Mobius Transformations

Suppose you want to map the upper half-plane conformally onto the open unit disk. Or you want to send three arbitrary points on a circle to three prescribed points on another circle. What single family of maps does all of this simultaneously? It sends lines and circles to lines and circles. It forms a group under composition. The answer is the Möbius transformations — the fractional linear maps z↦az+bcz+dz \mapsto \frac{az+b}{cz+d} with ad−bc≠0ad - bc \neq 0. They are the automorphisms of the Riemann sphere C^=C∪{∞}\widehat{\mathbb{C}} = \mathbb{C} \cup \{\infty\}. Understanding them is the gateway to hyperbolic geometry, elliptic functions, and the modular group. Möbius transformations matter because they are exactly the biholomorphic (conformal, bijective, holomorphic) self-maps of the extended complex plane. Every other conformal automorphism of C^\widehat{\mathbb{C}} is one of these. There are no others — a rigidity fact with no real analogue. They also act transitively and "3-transitively" on triples of points. This property is captured precisely by the invariant called the cross-ratio. This single invariant explains why circles map to circles (or lines). It governs when four points are concyclic. And it gives an explicit recipe for constructing the map sending any three points to any other three. The big picture: Möbius transformations unify Euclidean similarities, inversions, and the isometries of the hyperbolic plane. They combine into one algebraic package, PGL(2,C)\mathrm{PGL}(2,\mathbb{C}), acting on C^\widehat{\mathbb{C}}. Viewing C^\widehat{\mathbb{C}} as the Riemann sphere via stereographic projection makes the circle-preserving property geometrically transparent. These maps are literally the restrictions to the sphere of certain rigid motions of R3\mathbb{R}^3, composed with projections. Still, the cleanest proof is purely algebraic via the cross-ratio. This article develops the group structure. It proves the fundamental theorem that Möbius transformations preserve the class of "circles-or-lines." It establishes the cross-ratio invariance and its use in constructing explicit maps. It also works through concrete half-plane-to-disk and three-point examples. It closes by placing Möbius maps in their role as the first case study for Analytic Continuation and as the isometry group of hyperbolic space.

Key takeaways
  • A Möbius transformation is T(z)=az+bcz+dT(z) = \dfrac{az+b}{cz+d} with a,b,c,d∈Ca,b,c,d \in \mathbb{C}, ad−bc≠0ad-bc \neq 0, extended to C^\widehat{\mathbb{C}}.
  • They form a group under composition, isomorphic to PGL(2,C)=GL(2,C)/{λI}\mathrm{PGL}(2,\mathbb{C}) = GL(2,\mathbb{C})/\{\lambda I\}, acting by matrix multiplication on homogeneous coordinates.
  • Every Möbius transformation is a composite of translations, scalings/rotations, and the inversion z↦1/zz \mapsto 1/z.
  • The generalized circle (circle or line) family in C^\widehat{\mathbb{C}} is exactly preserved by every Möbius transformation.
  • The cross-ratio (z1,z2,z3,z4)(z_1,z_2,z_3,z_4) is invariant under Möbius maps and is real iff the four points are concyclic or collinear.
  • Given any two ordered triples of distinct points in C^\widehat{\mathbb{C}}, there is a unique Möbius transformation carrying one triple to the other.
  • Key idea: Möbius transformations are precisely the conformal automorphisms of the Riemann sphere, and the cross-ratio is their complete invariant on point-quadruples.

Where this lives today

Möbius transformations are the automorphism group of the hyperbolic plane in both the upper half-plane and disk models — the subgroup of Möbius maps with real coefficients and positive determinant, PSL(2,R)\mathrm{PSL}(2,\mathbb R), is exactly the isometry group of H\mathbb H with the hyperbolic metric, and this is the starting point for Fuchsian groups, modular forms, and Teichmüller theory. In complex dynamics, Möbius transformations classify the possible linearizations of rational maps near fixed points and appear as the "trivial" building blocks against which more complex dynamics (Julia sets, Kleinian groups) is measured. In computer graphics and complex analysis software, Möbius transformations give the standard method for conformally mapping polygonal or circular domains onto canonical shapes like the disk, a first step toward numerical Analytic Continuation and Riemann-mapping algorithms. In special relativity, the Möbius group PSL(2,C)\mathrm{PSL}(2,\mathbb C) acting on the celestial sphere (via stereographic projection, identified with C^\widehat{\mathbb C}) realizes the Lorentz group's action on the sky of an observer, connecting complex geometry to physics. In cryptography and coding theory, projective linear group actions related to PGL(2,q)\mathrm{PGL}(2,q) over finite fields provide highly symmetric combinatorial structures used in the construction of error-correcting codes and permutation groups with strong transitivity properties, a finite echo of the same three-point rigidity proven here.

Ask the tutor: How do Möbius transformations with real coefficients generate the isometries of the hyperbolic plane, and how does that connect to analytic continuation along paths in H\mathbb H?

DefinitionMöbius Transformation

Let a,b,c,d∈Ca,b,c,d \in \mathbb{C} satisfy ad−bc≠0ad - bc \neq 0. The Möbius transformation (or fractional linear transformation) associated to these coefficients is the map

T(z)=az+bcz+d.T(z) = \frac{az+b}{cz+d}.

Extend TT to the Riemann sphere C^=C∪{∞}\widehat{\mathbb{C}} = \mathbb{C} \cup \{\infty\} by setting

T(∞)={a/cc≠0∞c=0,T(−d/c)=∞  if c≠0.T(\infty) = \begin{cases} a/c & c \neq 0 \\ \infty & c = 0 \end{cases}, \qquad T(-d/c) = \infty \ \text{ if } c \neq 0.

With this extension, T:C^→C^T : \widehat{\mathbb{C}} \to \widehat{\mathbb{C}} is a bijection. Two coefficient tuples (a,b,c,d)(a,b,c,d) and (a′,b′,c′,d′)(a',b',c',d') give the same transformation if and only if (a′,b′,c′,d′)=λ(a,b,c,d)(a',b',c',d') = \lambda(a,b,c,d) for some λ∈C×\lambda \in \mathbb{C}^\times. Writing M=(abcd)∈GL(2,C)M = \begin{pmatrix} a & b \\ c & d\end{pmatrix} \in GL(2,\mathbb{C}), the assignment M↦TMM \mapsto T_M is a surjective group homomorphism from GL(2,C)GL(2,\mathbb{C}) onto the group Mo¨b\mathrm{M\ddot{o}b} of Möbius transformations, with kernel the nonzero scalar matrices C×I\mathbb{C}^\times I. Hence

Mo¨b  ≅  GL(2,C)/C×I  =  PGL(2,C).\mathrm{M\ddot{o}b} \;\cong\; GL(2,\mathbb{C})/\mathbb{C}^\times I \;=\; \mathrm{PGL}(2,\mathbb{C}).

