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Recitation 10A

Denote a 2×22\times 2 orthogonal matrix by [acbd]\begin{bmatrix}a & c\\ b & d\end{bmatrix}.

Since it is an orthogonal matrix, the entries satisfy a2+b2=1,ac+bd=0,c2+d2=1.a^2+b^2=1, ac+bd=0, c^2+d^2=1.

Since a2+b2=1a^2+b^2=1, it is standard to parametrize aa and bb by a=cosθa=\cos\theta and b=sinθb=\sin\theta. Using the last two equations, we can get c=sinθ,d=±cosθc=\mp \sin\theta, d=\pm\cos\theta. In other words, we have two types of orthogonal matrix A=[cosθsinθsinθcosθ],B=[cosθsinθsinθcosθ].A = \begin{bmatrix}\cos\theta & -\sin\theta \\ \sin\theta & \cos\theta\end{bmatrix}, B = \begin{bmatrix}\cos\theta & \sin\theta \\ \sin\theta & -\cos\theta\end{bmatrix}.

Problem: What are the eigenvalues and correspondent eigenvectors of the matrix BB? How are those two eigenvectors related to each other? What does the linear transformation SS that sends xx to BxBx do? What about the linear transformation TT that sends xx to B2xB^2x?

Solution: To get the eigenvalues of the matrix BB, consider the characteristic equation det(BλI)=cosθλsinθsinθcosθλ=(cosθλ)(cosθλ)sin2θ=λ21=0det\left(B-\lambda I\right)=\begin{vmatrix}\cos\theta-\lambda & \sin\theta \\ \sin\theta & -\cos\theta-\lambda\end{vmatrix}=(\cos\theta-\lambda)(-\cos\theta-\lambda)-\sin^2\theta=\lambda^2-1=0. This gives us two eigenvalues λ1=1,λ2=1\lambda_1 = 1, \lambda_2=-1.

For λ1=1\lambda_1=1, the eigenvector can be u=(sinθ,1cosθ)\mathbf{u}=(\sin\theta, 1-\cos\theta). For λ2=1\lambda_2=-1, the eigenvector can be v=(sinθ,1+cosθ)\mathbf{v}=(-\sin\theta, 1+\cos\theta). These two vectors u,v\mathbf{u}, \mathbf{v} are perpendicular to each other because their inner product is $$. Now we have two perpendicular directions u\mathbf{u} and v\mathbf{v}. On one hand, because the vector u\mathbf{u} is correspondent to the eigenvalue 11, SS preserves all the vectors who have the same direction as u\mathbf{u}. On the other hand, because the vector v\mathbf{v} is correspondent to the eigenvalue 1-1, SS reverses the direction of all the vectors who have the same direction as v\mathbf{v}. Therefore SS is a reflection across the line through the origin with direction u\mathbf{u}. Since the composition of two same reflections does nothing, the linear transformation TT that sends xx to B2xB^2x is an identity map. Also it is easy to check B2B^2 is indeed an identity matrix.