The extended Euclidean plane can be identified with the extended complex plane, so that equations of complex numbers can be used to describe lines, circles and inversions.
A circle Γ {\displaystyle \Gamma } is the set of points z {\displaystyle z} in a plane that lie at radius r {\displaystyle r} from a center point γ . {\displaystyle \gamma .}
In the complex plane, γ {\displaystyle \gamma } is a complex number and Γ {\displaystyle \Gamma } is a set of complex numbers. Using the property that a complex number multiplied by its conjugate is the square of its modulus (its Euclidean distance from the origin), an implicit equation for Γ {\displaystyle \Gamma } is:
This is a homogeneous bivariate linear polynomial equation in terms of the complex variable z {\displaystyle z} and its conjugate z ¯ , {\displaystyle {\bar {z}},} of the form
where coefficients A {\displaystyle A} and D {\displaystyle D} are real, and B {\displaystyle B} and C {\displaystyle C} are complex conjugates.
By dividing by A {\displaystyle A} and then reversing the steps above, the radius r {\displaystyle r} and center γ {\displaystyle \gamma } can be recovered from any equation of this form. The equation represents a generalized circle in the plane when r {\displaystyle r} is real, which occurs when A D < B C {\displaystyle AD<BC} so that the squared radius r 2 = ( B C − A D ) / A 2 {\displaystyle r^{2}=(BC-AD)/A^{2}} is positive. When A {\displaystyle A} is zero, the equation defines a straight line.
That the reciprocal transformation z ↦ w = 1 / z {\displaystyle z\mapsto w=1/z} maps generalized circles to generalized circles is straight-forward to verify:
Lines through the origin ( A = D = 0 {\displaystyle A=D=0} ) map to lines through the origin; lines not through the origin ( A = 0 , D ≠ 0 {\displaystyle A=0,D\neq 0} ) map to circles through the origin; circles through the origin ( A ≠ 0 , D = 0 {\displaystyle A\neq 0,D=0} ) map to lines not through the origin; and circles not through the origin ( A ≠ 0 , D ≠ 0 {\displaystyle A\neq 0,D\neq 0} ) map to circles not through the origin.
The defining equation of a generalized circle
can be written as a matrix equation
Symbolically,
with coefficients placed into an invertible hermitian matrix C = C † {\displaystyle {\mathfrak {C}}={\mathfrak {C}}^{\dagger }} representing the circle, and z = ( z 1 ) T {\displaystyle \mathbf {z} ={\begin{pmatrix}z&1\end{pmatrix}}^{\text{T}}} a vector representing an extended complex number.
Two such matrices specify the same generalized circle if and only if one is a scalar multiple of the other.
To transform the generalized circle represented by C {\displaystyle {\mathfrak {C}}} by the Möbius transformation H , {\displaystyle {\mathfrak {H}},} apply the inverse of the Möbius transformation G = H − 1 {\displaystyle {\mathfrak {G}}={\mathfrak {H}}^{-1}} to the vector z {\displaystyle \mathbf {z} } in the implicit equation,
so the new circle can be represented by the matrix G T C G ¯ . {\displaystyle {\mathfrak {G}}^{\text{T}}{\mathfrak {C}}{\bar {\mathfrak {G}}}.}
Hitchman, Michael P. (2009). Geometry with an Introduction to Cosmic Topology. Jones & Bartlett. p. 43. https://books.google.com/books?id=yveG5B1few4C&pg=PA43 ↩