Intuition

Think of a Möbius transformation as being built from three elementary geometric moves: translate, then rotate-and-scale, then invert. Concretely, if c≠0c \neq 0, the algebraic identity

az+bcz+d=ac−ad−bcc⋅1cz+d\frac{az+b}{cz+d} = \frac{a}{c} - \frac{ad-bc}{c}\cdot \frac{1}{cz+d}

shows that T=T4∘T3∘T2∘T1T = T_4 \circ T_3 \circ T_2 \circ T_1 where T1(z)=cz+dT_1(z) = cz + d (rotation-scaling plus translation), T2(z)=1/zT_2(z) = 1/z (inversion), T3(w)=−ad−bccwT_3(w) = -\frac{ad-bc}{c} w (rotation-scaling), and T4(w)=w+a/cT_4(w) = w + a/c (translation). Translations and rotation-scalings obviously send lines to lines and circles to circles (they are Euclidean similarities). The only nontrivial ingredient is inversion z↦1/zz \mapsto 1/z, and once we know inversion sends generalized circles to generalized circles, the whole group inherits this property by composition. The second key intuition is rigidity from three points. A Möbius transformation is determined by its values at any three distinct points of C^\widehat{\mathbb{C}}, and any three target values can be achieved. This is unlike affine maps (which need only two points to pin down, but can't achieve arbitrary triples) and unlike general conformal maps (which have infinitely many degrees of freedom). The cross-ratio packages this rigidity: it is the unique function of four points invariant under the group, and setting it up to equal a fixed value is exactly the equation of the Möbius map sending three basepoints to 0,1,∞0,1,\infty.

Figure
Building a Möbius map from translation, rotation-scaling, and inversion
z-plane: circle |z|=r T₁(z)=cz+d translated + rotated circle T₂(w)=1/w image: circle or line
TheoremMöbius transformations preserve generalized circles

Let T(z)=az+bcz+dT(z) = \dfrac{az+b}{cz+d} be a Möbius transformation (ad−bc≠0ad - bc \neq 0). Define a generalized circle in C^\widehat{\mathbb{C}} to be either (i) an ordinary circle {z∈C:∣z−p∣=r}\{z \in \mathbb{C} : |z - p| = r\} for some p∈Cp \in \mathbb{C}, r>0r > 0, or (ii) a set L∪{∞}L \cup \{\infty\} where LL is a straight line in C\mathbb{C}. Then TT maps every generalized circle onto a generalized circle. Moreover the class of generalized circles is exactly preserved: TT maps circles to circles or lines, and lines to circles or lines, with the line case for the image occurring precisely when the generalized circle passes through T−1(∞)T^{-1}(\infty).

Proof

Technique: algebraic characterization of generalized circles via a single real quadratic equation, then verification under the elementary generators of the Möbius group. Step 1: Algebraic form of a generalized circle. A subset Γ⊂C\Gamma \subset \mathbb{C} (before adjoining ∞\infty) is an ordinary circle or a line if and only if it is the solution set of an equation

Azzˉ+Bz+Bˉzˉ+C=0,(⋆)A z\bar z + B z + \bar B \bar z + C = 0, \qquad (\star)

where A,C∈RA, C \in \mathbb{R}, B∈CB \in \mathbb{C}, and ∣B∣2>AC|B|^2 > AC, with the further conditions:

  • if A≠0A \neq 0, (⋆)(\star) describes a circle (complete the square: dividing by AA, (⋆)(\star) becomes ∣z+B/A∣2=∣B∣2/A2−C/A>0|z + B/A|^2 = |B|^2/A^2 - C/A > 0, a genuine circle since the right side is positive);
  • if A=0A = 0, (⋆)(\star) becomes Bz+Bˉzˉ+C=0Bz + \bar B \bar z + C = 0, i.e. 2 Re(Bˉz)=−C2\,\mathrm{Re}(\bar B z) = -C, which is precisely the equation of a straight line (nondegenerate since B≠0B \neq 0, forced by ∣B∣2>AC=0|B|^2 > AC = 0).

Conversely, every circle ∣z−p∣=r|z-p|=r expands to zzˉ−pˉz−pzˉ+(∣p∣2−r2)=0z\bar z - \bar p z - p \bar z + (|p|^2 - r^2) = 0, matching (⋆)(\star) with A=1A=1, B=−pB = -p, C=∣p∣2−r2C = |p|^2-r^2, and ∣B∣2−AC=r2>0|B|^2 - AC = r^2 > 0. Every line Re(βˉz)=t\mathrm{Re}(\bar\beta z) = t (β≠0\beta \neq 0, t∈Rt\in\mathbb R) matches (⋆)(\star) with A=0A = 0, B=β/2B = \beta/2... wait, normalize: with A=0A=0, B=βB = \beta, C=−2tC = -2t, we need ∣B∣2>AC|B|^2 > AC, i.e. ∣β∣2>0|\beta|^2 > 0, true. So (⋆)(\star) with the stated sign condition is exactly the class of circles and lines. We adjoin ∞\infty to the line-solutions, and by convention a "generalized circle" is the solution set of (⋆)(\star) in C^\widehat{\mathbb{C}}, with ∞\infty included exactly when A=0A = 0. Step 2: Reduce to generators. By the factorization in the Intuition section, every Möbius transformation TT with c≠0c \neq 0 is a composite

T=T4∘T2∘T3∘T1,T1(z)=cz+d, T2(w)=1/w, T3(u)=−ad−bccu, T4(v)=v+ac,T = T_4 \circ T_2 \circ T_3 \circ T_1, \quad T_1(z) = cz+d,\ T_2(w)=1/w,\ T_3(u) = -\tfrac{ad-bc}{c}u,\ T_4(v) = v + \tfrac{a}{c},

and if c=0c = 0 then T(z)=adz+bdT(z) = \frac{a}{d} z + \frac{b}{d} is already affine (a composite of a scaling/rotation and a translation). Since the class of generalized circles is preserved under composition of maps that individually preserve it, it suffices to check three types of generators: (a) translations z↦z+tz \mapsto z + t, (b) scalings/rotations z↦λzz \mapsto \lambda z (λ≠0\lambda \neq 0), and (c) inversion z↦1/zz \mapsto 1/z. Step 3: Translations and rotation-scalings. Let w=z+tw = z + t. Substituting z=w−tz = w - t into (⋆)(\star):

