Every point of the $y = x^2$ parabola can be seen as the endpoint of a position vector of the form $< t, t^2>$.
So, rotating this curve counterclockwise can be assimilated to applying a linear transformation to this generic position vector, that is to say, applying the matrix the columns of which are the images of the bases $(1,0)$ and $(0,1)$ under a counterclockwise rotation by $R$ radians:
$\begin{bmatrix} \cos (R) & -\sin(R)\\\sin(R) & \cos(R)\end{bmatrix} \begin{pmatrix}t\\t^2\end{pmatrix} = \begin{pmatrix}\cos(R) t- \sin(R) t^2\\\sin(R) t + \cos(R) t^2\end{pmatrix}$
My question is, how to recover the cartesian equation of the rotated curve.
That is to say, how to eliminate the parameter $t$ in these equations :
$$ x = \cos(R) t- \sin(R) t^2$$
$$ y = \sin(R) t + \cos(R) t^2$$.
Note : my question is not as to what the cartesian form of the equation looks like, but as to how to recover it using this linear algebra method ( being given that the geometric prof of the rotation formula is not much intuitive).
You can start by writing the general form of a conic section $$ax^2+bxy+cy^2+dx+ey+f=0$$ Then plug in your forms for $x$ and $y$. Your equations are obeyed for any $t$ if you can identify the coefficients for each power of $t$ and set them to $0$ $$a(t\cos R-t^2\sin R)^2+b(t\cos R-t^2\sin R)(t\sin R+t^2\cos R)+\\c(t\sin R+t^2\cos R)^2+d(t\cos R-t^2\sin R)+e(t\sin R+t^2\cos R)+f=0$$
You can immediately see that $f=0$. Then for the coefficient of $t$ you get $$d\cos R+e\sin R=0$$ and so on, until the coefficient of $t^4$ is given by $$a\sin^2R+b\sin R\cos R+c\cos^2R=0$$ Notice that you have four equations with five unknowns, so you fix one of the $a,b,c,d,e$ values and calculate the rest.