- Asked 5/34
- 2068 Chaitra · 5 marks
Hermitian and skew-Hermitian matrices
Short answer
A matrix is Hermitian if A* = A (conjugate transpose) and skew-Hermitian if A* = −A. Every square matrix A can be uniquely expressed as A = P + Q with P = ½(A+A*) Hermitian and Q = ½(A−A*) skew-Hermitian.
Define Hermitian and skew-Hermitian matrices. Show that every square matrix can be uniquely expressed as the sum of a Hermitian and a skew-Hermitian matrix.
Definitions
Let A* = (Ā)ᵀ be the conjugate transpose of a complex square matrix A.
- A is Hermitian if A* = A (aᵢⱼ = conj(aⱼᵢ); the diagonal entries are real). Example: [3 2−i; 2+i 5].
- A is skew-Hermitian if A* = −A (aᵢⱼ = −conj(aⱼᵢ); the diagonal entries are zero or purely imaginary). Example: [2i 1+i; −1+i 0].
Existence
Define P = ½(A + A*) and Q = ½(A − A*). Using (A*)* = A and (kA)* = k̄A* with k = ½ real:
- P* = ½(A* + A) = P, so P is Hermitian.
- Q* = ½(A* − A) = −Q, so Q is skew-Hermitian.
- P + Q = A.
Uniqueness
Suppose A = R + S with R Hermitian and S skew-Hermitian. Taking the conjugate transpose:
A* = R* + S* = R − S
Adding and subtracting with A = R + S:
A + A* = 2R ⇒ R = ½(A + A*) = P
A − A* = 2S ⇒ S = ½(A − A*) = Q
So the decomposition is unique.
Example. A = [1 2+i; 3 i]. Then A* = [1 3; 2−i −i]. P = ½(A + A*) = [1 (5+i)/2; (5−i)/2 0] (Hermitian), and Q = ½(A − A*) = [0 (−1+i)/2; (1+i)/2 i] (skew-Hermitian), with P + Q = A. ∎
✓ Answer checked by Claude Opus 5.5 (high effort)
Related questions
- Hermitian plus skew-Hermitian decomposition · Mathematics III, chapter 1 · asked 5×
- Hermitian and skew-Hermitian matrices · Mathematics III, chapter 1
- Hermitian and skew-Hermitian matrices · Mathematics III, chapter 1
- Symmetric plus skew-symmetric decomposition · Mathematics III, chapter 1 · asked 8×
- Symmetric plus skew-symmetric decomposition · Mathematics III, chapter 1 · asked 8×
- Sum of two matrices in FORTRAN · Computer Programming, chapter 11
- Sum of both diagonals of matrix · Computer Programming, chapter 7
- Stiffness matrix: element matrices, member forces, BMD · Theory of Structures II, chapter 3