The conjugate transpose of an matrix
is the
matrix
defined by
|
(1)
|
where denotes the transpose
of the matrix
and
denotes the
conjugate matrix. In all common spaces (i.e.,
separable Hilbert spaces), the conjugate and transpose
operations commute, so
|
(2)
|
The symbol (where the "H" stands
for "Hermitian") gives official recognition to the fact that for complex
matrices, it is almost always the case that the combined operation of taking
the transpose and complex conjugate arises in physical or computation contexts and
virtually never the transpose in isolation (Strang
1988, pp. 220-221).
The conjugate transpose of a matrix is implemented
in the Wolfram Language as ConjugateTranspose[A].
The conjugate transpose is also known as the adjoint matrix, adjugate matrix, Hermitian adjoint, or Hermitian transpose (Strang 1988, p. 221). Unfortunately, several
different notations are in use as summarized in the following table. While the notation
is universally used in quantum field
theory,
is commonly used in linear algebra.
Note that because
is sometimes used to denote the complex conjugate, special care must be taken not
to confuse notations from different sources.
| notation | references |
| This work; Golub and van Loan (1996, p. 14), Strang (1988, p. 220) | |
| Courant and Hilbert (1989, p. 9), Lancaster and Tismenetsky (1984), Meyer (2000) | |
| Arfken (1985, p. 210), Weinberg (1995, p. xxv) |
If a matrix is equal to its own conjugate transpose, it is said to be self-adjoint and is called a Hermitian.
The conjugate transpose of a matrix product is given by
|
(3)
|
Using the identity for the product of transpose gives
|
(4)
| |||
|
(5)
| |||
|
(6)
| |||
|
(7)
| |||
|
(8)
|
where Einstein summation has been used here to sum over repeated indices, it follows that
|
(9)
|

