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Special matrices: projection, orthogonal, idempotent and partitioned

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A map of the special matrices

TypeDefining propertyEigenvaluesDeterminant
SymmetricA⊤=AA^\top = Arealproduct of eigenvalues
Skew-symmetricA⊤=−AA^\top = -A0 or purely imaginary0 when the order is odd
OrthogonalQ⊤Q=IQ^\top Q = I∣λ∣=1\lvert\lambda\rvert = 1±1\pm 1
IdempotentP2=PP^2 = P0 or 10 or 1
Orthogonal projectionP2=P=P⊤P^2 = P = P^\top0 or 10 unless P=IP = I
NilpotentNk=0N^k = 0 for some kkall 00
InvolutoryA2=IA^2 = I±1\pm 1±1\pm 1
Triangularzeros below (or above) the diagonalthe diagonal entriesproduct of the diagonal
Diagonalzeros off the diagonalthe diagonal entriesproduct of the diagonal

How the eigenvalue rules are proved. If Av=λvAv = \lambda v with v≠0v \ne 0, then any polynomial identity in AA also holds for λ\lambda. For example:

  • P2=PP^2 = P gives λ2v=λv\lambda^2 v = \lambda v, so λ2=λ\lambda^2 = \lambda and λ∈{0,1}\lambda \in \{0, 1\};
  • Nk=0N^k = 0 gives λk=0\lambda^k = 0;
  • A2=IA^2 = I gives λ2=1\lambda^2 = 1.

Symmetric and skew-symmetric matrices

Every square matrix splits uniquely into a symmetric part and a skew-symmetric part:

A=12(A+A⊤)⏟symmetric+12(A−A⊤)⏟skew.A = \underbrace{\tfrac12(A + A^\top)}_{\text{symmetric}} + \underbrace{\tfrac12(A - A^\top)}_{\text{skew}} .

Example 1. A=(1423)A = \begin{pmatrix} 1 & 4 \\ 2 & 3 \end{pmatrix} has symmetric part (1333)\begin{pmatrix} 1 & 3 \\ 3 & 3 \end{pmatrix} and skew part (01−10)\begin{pmatrix} 0 & 1 \\ -1 & 0 \end{pmatrix}.

Spectral theorem. A real symmetric matrix has real eigenvalues, and it has an orthonormal basis of eigenvectors. So

A=QΛQ⊤=∑iλi qiqi⊤,A = Q \Lambda Q^\top = \sum_i \lambda_i\, q_i q_i^\top ,

with QQ orthogonal and Λ\Lambda diagonal. Eigenvectors belonging to different eigenvalues are automatically orthogonal.

Why. If Av=λvAv = \lambda v and Aw=μwAw = \mu w with λ≠μ\lambda \ne \mu, then λ v⊤w=(Av)⊤w=v⊤Aw=μ v⊤w\lambda\, v^\top w = (Av)^\top w = v^\top A w = \mu\, v^\top w, so v⊤w=0v^\top w = 0.

Skew-symmetric facts.

  • The diagonal is zero, since aii=−aiia_{ii} = -a_{ii}.
  • x⊤Ax=0x^\top A x = 0 for every xx.
  • For odd nn, det⁡A=det⁡A⊤=det⁡(−A)=(−1)ndet⁡A=−det⁡A\det A = \det A^\top = \det(-A) = (-1)^n \det A = -\det A, so det⁡A=0\det A = 0.

Example 2. (0−110)\begin{pmatrix} 0 & -1 \\ 1 & 0 \end{pmatrix} has λ2+1=0\lambda^2 + 1 = 0, so λ=±i\lambda = \pm i, which is purely imaginary. Any 3×33 \times 3 skew-symmetric matrix has determinant 0.

Products.

  • A⊤AA^\top A and AA⊤AA^\top are always symmetric, with eigenvalues ≥0\ge 0.
  • The product of two symmetric matrices is symmetric only if they commute: (AB)⊤=BA(AB)^\top = BA.

Orthogonal matrices

Definition. QQ is orthogonal if Q⊤Q=IQ^\top Q = I, so Q−1=Q⊤Q^{-1} = Q^\top. Its columns are orthonormal, and so are its rows.

Properties.

  • Lengths and angles are kept: ∥Qx∥=∥x∥\lVert Qx\rVert = \lVert x\rVert and (Qx)⋅(Qy)=x⋅y(Qx)\cdot(Qy) = x \cdot y.
  • det⁡Q=±1\det Q = \pm 1. +1+1 means a rotation and −1-1 means a reflection is involved.
  • Every eigenvalue has ∣λ∣=1\lvert\lambda\rvert = 1.
  • Products and inverses of orthogonal matrices are orthogonal.
  • Permutation matrices are orthogonal.

Examples.

  • Rotation by θ\theta: R=(cos⁡θ−sin⁡θsin⁡θcos⁡θ)R = \begin{pmatrix} \cos\theta & -\sin\theta \\ \sin\theta & \cos\theta \end{pmatrix}, with det⁡R=1\det R = 1 and eigenvalues e±iθe^{\pm i\theta}.
  • Reflection across the line y=xy = x: (0110)\begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix}, with determinant −1-1 and eigenvalues 11 (along (1,1)(1, 1)) and −1-1 (along (1,−1)(1, -1)).
  • Householder reflection: H=I−2uu⊤u⊤uH = I - 2\dfrac{uu^\top}{u^\top u}. It reflects across the hyperplane perpendicular to uu, and it is symmetric, orthogonal and involutory.

Example 3. With u=(1,1)u = (1, 1): H=I−(1111)=(0−1−10)H = I - \begin{pmatrix} 1 & 1 \\ 1 & 1\end{pmatrix} = \begin{pmatrix} 0 & -1 \\ -1 & 0 \end{pmatrix}.

  • H(1,1)=(−1,−1)H(1, 1) = (-1, -1): the vector uu is flipped.
  • H(1,−1)=(1,−1)H(1, -1) = (1, -1): vectors perpendicular to uu stay put.

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