P}(|X_n-X|>\epsilon)\rightarrow 0$$
Any tips are highly appreciated!