A(w−t)(w−t)‾+B(w−t)+Bˉ(w−t)‾+C=0,A(w-t)\overline{(w-t)} + B(w-t) + \bar B \overline{(w-t)} + C = 0,

which expands to Awwˉ+(B−At)w+(B−At)‾wˉ+C′=0A w\bar w + (B - At)w + \overline{(B-At)}\bar w + C' = 0 for a suitable real constant C′C' (direct computation: C′=C−Bt−Bˉtˉ+A∣t∣2C' = C - B t - \bar B \bar t + A|t|^2, real since A,C∈RA,C \in \mathbb R and the middle terms are conjugates of each other up to the real coefficient AA). This is again of form (⋆)(\star) with the same AA, new B′=B−AtB' = B - At; the discriminant condition ∣B′∣2>AC′|B'|^2 > AC' is preserved because a Euclidean translation cannot change whether a curve is a genuine circle or line (this can also be checked directly, but geometric preservation of circles/lines under translation is elementary). So translations preserve the class, with AA unchanged — in particular preserving whether ∞\infty is in the generalized circle. Similarly for w=λzw = \lambda z with λ≠0\lambda \ne 0: substitute z=w/λz = w/\lambda into (⋆)(\star) to get

A∣λ∣2wwˉ+Bλw+Bˉλˉwˉ+C=0,\frac{A}{|\lambda|^2} w\bar w + \frac{B}{\lambda} w + \frac{\bar B}{\bar\lambda}\bar w + C = 0,

multiply through by ∣λ∣2|\lambda|^2 to get Awwˉ+(Bλˉ)w+(Bˉλ)wˉ+C∣λ∣2=0A w\bar w + (B\bar\lambda) w + (\bar B \lambda)\bar w + C|\lambda|^2 = 0, again of form (⋆)(\star) with AA unchanged (up to an overall positive rescale which doesn't affect the sign structure), B′′=BλˉB'' = B\bar\lambda, C′′=C∣λ∣2C'' = C|\lambda|^2, and one checks ∣B′′∣2−AC′′=∣λ∣2(∣B∣2−AC)>0|B''|^2 - A C'' = |\lambda|^2(|B|^2 - AC) > 0 is preserved. So rotation-scalings preserve the class and preserve whether A=0A = 0. Step 4: Inversion. Let w=1/zw = 1/z, i.e. z=1/wz = 1/w (for z,w≠0z, w \neq 0). Substitute into (⋆)(\star):

A1w1wˉ+B1w+Bˉ1wˉ+C=0.A\frac{1}{w}\frac{1}{\bar w} + B\frac{1}{w} + \bar B \frac{1}{\bar w} + C = 0.

Multiply both sides by wwˉ=∣w∣2≠0w \bar w = |w|^2 \neq 0:

A+Bwˉ+Bˉw+Cwwˉ=0,A + B \bar w + \bar B w + C w \bar w = 0,

i.e.

C wwˉ+Bˉw+Bwˉ+A=0.C\, w\bar w + \bar B w + B \bar w + A = 0.

This is exactly of the form (⋆)(\star) in the variable ww with new coefficients A∗=CA^* = C, B∗=BˉB^* = \bar B, C∗=AC^* = A (all real/complex-conjugate-compatible as required since A,CA, C real), and the discriminant condition becomes ∣B∗∣2>A∗C∗|B^*|^2 > A^*C^*, i.e. ∣Bˉ∣2>CA|\bar B|^2 > CA, i.e. ∣B∣2>AC|B|^2 > AC — identical to the original condition. So inversion maps the solution set of (⋆)(\star) (minus possibly the point z=0z=0 or w=0w=0) to the solution set of the transformed equation, again a generalized circle. We must also handle z=0z=0 and w=∞w=\infty, z=∞z=\infty and w=0w=0: if 00 satisfies (⋆)(\star), that means C=0C = 0, so the original curve passes through the origin; the transformed equation has A∗=C=0A^* = C = 0, meaning the image curve is a line (through the point at infinity, i.e. genuinely unbounded) — consistent with the map z↦1/zz\mapsto 1/z sending a circle/line through 00 to a line. Conversely if A=0A = 0 (original is a line, containing ∞\infty), then A∗=CA^* = C; the image equation has "circle indicator" A∗=CA^* = C, and by symmetry the image is a line iff C=0C = 0 iff the original line passes through the origin. This matches the geometric fact that inversion sends a line through the origin to itself (a line) and a line missing the origin to a circle through the origin. Step 5: Conclusion. Since (⋆)(\star) exactly characterizes generalized circles (Step 1), and each generator (Steps 3–4) transforms a solution set of an equation of form (⋆)(\star) into the solution set of another equation of the same form with the same nondegeneracy condition, by induction (Step 2) every Möbius transformation TT carries generalized circles to generalized circles. The "circle →\to line" case occurs exactly when Afinal=0A^{\text{final}} = 0; tracing through the composition, this happens precisely when T−1(∞)T^{-1}(\infty) lies on the original curve, since ∞\infty enters the image curve exactly when the coefficient of zzˉz\bar z vanishes after transformation, which by Step 4's inversion step corresponds to the pole of TT lying on the source curve. ■\blacksquare

∎
LemmaCross-ratio invariance

For four distinct points z1,z2,z3,z4∈C^z_1, z_2, z_3, z_4 \in \widehat{\mathbb{C}} define the cross-ratio

(z1,z2,z3,z4)=(z1−z3)(z2−z4)(z1−z4)(z2−z3),(z_1, z_2, z_3, z_4) = \frac{(z_1 - z_3)(z_2-z_4)}{(z_1-z_4)(z_2-z_3)},

with the convention that if one zi=∞z_i = \infty, the two factors containing it are replaced by 11 (formally, take the limit). Then for every Möbius transformation TT,

(Tz1,Tz2,Tz3,Tz4)=(z1,z2,z3,z4).(T z_1, Tz_2, Tz_3, Tz_4) = (z_1,z_2,z_3,z_4).
Proof

Technique: direct algebraic computation, reduced to the three generator types, using that the cross-ratio of Tz1,…,Tz4T z_1,\dots,Tz_4 is a rational function of z1,…,z4z_1,\dots,z_4 we can simplify directly for a general TT. Write T(z)=az+bcz+dT(z) = \frac{az+b}{cz+d}, ad−bc≠0ad-bc\ne0. For any i≠ji \ne j with zi,zj≠∞z_i, z_j \ne \infty,

Tzi−Tzj=azi+bczi+d−azj+bczj+d=(azi+b)(czj+d)−(azj+b)(czi+d)(czi+d)(czj+d).Tz_i - Tz_j = \frac{az_i+b}{cz_i+d} - \frac{az_j+b}{cz_j+d} = \frac{(az_i+b)(cz_j+d) - (az_j+b)(cz_i+d)}{(cz_i+d)(cz_j+d)}.

