# Hermitian matrix

In mathematics, a **Hermitian matrix** (or **self-adjoint matrix**) is a complex square matrix that is equal to its own conjugate transpose—that is, the element in the i-th row and j-th column is equal to the complex conjugate of the element in the j-th row and i-th column, for all indices i and j:

Hermitian matrices can be understood as the complex extension of real symmetric matrices.

Hermitian matrices can be characterized in a number of equivalent ways, some of which are listed below:

This is also the way that the more general concept of self-adjoint operator is defined.

Hermitian matrices are fundamental to the quantum theory of matrix mechanics created by Werner Heisenberg, Max Born, and Pascual Jordan in 1925.

The diagonal elements must be real, as they must be their own complex conjugate.

Well-known families of Hermitian matrices include the Pauli matrices, the Gell-Mann matrices and their generalizations. In theoretical physics such Hermitian matrices are often multiplied by imaginary coefficients,^{[1]}^{[2]} which results in skew-Hermitian matrices.

The entries on the main diagonal (top left to bottom right) of any Hermitian matrix are real.

Only the main diagonal entries are necessarily real; Hermitian matrices can have arbitrary complex-valued entries in their off-diagonal elements, as long as diagonally-opposite entries are complex conjugates.

A matrix that has only real entries is symmetric if and only if it is Hermitian matrix. A real and symmetric matrix is simply a special case of a Hermitian matrix.

The finite-dimensional spectral theorem says that any Hermitian matrix can be diagonalized by a unitary matrix, and that the resulting diagonal matrix has only real entries. This implies that all eigenvalues of a Hermitian matrix A with dimension n are real, and that A has n linearly independent eigenvectors. Moreover, a Hermitian matrix has orthogonal eigenvectors for distinct eigenvalues. Even if there are degenerate eigenvalues, it is always possible to find an orthogonal basis of **C**^{n} consisting of n eigenvectors of A.

The product of two Hermitian matrices A and B is Hermitian if and only if *AB* = *BA*.

The Hermitian complex n-by-n matrices do not form a vector space over the complex numbers, **C**, since the identity matrix *I*_{n} is Hermitian, but *i* *I*_{n} is not. However the complex Hermitian matrices *do* form a vector space over the real numbers **R**. In the 2*n*^{2}-dimensional vector space of complex *n* × *n* matrices over **R**, the complex Hermitian matrices form a subspace of dimension *n*^{2}. If *E*_{jk} denotes the n-by-n matrix with a 1 in the *j*,*k* position and zeros elsewhere, a basis (orthonormal with respect to the Frobenius inner product) can be described as follows:

An example is that the four Pauli matrices form a complete basis for the vector space of all complex 2-by-2 Hermitian matrices over **R**.

(Alternatively, the determinant is the product of the matrix's eigenvalues, and as mentioned before, the eigenvalues of a Hermitian matrix are real.)

The Rayleigh quotient is used in the min-max theorem to get exact values of all eigenvalues. It is also used in eigenvalue algorithms to obtain an eigenvalue approximation from an eigenvector approximation. Specifically, this is the basis for Rayleigh quotient iteration.