Recently, I have become quite obsessed with the follow series:
$$f(t,x)=\sum_{m=-\infty}^{\infty} (-1)^m f(t+x m)$$
where $f$ is analytic. This series automatically produces a periodic function with period $2x$ (assuming it converges). Let use focus on four seemingly similar functions of the form $g(t)e^{-h(t)}$:
$$\begin{align} f1(t)&=t e^{-t^2} \\ f2(t)&=\tanh(t) e^{-\cosh(t)} \\ f3(t)&=\tanh(t/2) e^{-\cosh(t)} \\ f4(t)&=t e^{-\cosh(t)} \end{align}$$
There is an interplay between the increasing behavior of $g(t)$ and $h(t)$ that I don't understand. In particular, I would like to know when $f(t,x)$ is positive on the first quarter of it's periodicity, that is when $t\in (0,x/2)$.
Using mathematica, it appears that $f1$ and $f2$ are never negative. In fact, it appears:
$$f(t,x)>(f(x/2,x)/(x/2)) * t$$
for all $t\in(0,x/2)$. However, $f3$ and $f4$ appear to fail being positive. Indeed, focusing on $f4$ and choosing $x\approx 0.82$, it appears that $f(t,x)<0$ for all $t\in(0,x/2)$. The split appears to be at $c\approx 0.919583$. Zooming in very very close to zero, it does appear that at $c$, $f4$ has multiple simple zeros being both positive and negative. However, to the right and left of this value $f4$ appears to be either all positive or all negative.
Likewise, for $c\approx 0.61093879$ and function $f3$, it appears that $f(t,x)$ is positive for $x>c$ and negative for $x<c$, again for $t\in(0,x/2)$. This is very surprising considering the extreme similarity of $f2$ and $f3$. Also, zooming in very very close to zero at $x\approx 0.61093879$ it does not appear that $f3$ has any simple zeros, meaning that is appears there exists some constant $c\approx 0.61093879 $, such that
$$\sum_{m=-\infty}^\infty (-1)^m \tanh((t+cm)/2)e^{-\cosh(t+cm)}=0$$
for all $t\in\mathbb{R}$. That seems very interesting.
Question: Is it indeed the case for $f2$, that $f(t,x)>0$ for all $t\in(0,x/2)$? Moreover is $f(t,x)>(f(x/2,x)/(x/2)) * t$?
UPDATE
So, it appears that $\sin(xt)$ serves as a better lower bound instead of a linear equation, in fact the series appears to uniformly approach $\sin(xt)$ as $x\to 0$, yielding a ratio of $1$ in their limit. I then went ahead and flipped over the function so that is would be between 0 and 1 (assuming the series is positive), and I then multiplied $t$ by $x$ so as to map the periodicity between $(0,1)$. I then graphed through different values of $x$ to see what $t$ looks like. The below animation is
$$ g(t,x):=\frac{f(x/2,x)*\sin(\pi t)}{f(xt,x)}$$
where the series uses the functions $f_2(t)=\tanh(t)e^{-\cosh(t)}$ and $f_5(t)=\tanh(t/2)e^{-\cosh(t)}$. We see that $f_2$ appears to be strictly decreasing as $x$ increases. Likewise, we see that $f_5$ appears to oscillate around $1$ at the start, in particular since the series for $f_5$ appears to be negative for some values of $x$, we see here the ratio is $>1$ for those same values of $x$. How would we prove that for $t>0$ and $f(t)=\tanh(t)e^{-\cosh(t)}$, we have
$$\frac{d}{dx} g(t,x) = \frac{d}{dx}\frac{f(x/2,x)*\sin(\pi t)}{f(xt,x)}\le 0 $$
for any $x$? How do we prove $\lim g(t,x)=1$ when $x\to 0$ and $\lim g(t,x)=0$ ($t\not= 1/2$) when $x\to\infty$? Working with this series seems particularly difficult, even though we can see what it is doing.