Expand the numerator:

(azi+b)(czj+d)−(azj+b)(czi+d)=aczizj+adzi+bczj+bd−aczizj−adzj−bczi−bd(az_i+b)(cz_j+d) - (az_j+b)(cz_i+d) = ac z_iz_j + adz_i + bcz_j + bd - ac z_iz_j - adz_j - bcz_i - bd
=ad(zi−zj)−bc(zi−zj)=(ad−bc)(zi−zj).= ad(z_i - z_j) - bc(z_i-z_j) = (ad-bc)(z_i-z_j).

Hence

Tzi−Tzj=(ad−bc)(zi−zj)(czi+d)(czj+d).(†)Tz_i - Tz_j = \frac{(ad-bc)(z_i - z_j)}{(cz_i+d)(cz_j+d)}. \tag{$\dagger$}

Now form the cross-ratio of the images, using (†)(\dagger) for each of the four factors (Tz1−Tz3)(Tz_1-Tz_3), (Tz2−Tz4)(Tz_2-Tz_4), (Tz1−Tz4)(Tz_1-Tz_4), (Tz2−Tz3)(Tz_2-Tz_3):

(Tz1,Tz2,Tz3,Tz4)=(ad−bc)(z1−z3)(cz1+d)(cz3+d)⋅(ad−bc)(z2−z4)(cz2+d)(cz4+d)(ad−bc)(z1−z4)(cz1+d)(cz4+d)⋅(ad−bc)(z2−z3)(cz2+d)(cz3+d).(Tz_1,Tz_2,Tz_3,Tz_4) = \frac{\dfrac{(ad-bc)(z_1-z_3)}{(cz_1+d)(cz_3+d)}\cdot \dfrac{(ad-bc)(z_2-z_4)}{(cz_2+d)(cz_4+d)}}{\dfrac{(ad-bc)(z_1-z_4)}{(cz_1+d)(cz_4+d)}\cdot \dfrac{(ad-bc)(z_2-z_3)}{(cz_2+d)(cz_3+d)}}.

Every factor (czk+d)(cz_k+d) for k=1,2,3,4k=1,2,3,4 appears exactly once in the numerator's denominator-product and once in the denominator's denominator-product (each zkz_k appears in exactly two of the four original differences, once "up" and once "down" combinatorially — check: z1z_1 appears in (z1−z3)(z_1-z_3) and (z1−z4)(z_1-z_4), contributing (cz1+d)(cz_1+d) to both numerator and denominator of the big fraction). Concretely, all four factors (cz1+d),(cz2+d),(cz3+d),(cz4+d)(cz_1+d), (cz_2+d), (cz_3+d), (cz_4+d) appear exactly once in the numerator's denominator and exactly once in the denominator's denominator, so they cancel completely. The two factors of (ad−bc)(ad-bc) in the numerator cancel against the two in the denominator (nonzero since ad−bc≠0ad-bc \ne 0). We are left with

(Tz1,Tz2,Tz3,Tz4)=(z1−z3)(z2−z4)(z1−z4)(z2−z3)=(z1,z2,z3,z4).(Tz_1,Tz_2,Tz_3,Tz_4) = \frac{(z_1-z_3)(z_2-z_4)}{(z_1-z_4)(z_2-z_3)} = (z_1,z_2,z_3,z_4).

If one of the ziz_i equals ∞\infty, or one of the TziTz_i involves the pole of TT, the identity persists by continuity: both sides are continuous (indeed rational) functions of z1,…,z4z_1,\dots,z_4 on C^4\widehat{\mathbb{C}}^4 minus diagonals, and the identity holds on a dense open set, hence everywhere by continuity of both sides. ■\blacksquare

∎
CorollaryThree-point rigidity and the concyclicity criterion

(a) Given any two ordered triples of distinct points (z1,z2,z3)(z_1,z_2,z_3) and (w1,w2,w3)(w_1,w_2,w_3) in C^\widehat{\mathbb{C}}, there exists a unique Möbius transformation TT with Tzi=wiTz_i = w_i for i=1,2,3i=1,2,3. (b) Four distinct points z1,z2,z3,z4∈Cz_1,z_2,z_3,z_4 \in \mathbb{C} lie on a common generalized circle if and only if (z1,z2,z3,z4)∈R(z_1,z_2,z_3,z_4) \in \mathbb{R}.

Proof

(a) Existence. Define S(z)=(z,z1,z2,z3)S(z) = (z, z_1, z_2, z_3), i.e.

S(z)=(z−z2)(z1−z3)(z−z3)(z1−z2).S(z) = \frac{(z-z_2)(z_1-z_3)}{(z-z_3)(z_1-z_2)}.

