As 'Jean Marie' said, the set of points whose difference of distances from $F_1$ and $F_2$ is a fixed number, constitutes a hyperbola in the complex plane. In what follows it is assumed the $x$ coordinate is the real part of $z$, and $y$ is the imaginary part. To find the equation of this hyperbola, in the most direct way is as follows:
- The equation of the hyperbola in the rotated coordinate frame is
$ \dfrac{u^2}{a^2} - \dfrac{v^2}{b^2} = 1$
where the rotated coordinate is centered at the center of the hyperbola, and its $u$ axis extends along the vector pointing from $F_1$ to $F_2$.
Define the vector $\Delta F = F_2 - F_1 $, then $| \Delta F | = 2 c $ where $c$ is the distance between each of the two foci ($F_1$ , $F_2$) and the center of the hyperbola which is at $C = \frac{1}{2} (F_1 + F_2) $.
The relation between $c , a, b $ is as follows $c = \sqrt{a^2 + b^2} $
Also, we have a following relation that involves $d$, namely,
$ d = 2 a $
Thus, from $(4.)$, we can find $a$, then from $(3.), (2.)$ we can find $b$.
Now the equation of the hyperbola is almost ready. The rotation matrix that expresses the hyperbola with the equation given in $(1.)$ in the $x, y$ coordinates, we need to relate $(x, y)$ to $(u, v)$
$ \begin{bmatrix} x \\y \end{bmatrix} = C + R \begin{bmatrix} u \\ v \end{bmatrix} $
- The rotation matrix R is given by
$ R = \begin{bmatrix} \cos \theta && - \sin \theta \\ \sin \theta && \cos \theta \end{bmatrix} $
where $\theta$ is the angle that $\Delta F$ makes with the positive $x$ axis.
- Finally, the equation of the hyperbola is
$ (r - C)^T Q (r - C) = 1 $
where $Q = R D R^T$ with $D = \begin{bmatrix} \dfrac{1}{a^2} && 0 \\ 0 && - \dfrac{1}{b^2} \end{bmatrix} $ and $r = [x, y]^T $
- To find all the points on this hyperbola, define $w = R^T (r - C) $, then
$ r = C + R w $ and $w^T D w = 1$, from which it follows that $\dfrac{w_1^2}{a^2} - \dfrac{w_2^2}{b^2} = 1 $
Hence, we can take $w_1 = a \sec \theta$ and $w_2 = b \tan \theta $
From $(9.)$ we have a parameterization for vector $w = [w_1, w_2]^T $ which when we plug into $ r = C + R w $ we get $r$.