Playing with identities ($1$) and ($2$) from this blog post and infinite geometric series, I've noticed the following.
For $x > 1$, the following series is convergent:
$$\sum_{n=0}^{\infty} e^{(2n + 1)i\cos^{-1}(x)} = \frac{1}{2\sqrt{x^2 - 1}}.\tag{$*$}\label{481686_star}$$
For $x < -1$, the following series is convergent:
$$\sum_{n=0}^{\infty} e^{-(2n + 1)i\cos^{-1}(x)} = \frac{1}{2\sqrt{x^2 - 1}}.\tag{$**$}\label{481686_starstar}$$
Regularized results (for context see here and here)
For $x \in (-1, 1)$, the series $\sum_{n=0}^{\infty} e^{-i (2n + 1) \cos^{-1}(x)}$ is divergent, but we can obtain regularized results using
$$\sum_{n=0}^{\infty} e^{-(2n + 1)i\cos^{-1}(x)} = \frac{1}{2\sqrt{x^2 - 1}}.$$
Indeed, suppose $x=0$, then $$\sum_{n=0}^{\infty} e^{-(2n + 1)i\cos^{-1}(0)} = \frac{1}{2\sqrt{0^2 - 1}}=\frac{1}{2i}=-\frac{i}{2}.$$ This result is consistent with the Abel, Borel and Cesàro regularizations. Now, suppose $x=-2$, then using \eqref{481686_star} yields $$\sum_{n=0}^{\infty} e^{(2n + 1)i\cos^{-1}(x)} = \frac{1}{2\sqrt{(-2)^2 - 1}}=\frac{\sqrt{3}}{6},$$ which is consistent with Borel regularization.
Both \eqref{481686_star} and \eqref{481686_starstar} allow for a slight generalization, since ($1$–$2$) from the aforementioned link are generalized in the formula ($22$) of the same link.
To be honest, the concept of regularization of divergent series is new to me. As you can see, I have managed to arrive at results consistent with the aforementioned classical methods using the 'trick' described above. Are the Abel, Borel and Cesàro regularizations (and mine?) the only ways to achieve these results?
Notice the first terms of the series
$$\sum_{n=0}^{\infty} e^{-(2n + 1)i \cos^{-1}(x)}$$
when $x = 0$ are:
$$-i + i - i + i - i + i\dotsb$$
Applying $(**)$ and multiplying by $i$ gives Grandi's series.