SS is a Möbius transformation (its coefficients form an invertible matrix because z1,z2,z3z_1,z_2,z_3 are distinct — direct check: the determinant of the associated matrix is a nonzero multiple of (z1−z2)(z1−z3)(z2−z3)≠0(z_1-z_2)(z_1-z_3)(z_2-z_3)\neq 0), and S(z1)=1S(z_1) = 1... let us verify directly: S(z1)=(z1−z2)(z1−z3)(z1−z3)(z1−z2)=1S(z_1) = \frac{(z_1-z_2)(z_1-z_3)}{(z_1-z_3)(z_1-z_2)} = 1, and one checks S(z2)=0S(z_2) = 0 (numerator vanishes) and S(z3)=∞S(z_3) = \infty (denominator vanishes). Similarly define R(w)=(w,w1,w2,w3)R(w) = (w,w_1,w_2,w_3) with R(w1)=1,R(w2)=0,R(w3)=∞R(w_1)=1, R(w_2)=0,R(w_3)=\infty. Then T:=R−1∘ST := R^{-1}\circ S is Möbius (composition and inverse of Möbius maps are Möbius, since Mo¨b\mathrm{M\ddot ob} is a group under composition, matching matrix multiplication and inversion in PGL(2,C)\mathrm{PGL}(2,\mathbb C)), and T(zi)=R−1(S(zi))=wiT(z_i) = R^{-1}(S(z_i))= w_i for i=1,2,3i=1,2,3 by construction. Uniqueness. Suppose T1,T2T_1, T_2 both send (z1,z2,z3)↦(w1,w2,w3)(z_1,z_2,z_3)\mapsto(w_1,w_2,w_3). Then U:=T2−1∘T1U := T_2^{-1}\circ T_1 fixes z1,z2,z3z_1,z_2,z_3. A nonidentity Möbius transformation U(z)=az+bcz+dU(z) = \frac{az+b}{cz+d} has at most two fixed points in C^\widehat{\mathbb C}: solving U(z)=zU(z)=z gives cz2+(d−a)z−b=0cz^2 + (d-a)z - b = 0 if c≠0c\ne 0 (a quadratic, at most 2 roots, and ∞\infty is not a fixed point since c≠0c\ne0 means U(∞)=a/c≠∞U(\infty)=a/c\ne\infty), or if c=0c=0, U(z)=adz+bdU(z) = \frac{a}{d}z+\frac bd which fixes ∞\infty and at most one finite point (if a≠da\ne d) or is the identity (if a=d,b=0a=d, b=0). Either way a non-identity Möbius map has at most 2 fixed points. Since UU fixes three distinct points z1,z2,z3z_1,z_2,z_3, UU must be the identity, so T1=T2T_1 = T_2. (b) By the cross-ratio invariance lemma, applying S(z)=(z,z1,z2,z3)S(z) = (z,z_1,z_2,z_3) from part (a)'s construction, we have (z1,z2,z3,z4)=(Sz1,Sz2,Sz3,Sz4)=(1,0,∞,Sz4)=Sz4(z_1,z_2,z_3,z_4) = (Sz_1,Sz_2,Sz_3,Sz_4) = (1,0,\infty, Sz_4) = Sz_4 (direct check of the degenerate cross-ratio with entries 1,0,∞1,0,\infty collapses to the fourth argument itself: (1,0,∞,w)=lim⁡Z→∞(1−∞)(0−w)(1−w)(0−∞)=0−w−(1−w)⋅−1−1(1,0,\infty,w) = \lim_{Z\to\infty}\frac{(1-\infty)(0-w)}{(1-w)(0-\infty)} = \frac{0-w}{-(1-w)}\cdot\frac{-1}{-1}; computing the limit carefully by clearing Z=∞Z=\infty symbolically gives (1,0,∞,w)=w(1,0,\infty,w) = w). So (z1,z2,z3,z4)=S(z4)(z_1,z_2,z_3,z_4) = S(z_4). Since SS is a Möbius transformation with S(z1)=1,S(z2)=0,S(z3)=∞S(z_1)=1, S(z_2)=0,S(z_3)=\infty, and by Möbius transformations preserve generalized circles SS maps the generalized circle Γ\Gamma through z1,z2,z3z_1,z_2,z_3 (unique such circle, since three distinct points determine a unique circle or line — standard Euclidean fact, or apply the theorem's Step 1 characterization: three points impose three real linear conditions on the 3 real parameters (A,B,C)(A,B,C) up to scale) onto a generalized circle through 1,0,∞1, 0, \infty. A generalized circle through ∞\infty is a line; the line through 00 and 11 is R\mathbb{R} itself. So S(Γ)=R^=R∪{∞}S(\Gamma) = \widehat{\mathbb{R}} = \mathbb{R}\cup\{\infty\}. Therefore z4∈Γz_4 \in \Gamma if and only if S(z4)∈R^S(z_4) \in \widehat{\mathbb R}, i.e. iff (z1,z2,z3,z4)=S(z4)∈R∪{∞}(z_1,z_2,z_3,z_4) = S(z_4) \in \mathbb R \cup \{\infty\}; excluding the case S(z4)=∞S(z_4)=\infty (which happens iff z4=z3z_4 = z_3, excluded since points are distinct), we get (z1,z2,z3,z4)∈R(z_1,z_2,z_3,z_4)\in\mathbb R iff z4∈Γz_4 \in \Gamma, as claimed. ■\blacksquare

∎

Worked examples

Example 1: The Cayley-type map from the upper half-plane to the disk, via three points. We construct explicitly a Möbius transformation sending the upper half-plane H={z:Im z>0}\mathbb{H} = \{z : \mathrm{Im}\,z > 0\} onto the open unit disk D={w:∣w∣<1}\mathbb D = \{w : |w| < 1\}, using the three-point method with an asymmetric choice of boundary points: we send z1=1,z2=0,z3=−1z_1 = 1, z_2 = 0, z_3 = -1 (three points on ∂H=R\partial \mathbb H = \mathbb R, in this order) to w1=1,w2=i,w3=−1w_1 = 1, w_2 = i, w_3 = -1 (three points on ∂D\partial \mathbb D, matching orientation). By the cross-ratio construction, T(z)=R−1(S(z))T(z) = R^{-1}(S(z)) where S(z)=(z,1,0,−1)S(z) = (z,1,0,-1) and R(w)=(w,1,i,−1)R(w) = (w,1,i,-1). Compute SS directly:

S(z)=(z−0)(1−(−1))(z−(−1))(1−0)=2zz+1.S(z) = \frac{(z-0)(1-(-1))}{(z-(-1))(1-0)} = \frac{2z}{z+1}.

Compute RR:

R(w)=(w−i)(1−(−1))(w−(−1))(1−i)=2(w−i)(w+1)(1−i).R(w) = \frac{(w-i)(1-(-1))}{(w-(-1))(1-i)} = \frac{2(w-i)}{(w+1)(1-i)}.

We want T=R−1∘ST = R^{-1}\circ S, i.e. solve R(T(z))=S(z)R(T(z)) = S(z) for T(z)T(z). Set ζ=S(z)=2zz+1\zeta = S(z) = \frac{2z}{z+1} and solve R(w)=ζR(w) = \zeta for ww:

2(w−i)(w+1)(1−i)=ζ⟹2(w−i)=ζ(1−i)(w+1)\frac{2(w-i)}{(w+1)(1-i)} = \zeta \quad\Longrightarrow\quad 2(w-i) = \zeta(1-i)(w+1)
2w−2i=ζ(1−i)w+ζ(1−i)⟹w(2−ζ(1−i))=2i+ζ(1−i)2w - 2i = \zeta(1-i) w + \zeta(1-i) \quad\Longrightarrow\quad w\big(2 - \zeta(1-i)\big) = 2i + \zeta(1-i)
w=2i+ζ(1−i)2−ζ(1−i).w = \frac{2i + \zeta(1-i)}{2 - \zeta(1-i)}.

Now substitute ζ=2zz+1\zeta = \frac{2z}{z+1}:

w=2i(z+1)+2z(1−i)2(z+1)−2z(1−i)=2iz+2i+2z−2iz2z+2−2z+2iz=2i+2z2+2iz=z+i1+iz.w = \frac{2i(z+1) + 2z(1-i)}{2(z+1) - 2z(1-i)} = \frac{2iz + 2i + 2z - 2iz}{2z+2 - 2z+2iz} = \frac{2i + 2z}{2 + 2iz} = \frac{z+i}{1+iz}.

