$$\sin(x)^{\cos(x)}=\frac{1}{2}$$
$$e^{\ln(-(\frac{1}{2}i)(e^{ix}-e^{-ix}))(\frac{1}{2}e^{ix}+\frac{1}{2}e^{-ix})}=1/2$$
$$\ln(-(\frac{1}{2}i)(e^{ix}-e^{-ix}))(\frac{1}{2}e^{ix}+\frac{1}{2}e^{-ix})=-\ln(2)$$
Looks too complicated.
$\ $
$$\sin(x)^{\cos(x)}=\frac{1}{2}\tag{1}$$
$\sin(x)\to\sqrt{1-\cos(x)}$:
$$\sqrt{1-\cos(x)^2}^{\ \cos(x)}=\frac{1}{2}$$
$$\left(\sqrt{1-\cos(x)^2}^{\ \cos(x)}\right)^2=\frac{1}{4}$$
$$(1-\cos(x)^2)^{\cos(x)}=\frac{1}{4}$$
$\cos(x)\to t$:
$$(1-t^2)^t=\frac{1}{4}$$
$$e^{\ln(1-t^2)t}=\frac{1}{4}$$
$$\ln(e^{\ln(1-t^2)t})=-2\ln(2)$$
$$\ln(1-t^2)t=-2\ln(2)$$
$t\to\sqrt{1-e^u}$:
$$\ln(e^u)\sqrt{1-e^u}=-2\ln(2)$$
$$u\sqrt{1-e^u}=-2\ln(2)$$
$$u^2(1-e^u)=4\ln(2)^2$$
$$u^2-u^2e^u=4\ln(2)^2$$
$$-u^2e^u=4\ln(2)^2-u^2$$
$$\frac{-u^2}{4\ln(2)^2-u^2}e^u=1$$
$$\frac{u^2}{u^2-4\ln(2)^2}e^u=1\tag{2}$$
We see, this equation cannot be solved in terms of Lambert W, but in terms of Generalized Lambert W:
$$\frac{u^2}{(u-2\ln(2))(u+2\ln(2))}e^u=1$$
$$\frac{(u-0)(u-0)}{(u-2\ln(2))(u-(-2\ln(2)))}e^u=1$$
$$u=W\left(^{\ \ \ \ \ \ 0,\ \ \ \ \ \ 0}_{2\ln(2),-2\ln(2)};1\right)$$
Back substitution of $u$ and $t$ yields candidates for $x$. Because the square function isn't injective, squaring isn't an equivalence operation. We made two squaring steps. Therefore the solution set of equation (1) is a proper or improper subset of the solution set of equation (2).
So we have a closed form for $x$, and the series representations of Generalized Lambert W give some hints for calculating $x$.
May be there are simpler solutions.
[Mező 2017] Mező, I.: On the structure of the solution set of a generalized Euler-Lambert equation. J. Math. Anal. Appl. 455 (2017) (1) 538-553
[Mező/Baricz 2017] Mező, I.; Baricz, Á.: On the generalization of the Lambert W function. Transact. Amer. Math. Soc. 369 (2017) (11) 7917–7934 (On the generalization of the Lambert W function with applications in theoretical physics. 2015)
[Castle 2018] Castle, P.: Taylor series for generalized Lambert W functions. 2018