For example, for $n=100, t=2, i=50,$ t=2,$ the number of paths is
For $n=101, t=2, i=51,$ t=2,$ the number of paths is
Now for some speculation: I believe a
A lot more can be said when $t$ varies, but the answers should be are more complicated. For $t$ slowly increasing, it may help to know how the eigenvectors change as you increment $t$. The geometry of this change should tell you how long you need to keep $t$ constant c\sqrt[3]n$, there is enough time for the distribution to stabilize (for a fixed each parity) at a given value of $n$), t$, since the ratio between the magnitudes of the largest two eigenvalues and what constant factors you the magnitudes of the next two is about $1+c/t^2$, and the principal eigenvectors have a small $L^1$ distance for adjacent values of $t$. You should pick up a constant factor for each transition.
You may want to use stochastic differential equations to determine In other words, the number of paths when you spend at least $n_t \gt c t^2$ steps at a given $t$ should be
$$C \prod_{t \le t_{max}} (2 \cos \frac{\pi}{2t+2})^{n_t}$$
where $C$ is between some functions $f_{lower}(t_{max}) \lt C \lt f_{upper}(t_{max})$ which does not depend on the values of $n_t$. I don't think the $n_t \gt c t^2$ condition is sharp for this behavior. Something like $n_t \gt c t^2/\log t$ should work, too. The geometry of Brownian motion with similar boundariesthe eigenvectors for adjacent values of $t$ lets you estimate $f_{lower}$ and $f_{upper}$.
For $t$ more rapidly increasing, different behaviors occur. By the law of the iterated logarithm, if $t$ increases as $t(n) = \sqrt {(2-\epsilon) n \log\log n},$ random paths will almost surely violate the constraint. I think there are precise versions of the law of the iterated logarithm which should be may tell you when a good guidepositive proportion of random paths do not violate the constraint. I would guess that if $t(n) = \sqrt{(2+\epsilon) n \log\log n}$ then a positive percentage of random paths won't violate the constraint.

