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mathematics Mathematics is an area of knowledge that includes the topics of numbers, formulas and related structures, shapes and the spaces in which they are contained, and quantities and their changes. These topics are represented in modern mathematics ...
, the conjugate transpose, also known as the Hermitian transpose, of an m \times n complex
matrix Matrix most commonly refers to: * ''The Matrix'' (franchise), an American media franchise ** '' The Matrix'', a 1999 science-fiction action film ** "The Matrix", a fictional setting, a virtual reality environment, within ''The Matrix'' (franchi ...
\boldsymbol is an n \times m matrix obtained by transposing \boldsymbol and applying complex conjugate on each entry (the complex conjugate of a+ib being a-ib, for real numbers a and b). It is often denoted as \boldsymbol^\mathrm or \boldsymbol^* or \boldsymbol'. H. W. Turnbull, A. C. Aitken, "An Introduction to the Theory of Canonical Matrices," 1932. For real matrices, the conjugate transpose is just the transpose, \boldsymbol^\mathrm = \boldsymbol^\mathsf.


Definition

The conjugate transpose of an m \times n matrix \boldsymbol is formally defined by where the subscript ij denotes the (i,j)-th entry, for 1 \le i \le n and 1 \le j \le m, and the overbar denotes a scalar complex conjugate. This definition can also be written as :\boldsymbol^\mathrm = \left(\overline\right)^\mathsf = \overline where \boldsymbol^\mathsf denotes the transpose and \overline denotes the matrix with complex conjugated entries. Other names for the conjugate transpose of a matrix are Hermitian conjugate, adjoint matrix or transjugate. The conjugate transpose of a matrix \boldsymbol can be denoted by any of these symbols: * \boldsymbol^*, commonly used in
linear algebra Linear algebra is the branch of mathematics concerning linear equations such as: :a_1x_1+\cdots +a_nx_n=b, linear maps such as: :(x_1, \ldots, x_n) \mapsto a_1x_1+\cdots +a_nx_n, and their representations in vector spaces and through matrice ...
* \boldsymbol^\mathrm, commonly used in linear algebra * \boldsymbol^\dagger (sometimes pronounced as ''A
dagger A dagger is a fighting knife with a very sharp point and usually two sharp edges, typically designed or capable of being used as a thrusting or stabbing weapon.State v. Martin, 633 S.W.2d 80 (Mo. 1982): This is the dictionary or popular-use def ...
''), commonly used in
quantum mechanics Quantum mechanics is a fundamental theory in physics that provides a description of the physical properties of nature at the scale of atoms and subatomic particles. It is the foundation of all quantum physics including quantum chemistry, ...
* \boldsymbol^+, although this symbol is more commonly used for the Moore–Penrose pseudoinverse In some contexts, \boldsymbol^* denotes the matrix with only complex conjugated entries and no transposition.


Example

Suppose we want to calculate the conjugate transpose of the following matrix \boldsymbol. :\boldsymbol = \begin 1 & -2 - i & 5 \\ 1 + i & i & 4-2i \end We first transpose the matrix: :\boldsymbol^\mathsf = \begin 1 & 1 + i \\ -2 - i & i \\ 5 & 4-2i\end Then we conjugate every entry of the matrix: :\boldsymbol^\mathrm = \begin 1 & 1 - i \\ -2 + i & -i \\ 5 & 4+2i\end


Basic remarks

A square matrix \boldsymbol with entries a_ is called * Hermitian or
self-adjoint In mathematics, and more specifically in abstract algebra, an element ''x'' of a *-algebra is self-adjoint if x^*=x. A self-adjoint element is also Hermitian, though the reverse doesn't necessarily hold. A collection ''C'' of elements of a st ...
if \boldsymbol=\boldsymbol^\mathrm; i.e., a_ = \overline. * Skew Hermitian or antihermitian if \boldsymbol=-\boldsymbol^\mathrm; i.e., a_ = -\overline. * Normal if \boldsymbol^\mathrm \boldsymbol = \boldsymbol \boldsymbol^\mathrm. *
Unitary Unitary may refer to: Mathematics * Unitary divisor * Unitary element * Unitary group * Unitary matrix * Unitary morphism * Unitary operator * Unitary transformation * Unitary representation In mathematics, a unitary representation of a grou ...
if \boldsymbol^\mathrm = \boldsymbol^, equivalently \boldsymbol\boldsymbol^\mathrm = \boldsymbol, equivalently \boldsymbol^\mathrm\boldsymbol = \boldsymbol. Even if \boldsymbol is not square, the two matrices \boldsymbol^\mathrm\boldsymbol and \boldsymbol\boldsymbol^\mathrm are both Hermitian and in fact positive semi-definite matrices. The conjugate transpose "adjoint" matrix \boldsymbol^\mathrm should not be confused with the adjugate, \operatorname(\boldsymbol), which is also sometimes called ''adjoint''. The conjugate transpose of a matrix \boldsymbol with real entries reduces to the transpose of \boldsymbol, as the conjugate of a real number is the number itself.