So

T(z)=z+iiz+1.T(z) = \frac{z+i}{iz+1}.

Verification. Check the three basepoints: T(1)=1+ii+1=1T(1) = \frac{1+i}{i+1} = 1. ✓. T(0)=i1=iT(0) = \frac{i}{1} = i. ✓. T(−1)=−1+i−i+1=−1+i1−i=(−1+i)(1+i)(1−i)(1+i)=−1−i+i+i22=−1−12=−1T(-1) = \frac{-1+i}{-i+1} = \frac{-1+i}{1-i} = \frac{(-1+i)(1+i)}{(1-i)(1+i)} = \frac{-1-i+i+i^2}{2} = \frac{-1-1}{2} = -1. ✓. Check that TT sends H\mathbb H into D\mathbb D: take z=iz = i (a representative interior point), T(i)=i+ii⋅i+1=2i−1+1=2i0T(i) = \frac{i+i}{i\cdot i+1} = \frac{2i}{-1+1} = \frac{2i}{0} — undefined! This signals ii is the pole of TT, i.e. T(i)=∞T(i) = \infty; indeed iz+1=0  ⟺  z=iiz+1=0 \iff z = i. So the pole of TT lies exactly on ∂H\partial \mathbb H's "point at infinity" partner... actually z=i∈Hz=i \in \mathbb H itself, not on the boundary — let's re-examine: we need T(H)=DT(\mathbb H) = \mathbb D, and a pole inside H\mathbb H would be wrong. Let's recheck the sign/orientation. Try instead z=2i∈Hz = 2i \in \mathbb H: T(2i)=2i+ii(2i)+1=3i−2+1=3i−1=−3iT(2i) = \frac{2i+i}{i(2i)+1} = \frac{3i}{-2+1} = \frac{3i}{-1} = -3i, and ∣−3i∣=3>1|-3i| = 3 > 1, so TT sends H\mathbb H to the exterior of D\mathbb D with this coefficient choice — the orientation of the boundary triple (1,0,−1)↦(1,i,−1)(1,0,-1)\mapsto(1,i,-1) traversed R\mathbb R and ∂D\partial\mathbb D in opposite senses relative to their interiors.

Correction. The standard fix: since a Möbius map sending ∂H→∂D\partial\mathbb H \to \partial \mathbb D sends H\mathbb H to one of the two complementary regions (D\mathbb D or its exterior), and we found it sends H\mathbb H to the exterior, we instead use T∗(z)=−z+iiz−1⋅(−1)T^*(z) = \frac{-z + i}{iz - 1}\cdot(-1)... more simply, compose with the map w↦1/wˉw \mapsto 1/\bar w is not Möbius (antiholomorphic); instead choose the conjugate boundary correspondence z3=−1↦w3=−1z_3=-1 \mapsto w_3 = -1 was fine, but let's instead directly test the well-known map T0(z)=z−iz+iT_0(z) = \frac{z-i}{z+i} and see it does work, then reconcile. Indeed the classical Cayley transform is T0(z)=z−iz+iT_0(z) = \frac{z-i}{z+i}; check T0(i)=0∈DT_0(i) = 0 \in \mathbb D ✓, and boundary points: T0(1)=1−i1+i=(1−i)22=1−2i−12=−iT_0(1) = \frac{1-i}{1+i} = \frac{(1-i)^2}{2} = \frac{1-2i-1}{2} = -i, T0(0)=−ii=−1T_0(0) = \frac{-i}{i} = -1, T0(−1)=−1−i−1+i=(−1−i)(−1−i)(−1+i)(−1−i)=(1+i)22=2i2=iT_0(-1) = \frac{-1-i}{-1+i} = \frac{(-1-i)(-1-i)}{(-1+i)(-1-i)} = \frac{(1+i)^2}{2} = \frac{2i}{2}=i. So the correct correspondence for our chosen basepoints, sending H→D\mathbb H \to \mathbb D, is (1,0,−1)↦(−i,−1,i)(1,0,-1) \mapsto (-i,-1,i), not (1,i,−1)(1,i,-1) as we assumed. The lesson: not every boundary triple-to-triple assignment respecting "the same three points" sends interior to interior — one must fix orientation by testing an interior point, exactly as we did. Our computed T(z)=z+iiz+1T(z) = \frac{z+i}{iz+1} correctly implements (1,0,−1)↦(1,i,−1)(1,0,-1)\mapsto (1,i,-1), and it sends H\mathbb{H} to the exterior of D\mathbb D; post-composing with the Möbius inversion J(w)=1/wJ(w) = 1/w (which swaps Dc\mathbb D^{c} and D\mathbb D appropriately combined with reflection) is not quite right either since 1/w1/w for ∣w∣>1|w|>1 gives ∣1/w∣<1|1/w|<1 — so J∘TJ\circ T works:

(J∘T)(z)=1T(z)=iz+1z+i.(J\circ T)(z) = \frac{1}{T(z)} = \frac{iz+1}{z+i}.

Check: (J∘T)(2i)=i(2i)+12i+i=−2+13i=−13i=i3(J\circ T)(2i) = \frac{i(2i)+1}{2i+i} = \frac{-2+1}{3i} = \frac{-1}{3i} = \frac{i}{3}, and ∣i/3∣=1/3<1|i/3| = 1/3 < 1. ✓ Interior goes to interior. And boundary points: (J∘T)(1)=i+11+i=1(J \circ T)(1) = \frac{i+1}{1+i}=1, (J∘T)(0)=1i=−i(J\circ T)(0) = \frac{1}{i} = -i, (J∘T)(−1)=−i+1−1+i=(1−i)−(1−i)=−1(J\circ T)(-1) = \frac{-i+1}{-1+i} = \frac{(1-i)}{-(1-i)} = -1. So the honest final answer, sending H→D\mathbb H \to \mathbb D with 1↦1,0↦−i,−1↦−11 \mapsto 1, 0 \mapsto -i, -1\mapsto -1, is

T(z)=iz+1z+i.\boxed{T(z) = \frac{iz+1}{z+i}}.

This exercise illustrates a genuine subtlety: the three-point construction determines a Möbius transformation carrying one triple to another, but whether it sends a given side of the first generalized circle to the correct side of the image circle must be separately checked at one interior point, since both "sides" are individually mapped onto by some correspondence of boundary triples.

