Here is an answer inspired (in particular) by the answer by Calvin Lin to this question.
Let us give the indexed name $A_n$ in the case $A$ is $n \times n$. Let $D_n$ denote its determinant. We have in particular
$$D_1=1, \ \ D_2=0 \tag{1}$$
Using two successive Laplace expansions of $D_n$ with respect to columns, one obtains the recurrence relationship:
$$D_n=D_{n-1}-D_{n-2}\tag{2}$$
(2) is a linear recurrence relationship with constant coefficients and initial conditions (1) ; it has a unique solution which cannot be "eyeballed".
The characteristic equation of (2) is $x^2-x+1=0$.
Its two roots are
$$x=\frac{1 \pm \sqrt{3}i}{2}$$
Otherwise said :
$$w=e^{i \pi/3} \ \text{and} \ \bar{w}=e^{-i \pi/3}.$$
Therefore, the general solution of (2) is :
$$D_n=aw^n+b\bar{w}^n\tag{3}$$
for constants $a$ and $b$. Here, $a$ and $b$ will be determined by initial conditions (1) :
$$\begin{cases}aw+b \bar{w}&=&1\\aw^2+b \bar{w}^2&=&0\end{cases},$$
a linear system whose solution is:
$$a=\frac{-iw}{\sqrt{3}}, \ \ b=\frac{i \bar{w}}{\sqrt{3}}\tag{4}$$
Plugging (4) into (3), we get:
$$D_n=\frac{i}{\sqrt{3}}\left(-w w^n+\bar{w}\bar{w}^n\right)=\frac{i}{\sqrt{3}}\left(- w^{n+1}+\bar{w}^{n+1}\right)$$
$$D_n=\frac{2}{\sqrt{3}}\sin \left((n+1)\frac{\pi}{3}\right)$$
giving (fortunately !) a real explicit expression for $D_n$.