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Hermitian matrix : ウィキペディア英語版
Hermitian matrix
In mathematics, a Hermitian matrix (or self-adjoint matrix) is a square matrix with complex entries that is equal to its own conjugate transpose—that is, the element in the -th row and -th column is equal to the complex conjugate of the element in the -th row and -th column, for all indices and :
:a_ = \overline}, in matrix form.
Hermitian matrices can be understood as the complex extension of real symmetric matrices.
If the conjugate transpose of a matrix A is denoted by A^\dagger, then the Hermitian property can be written concisely as
: A = A^\dagger.
Hermitian matrices are named after Charles Hermite, who demonstrated in 1855 that matrices of this form share a property with real symmetric matrices of always having real eigenvalues.
== Examples ==
See the following example:
:
\begin
2 & 2+i & 4 \\
2-i & 3 & i \\
4 & -i & 1 \\
\end

The diagonal elements must be real, as they must be their own complex conjugate.
Well-known families of Pauli matrices, Gell-Mann matrices and their generalizations are Hermitian. In theoretical physics such Hermitian matrices are often multiplied by imaginary coefficients,〔
〕〔
(Physics 125 Course Notes ) at California Institute of Technology
〕 which results in ''skew-Hermitian'' matrices (see below).
Here we offer another useful Hermitian matrix using an abstract example.
If a square matrix A equals the multiplication of a matrix and its conjugate transpose, that is, A=BB^\dagger , then A is a Hermitian positive semi-definite matrix. Furthermore, if B is row full-rank, then A is positive definite.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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