Example 2: Cross-ratio test for concyclicity, four asymmetric points. Let z1=2,z2=1+i,z3=−1,z4=3−2iz_1 = 2, z_2 = 1+i, z_3 = -1, z_4 = 3-2i. Are these four points concyclic (or collinear)? Compute the cross-ratio (z1,z2,z3,z4)=(z1−z3)(z2−z4)(z1−z4)(z2−z3)(z_1,z_2,z_3,z_4) = \dfrac{(z_1-z_3)(z_2-z_4)}{(z_1-z_4)(z_2-z_3)}. z1−z3=2−(−1)=3z_1 - z_3 = 2-(-1) = 3. z2−z4=(1+i)−(3−2i)=−2+3iz_2 - z_4 = (1+i)-(3-2i) = -2+3i. z1−z4=2−(3−2i)=−1+2iz_1 - z_4 = 2-(3-2i) = -1+2i. z2−z3=(1+i)−(−1)=2+iz_2 - z_3 = (1+i)-(-1) = 2+i. Numerator: 3⋅(−2+3i)=−6+9i3\cdot(-2+3i) = -6+9i. Denominator: (−1+2i)(2+i)=−2−i+4i+2i2=−2+3i−2=−4+3i(-1+2i)(2+i) = -2 -i +4i +2i^2 = -2+3i-2 = -4+3i. Cross-ratio =−6+9i−4+3i= \dfrac{-6+9i}{-4+3i}. Multiply numerator and denominator by the conjugate −4+3i‾=−4−3i\overline{-4+3i} = -4-3i:

(−6+9i)(−4−3i)(−4+3i)(−4−3i)=24+18i−36i−27i216+9=24−18i+2725=51−18i25.\frac{(-6+9i)(-4-3i)}{(-4+3i)(-4-3i)} = \frac{24+18i-36i-27i^2}{16+9} = \frac{24 -18i +27}{25} = \frac{51 - 18i}{25}.

This is 5125−1825i\frac{51}{25} - \frac{18}{25}i, which has nonzero imaginary part, so the cross-ratio is not real. By the Corollary (concyclicity criterion) proved above, these four points are not concyclic and not collinear.

Cross-check via direct circle-fitting. Find the circle through z1=2,z2=1+i,z3=−1z_1=2, z_2=1+i, z_3=-1 and test z4z_4. The general circle equation x2+y2+Dx+Ey+F=0x^2+y^2+Dx+Ey+F=0 through (2,0)(2,0): 4+2D+F=04+2D+F=0. Through (1,1)(1,1): 1+1+D+E+F=0⇒D+E+F=−21+1+D+E+F=0 \Rightarrow D+E+F=-2. Through (−1,0)(-1,0): 1−D+F=0⇒F=D−11-D+F=0 \Rightarrow F = D-1. From the first equation: F=−4−2DF = -4-2D. Combine with F=D−1F=D-1: D−1=−4−2D⇒3D=−3⇒D=−1D - 1 = -4-2D \Rightarrow 3D = -3 \Rightarrow D=-1, so F=−1−1=−2F = -1-1=-2. From the second equation: D+E+F=−2⇒−1+E−2=−2⇒E=1D+E+F=-2 \Rightarrow -1+E-2=-2 \Rightarrow E=1. So the circle is x2+y2−x+y−2=0x^2+y^2 - x + y - 2 = 0, i.e. (x−12)2+(y+12)2=2+14+14=52(x-\tfrac12)^2+(y+\tfrac12)^2 = 2 + \tfrac14+\tfrac14 = \tfrac52, center (12,−12)(\tfrac12,-\tfrac12), radius 5/2\sqrt{5/2}. Test z4=3−2i=(3,−2)z_4 = 3-2i = (3,-2): 32+(−2)2−3+(−2)−2=9+4−3−2−2=6≠03^2+(-2)^2 -3 + (-2) - 2 = 9+4-3-2-2 = 6 \ne 0. Since 6≠06 \ne 0, z4z_4 is not on the circle through z1,z2,z3z_1,z_2,z_3 — confirming the cross-ratio test's conclusion that the four points are not concyclic, by an entirely independent computation.

CounterexampleDropping ad−bc≠0ad - bc \neq 0 collapses the map to a constant

The hypothesis ad−bc≠0ad-bc \ne 0 in the definition of a Möbius transformation is not a technical nicety — without it, TT is not a bijection and none of the theory applies. Take a=2,b=4,c=1,d=2a=2, b=4, c=1, d=2, so ad−bc=4−4=0ad-bc = 4-4=0. Then

T(z)=2z+4z+2=2(z+2)z+2=2for all z≠−2,T(z) = \frac{2z+4}{z+2} = \frac{2(z+2)}{z+2} = 2 \quad \text{for all } z \ne -2,

a constant function, not injective, with no well-defined value forced at z=−2z=-2 beyond the removable identification T≡2T\equiv 2. Such a "degenerate" fractional linear expression is excluded from Mo¨b\mathrm{M\ddot ob} precisely because the cross-ratio invariance lemma's proof used ad−bc≠0ad-bc\ne 0 to divide by a nonzero quantity in (†)(\dagger); with ad−bc=0ad-bc=0, every cross-ratio of images collapses to an indeterminate 0/00/0 or to the constant value's degenerate cross-ratio (undefined, since repeated points give an undefined cross-ratio). The three-point rigidity corollary also fails completely: a constant map cannot send three distinct points to three distinct images, so the entire "unique map through three points" machinery presupposes ad−bc≠0ad-bc\neq0 from the start.

Scope, edge cases & common traps

SituationWhat happensCommon trap
c=0c = 0TT is affine, T(∞)=∞T(\infty)=\inftyForgetting TT still extends to a bijection of C^\widehat{\mathbb C}, fixing ∞\infty
c≠0c \neq 0T(−d/c)=∞T(-d/c)=\infty, T(∞)=a/cT(\infty)=a/cOmitting these two special values breaks bijectivity on C^\widehat{\mathbb C}
One of z1,…,z4z_1,\dots,z_4 is ∞\inftyCross-ratio defined by continuity/limitPlugging ∞\infty naively into the formula gives ∞/∞\infty/\infty
Checking image "side" of a circleMust test an interior pointAssuming boundary correspondence alone determines the correct half-plane/disk direction
ad−bc=0ad-bc=0Map degenerates to a constantTreating it as a valid (non-bijective) Möbius transformation

The mathematician behind it

Origins · 1 minAugust Ferdinand Möbius and how this was discovered
AF
August Ferdinand Möbius
1790–1868 · early 19th-century Germany, projective and analytic geometry

Möbius trained under Gauss at Göttingen and spent most of his career at Leipzig, working at the boundary of projective geometry, mechanics, and what would become topology. He introduced homogeneous barycentric coordinates and systematized the study of transformations that preserve incidence and cross-ratio, laying the groundwork for what we now call Möbius (fractional linear) transformations. He is also the namesake of the Möbius strip and the Möbius function in number theory, reflecting a career that moved fluidly between geometry, combinatorics, and astronomy (he directed the Leipzig observatory).

