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Exercise 2053Topology › Topology of Mn(ℝ) › Continuity of matrix mapsM1Added 7 Nov 2026

The Cayley transform of a skew-symmetric matrix

#Cayley transform#skew-symmetric#special orthogonal group#chart

Statement

Show that C(K)=(I−K)(I+K)−1C(K)=(I-K)(I+K)^{-1} is a homeomorphism from the space Skewn\mathrm{Skew}_n of skew-symmetric matrices onto {U∈SO(n):−1∉spec⁡U}\{U\in SO(n):-1\notin\operatorname{spec}U\}.

Hint

For skew KK, compute vT(I+K)vv^T(I+K)v to show that I+KI+K is invertible.

The inverse is given by the same formula: K=(I−U)(I+U)−1K=(I-U)(I+U)^{-1}.

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Solution

Idea. The matrices I+KI+K and I−KI-K commute and are transposes of each other, which gives orthogonality; the formula is an involution.

Step 1: I+KI+K is invertible. If (I+K)v=0(I+K)v=0 then 0=vT(I+K)v=∣v∣2+vTKv=∣v∣20=v^T(I+K)v=|v|^2+v^TKv=|v|^2, since vTKv=0v^TKv=0 for skew KK (vTKv=(vTKv)T=−vTKvv^TKv=(v^TKv)^T=-v^TKv). So v=0v=0.

Step 2: C(K)C(K) is orthogonal. Using KT=−KK^T=-K: (I+K)T=I−K(I+K)^T=I-K, so
C(K)T=((I+K)−1)T(I−K)T=(I−K)−1(I+K).C(K)^T=\big((I+K)^{-1}\big)^T(I-K)^T=(I-K)^{-1}(I+K).
Since I+KI+K and I−KI-K commute,
CTC=(I−K)−1(I+K)(I−K)(I+K)−1=(I−K)−1(I−K)(I+K)(I+K)−1=I.C^TC=(I-K)^{-1}(I+K)(I-K)(I+K)^{-1}=(I-K)^{-1}(I-K)(I+K)(I+K)^{-1}=I.
Moreover det⁡C=det⁡(I−K)det⁡(I+K)=1\det C=\frac{\det(I-K)}{\det(I+K)}=1, because det⁡(I−K)=det⁡((I+K)T)=det⁡(I+K)\det(I-K)=\det((I+K)^T)=\det(I+K). So C(K)∈SO(n)C(K)\in SO(n).

Step 3: −1-1 is not an eigenvalue. If C(K)v=−vC(K)v=-v, let w=(I+K)−1vw=(I+K)^{-1}v. Then (I−K)w=−(I+K)w(I-K)w=-(I+K)w, so w−Kw=−w−Kww-Kw=-w-Kw, hence 2w=02w=0, v=0v=0.

Step 4: the inverse map. For U∈SO(n)U\in SO(n) with I+UI+U invertible, define K=(I−U)(I+U)−1K=(I-U)(I+U)^{-1}.
- *Skew:* with UT=U−1U^T=U^{-1}, KT=(I+UT)−1(I−UT)=(U−1(U+I))−1U−1(U−I)=(I+U)−1(U−I)=−KK^T=(I+U^T)^{-1}(I-U^T)=\big(U^{-1}(U+I)\big)^{-1}U^{-1}(U-I)=(I+U)^{-1}(U-I)=-K (as I±UI\pm U commute).
- *C(K)=UC(K)=U:* I+K=2(I+U)−1I+K=2(I+U)^{-1} and I−K=2U(I+U)−1I-K=2U(I+U)^{-1}, so C(K)=2U(I+U)−1⋅12(I+U)=UC(K)=2U(I+U)^{-1}\cdot\frac12(I+U)=U.
- Similarly the inverse formula applied to C(K)C(K) returns KK (the roles of the two maps are symmetric: the Cayley formula is an involution).

Step 5: continuity. Both maps are composites of inversion (continuous, Problem 68), sums and products, hence continuous.

Example. n=2n=2, K=t(0−110)K=t\begin{pmatrix}0&-1\\1&0\end{pmatrix}: C(K)C(K) is the rotation by angle −2arctan⁡t-2\arctan t. Numerically t=0.7t=0.7 gives arctan⁡2(C10,C00)=−1.22145=−2arctan⁡0.7\arctan2(C_{10},C_{00})=-1.22145=-2\arctan0.7. The only rotation not reached is the one with −1-1 in its spectrum, namely Rπ=−IR_\pi=-I (t→∞t\to\infty).

Remark.
- For even nn, orthogonal matrices with det⁡=−1\det=-1 always have −1-1 as an eigenvalue, and for odd nn too; so the condition "∈SO(n)\in SO(n)" is automatic.
- This shows SO(n)SO(n) minus a closed nowhere dense set is homeomorphic to Rn(n−1)/2\mathbb{R}^{n(n-1)/2}: a rational (algebraic) chart, an alternative to the exponential map.