This question has repeatedly appeared to me whilst studying certain linear differential equations with time-dependent coefficients.
Let $\phi(t) \in C^2(\Bbb R, \Bbb C)$; that is, $\phi(t)$ is a twice continuously differentialble complex valued function on the real line $\Bbb R$. Assume that
$\lim_{t \to \infty} \vert \phi(t) \vert = 0, \tag{1}$
and
$\lim_{t \to \infty} \vert \ddot \phi(t) \vert \to 0 \tag{2}$
as well. Then must we also have
$\lim_{t \to \infty} \vert \dot \phi(t) \vert \to 0? \tag{3}$
An answer to the above question as such would be most appreciated. There are, however, two more restricted questions the answers to which would suffice for my purposes:
I.) Suppose instead of (2) we assume the existence of a globally bounded, non-negative real function $b: \Bbb R \to \Bbb R_{\ge 0}$ such that
$\vert \ddot \phi(t) \vert \le b(t) \vert \phi(t) \vert \tag{4}$
for sufficiently large $t$. Is this hypothesis, in concert with (1), sufficient to force (3)? Readers should feel free to add various hypotheses on $b(t)$ if they desire, such as $b(t) \in C^k(\Bbb R, \Bbb R_{\ge 0})$ for some $k\ge 0$, or that $b(t)$ exhibits some specific functional behavior, e.g. $b(t) = e^{-t}$ for sufficiently large $t$.
I am particularly interested in the case $b(t) = B > 0$ a constant, so that
$\vert \ddot \phi(t) \vert \le B \vert \phi(t) \vert. \tag{5}$
2.) Suppose $c(t) \in C^k(\Bbb R, \Bbb C)$, $\Vert c(t) \Vert_k < \infty$, and
$\ddot \phi(t) + c(t)\phi(t) = 0; \tag{6}$
then the hypothesis $\lim_{t \to \infty} \vert \phi(t) \vert \to 0$ clearly implies (2); can we now show $\lim_{t \to \infty} \vert \dot \phi(t) \vert \to 0$?
Of particular interest to me is the case $k = 0$, that is, $c(t):\Bbb R \to \Bbb C$ is a bounded, continuous function.
It is clear that these questions are, more or less, in order of decreasing generality: (2) is a case of (1), itself a case of most widely scoped question stated at the beginning.
My own efforts on this problem focused primarily on case (2.) and equation (6). I looked a several things; for instance, (6) implies
$\dot \phi \ddot \phi(t) + c(t)\phi(t) \dot \phi(t) = 0, \tag{7}$
or
$\dfrac{1}{2} \dfrac{d(\dot \phi(t))^2}{dt} + c(t) \dfrac{1}{2} \dfrac{d (\phi(t))^2}{dt} = 0 \tag{8}$
or
$\dfrac{d(\dot \phi(t))^2}{dt} + c(t)\dfrac{d (\phi(t))^2}{dt} = 0, \tag{9}$
which leads to an integral relationship
$( (\dot \phi(t))^2 - (\dot \phi(t_0))^2 + \displaystyle \int_{t_0}^t c(s)\dfrac{d (\phi(s))^2}{ds} = E, \tag{10}$
a constant. I think perhaps (10) might be used to show $\dot \phi(t)$ becomes small for large $t$, since $\phi(t)$ does; but I haven't found a conclusive argument along these lines as of this writing.
I also tried looking at (1) and (2) directly, hoping to show that if $\ddot \phi(t)$ became very small, so that $\dot \phi(t)$ couldn't change too much, it ($\dot \phi$) would have to remain relatively small, lest $\phi(t)$ itself grow in a way not permitted by (1); but these are at the present more intuitive speculations rather than rigorous results.
I'm hoping someone can help me fill in the gaps . . . any insights offered will be seriously considered and appreciated, whether or not they provide a complete solution.