History
- 1827: Möbius publishes Der barycentrische Calcul, introducing projective/barycentric coordinate methods that underlie the cross-ratio.
- 1850s: The cross-ratio and fractional linear transformations become standard tools in projective geometry, studied by Möbius, Steiner, and others.
- 1854: Riemann's work on functions of a complex variable and the sphere model gives Möbius transformations their modern role as automorphisms of C^\widehat{\mathbb C}.
- 1882: Poincaré and Klein develop the connection between Möbius transformations (real coefficients, unit disk/upper half-plane preserving) and models of hyperbolic geometry.
- 20th century: Möbius transformations become foundational in complex dynamics, Kleinian groups, and the theory of quasiconformal mappings.
Why must Möbius transformations be extended to C^\widehat{\mathbb C} rather than just C\mathbb C?

On C\mathbb C alone, T(z)=az+bcz+dT(z) = \frac{az+b}{cz+d} with c≠0c \neq 0 is undefined at z=−d/cz = -d/c and never attains the value a/ca/c, so it fails to be a bijection of C\mathbb C onto itself. Extending the domain and codomain to the Riemann sphere C^=C∪{∞}\widehat{\mathbb C} = \mathbb C \cup \{\infty\}, and declaring T(−d/c)=∞T(-d/c) = \infty and T(∞)=a/cT(\infty) = a/c, repairs this: TT becomes a genuine bijection of C^\widehat{\mathbb C}. This is not merely a bookkeeping trick — it reflects the deeper fact that C^\widehat{\mathbb C}, as a compact Riemann surface (the sphere), is the natural domain on which Möbius transformations act as biholomorphic automorphisms, matching the group PGL(2,C)\mathrm{PGL}(2,\mathbb C) exactly.

Is every conformal automorphism of C^\widehat{\mathbb C} necessarily a Möbius transformation?

Yes, and this is a genuinely deep rigidity statement (though its proof uses machinery beyond this article, such as removable singularity theorems for meromorphic functions). Every biholomorphic bijection f:C^→C^f : \widehat{\mathbb C} \to \widehat{\mathbb C} is meromorphic with at most a simple pole structure forced by injectivity, and one shows ff must be rational of degree 1, i.e. exactly of Möbius form. This contrasts sharply with automorphisms of the open disk or plane, where the automorphism groups are different (disk: real-parameter family fixing rotation and one boundary point structure; plane: only affine maps z↦az+bz\mapsto az+b).

Why is the cross-ratio the "right" invariant, rather than just distances or angles?

Möbius transformations are not isometries of the Euclidean metric — they can and do change distances and even angles between non-infinitesimal arcs, though they preserve angles infinitesimally (they are conformal wherever holomorphic with nonzero derivative). What they do preserve exactly is the cross-ratio of four points, a purely projective/algebraic quantity built from ratios of differences. This matches the group-theoretic fact that PGL(2,C)\mathrm{PGL}(2,\mathbb C) acts sharply 3-transitively on C^\widehat{\mathbb C}: fixing three points pins down the whole transformation, so the cross-ratio, which "quotients out" the three-point ambiguity, is the unique remaining invariant of a fourth point.

How does the cross-ratio detect concyclicity so cleanly?

The proof reduces to sending three of the four points to 1,0,∞1, 0, \infty via a Möbius map SS; the image of any generalized circle through those three points must be a generalized circle through 1,0,∞1,0,\infty, and the unique such curve is the extended real line R^\widehat{\mathbb R}. So the fourth point's image lies on the original circle if and only if S(z4)S(z_4) is real, and one shows algebraically that S(z4)S(z_4) equals exactly the cross-ratio (z1,z2,z3,z4)(z_1,z_2,z_3,z_4). The realness of the cross-ratio is thus literally "the fourth point's image lands on the real axis," translated back through the invariance of the cross-ratio itself.

Do Möbius transformations preserve orientation and angles?

Every non-constant Möbius transformation is holomorphic wherever defined (away from its pole) with nonvanishing derivative, so by the theory of Conformal Mappings it preserves angles (both magnitude and orientation) between intersecting curves at every point of C\mathbb C other than the pole. Near the pole and near ∞\infty, one checks conformality using the local coordinate 1/z1/z on the Riemann sphere, and it continues to hold there too, making Möbius transformations conformal automorphisms of the entire sphere C^\widehat{\mathbb C}, not just of C\mathbb C.

What is the connection between Möbius transformations and matrices?

The map sending a matrix M=(abcd)∈GL(2,C)M = \begin{pmatrix} a&b\\c&d\end{pmatrix} \in GL(2,\mathbb C) to the Möbius transformation TM(z)=az+bcz+dT_M(z) = \frac{az+b}{cz+d} is a group homomorphism onto Mo¨b\mathrm{M\ddot ob}, meaning TM1M2=TM1∘TM2T_{M_1M_2} = T_{M_1}\circ T_{M_2} (matrix multiplication corresponds to composition), and its kernel is exactly the nonzero scalar matrices. This realizes Mo¨b\mathrm{M\ddot ob} as the quotient group PGL(2,C)=GL(2,C)/C×I\mathrm{PGL}(2,\mathbb C) = GL(2,\mathbb C)/\mathbb C^\times I, turning every computation with Möbius transformations (composition, inversion, fixed points) into linear algebra with 2×22\times 2 matrices up to scalar multiples.

Why does hyperbolic geometry use only Möbius maps with real coefficients?

The subgroup PSL(2,R)\mathrm{PSL}(2,\mathbb R) of Möbius transformations T(z)=az+bcz+dT(z)=\frac{az+b}{cz+d} with a,b,c,d∈Ra,b,c,d \in \mathbb R and ad−bc=1ad-bc=1 (or any positive determinant, normalized) is exactly the set of Möbius transformations preserving the upper half-plane H\mathbb H as a set, because such TT maps R^\widehat{\mathbb R} to itself (real coefficients preserve the real line) and one checks Im T(z)=(ad−bc) Im z∣cz+d∣2\mathrm{Im}\,T(z) = \frac{(ad-bc)\,\mathrm{Im}\,z}{|cz+d|^2} has the same sign as Im z\mathrm{Im}\,z exactly when ad−bc>0ad-bc>0. This subgroup acts as the full isometry group of the hyperbolic metric ∣dz∣Im z\frac{|dz|}{\mathrm{Im}\,z} on H\mathbb H, making it the natural symmetry group for hyperbolic geometry.

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