The conjugate transpose of an matrix
is the
matrix defined by
(1)
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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)
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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)
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Using the identity for the product of transpose gives
(4)
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(5)
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(6)
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(7)
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(8)
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where Einstein summation has been used here to sum over repeated indices, it follows that
(9)
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