Crossposted on MathOverflow
Motivated by Bowman and McLaughlin (2000) on polynomial continued fractions, I considered an extension to functional continued fractions, where the numerator of each fraction is the integral of the previous fraction.
That is, define the continued fraction integral transform (CFIT) as \begin{align}\{\mathcal If(t)\}(s)=\dfrac{f(s)}{1+\dfrac{\int_0^s f(x)\,dx}{1+\dfrac{\int_0^s\int_0^u f(x)\,dx\,du}{1+\cdots}}}=\dfrac{f(s)}{1+\dfrac{f^{(-1)}(s)}{1+\dfrac{f^{(-2)}(s)}{1+\cdots}}}={\large{\mathop{\mathrm{K}}_{n=0}^{\infty}}}\frac{f^{(-n)}(s)}1\end{align} where $f\in C^\infty(\Bbb R)$ and $f^{(-k)}$ is Lagrange's notation for the $k$th antiderivative of $f$.
Some elementary properties of the transform include
$\{\mathcal I(0)\}(s)=0$;
$\{\mathcal If\}(0)=f(0)$;
$\{\mathcal If\}(s)=\dfrac{f'(s)}{\{\mathcal If'\}(s)}-1$ for all non-constant $f$ such that $f(0)=0$.
Considering the simplest, non-trivial case $f(t)\equiv1$, we have $f^{(-k)}(t)=t^k/k!$ so that $$\{\mathcal I(1)\}(s)=\dfrac{1}{1+\dfrac s{1+\dfrac{s^2/2!}{1+\cdots}}}.$$ 
We can see that as $n$ increases, $\mathcal I(1)$ produces more waves. As @PeterForeman mentioned in the comments, the limit $\lim\limits_{s\to-\infty}\mathcal I(1)$ does not exist since it is zero for odd $n$ and $+1$ for even $n$. However, I believe there are more things that can be investigated.
Questions
Has the CFIT already been studied/discovered? If so, reference to literature would be appreciated.
Going back to the example of $\{\mathcal I(1)\}(s)$, is it true that the maximum value of each wave increases as $s$ increases up to the first wave? Are there an infinite number of such waves, and is there a closed form for $\max\mathcal I(1)$?
The period of the oscillations of $\mathcal I(1)$ appears to converge to $$\dfrac4e=1.4715\cdots$$ Can this be proven?
Empirically, the argmins are
-2.12897, -3.73409, -5.26940, -6.78494, -8.29119, -9.79168, -11.2881, -12.7814, -14.2723,
-15.7613, -17.2487, -18.7348, -20.2198, -21.7038, -23.1870, -24.6695, -26.1513, -27.6326,
-29.1133, -30.5937, -32.0736, -33.5531, -35.0323, -36.5111, -37.9897, -39.4680, -40.9461,
-42.4239, -43.9015, -45.3790, -46.8562, -48.3332, -49.8101, -51.2869, -52.7635, -54.2399,
-55.7162, -57.1924, -58.6685, -60.1445, -61.6203, -63.0961, -64.5717, -66.0473, -67.5228,
...
with consecutive differences
1.60512, 1.53531, 1.51554, 1.50625, 1.50049, 1.49642, 1.49330, 1.49090,
1.48900, 1.48740, 1.48610, 1.48500, 1.48400, 1.48320, 1.48250, 1.48180, 1.48130,
1.48070, 1.48040, 1.47990, 1.47950, 1.47920, 1.47880, 1.47860, 1.47830, 1.47810,
1.47780, 1.47760, 1.47750, 1.47720, 1.47700, 1.47690, 1.47680, 1.47660, 1.47640,
1.47630, 1.47620, 1.47610, 1.47600, 1.47580, 1.47580, 1.47560, 1.47560, 1.47550, ...