Motivation

The conjugate transpose can be motivated by noting that complex numbers can be usefully represented by 2 \times 2 real matrices, obeying matrix addition and multiplication: :a + ib \equiv \begin a & -b \\ b & a \end. That is, denoting each ''complex'' number z by the ''real'' 2 \times 2 matrix of the linear transformation on the Argand diagram (viewed as the ''real'' vector space \mathbb^2), affected by complex ''z''-multiplication on \mathbb. Thus, an m \times n matrix of complex numbers could be well represented by a 2m \times 2n matrix of real numbers. The conjugate transpose, therefore, arises very naturally as the result of simply transposing such a matrix—when viewed back again as an n \times m matrix made up of complex numbers.


Properties of the conjugate transpose

* (\boldsymbol + \boldsymbol)^\mathrm = \boldsymbol^\mathrm + \boldsymbol^\mathrm for any two matrices \boldsymbol and \boldsymbol of the same dimensions. * (z\boldsymbol)^\mathrm = \overline \boldsymbol^\mathrm for any complex number z and any m \times n matrix \boldsymbol. * (\boldsymbol\boldsymbol)^\mathrm = \boldsymbol^\mathrm \boldsymbol^\mathrm for any m \times n matrix \boldsymbol and any n \times p matrix \boldsymbol. Note that the order of the factors is reversed. * \left(\boldsymbol^\mathrm\right)^\mathrm = \boldsymbol for any m \times n matrix \boldsymbol, i.e. Hermitian transposition is an involution. * If \boldsymbol is a square matrix, then \det\left(\boldsymbol^\mathrm\right) = \overline where \operatorname(A) denotes the
determinant In mathematics, the determinant is a scalar value that is a function of the entries of a square matrix. It characterizes some properties of the matrix and the linear map represented by the matrix. In particular, the determinant is nonzero if a ...
of \boldsymbol . * If \boldsymbol is a square matrix, then \operatorname\left(\boldsymbol^\mathrm\right) = \overline where \operatorname(A) denotes the trace of \boldsymbol. * \boldsymbol is invertible
if and only if In logic and related fields such as mathematics and philosophy, "if and only if" (shortened as "iff") is a biconditional logical connective between statements, where either both statements are true or both are false. The connective is bic ...
\boldsymbol^\mathrm is invertible, and in that case \left(\boldsymbol^\mathrm\right)^ = \left(\boldsymbol^\right)^. * The
eigenvalue In linear algebra, an eigenvector () or characteristic vector of a linear transformation is a nonzero vector that changes at most by a scalar factor when that linear transformation is applied to it. The corresponding eigenvalue, often denote ...
s of \boldsymbol^\mathrm are the complex conjugates of the
eigenvalue In linear algebra, an eigenvector () or characteristic vector of a linear transformation is a nonzero vector that changes at most by a scalar factor when that linear transformation is applied to it. The corresponding eigenvalue, often denote ...
s of \boldsymbol. * \left\langle \boldsymbol x,y \right\rangle_m = \left\langle x, \boldsymbol^\mathrm y\right\rangle_n for any m \times n matrix \boldsymbol, any vector in x \in \mathbb^n and any vector y \in \mathbb^m . Here, \langle\cdot,\cdot\rangle_m denotes the standard complex
inner product In mathematics, an inner product space (or, rarely, a Hausdorff pre-Hilbert space) is a real vector space or a complex vector space with an operation called an inner product. The inner product of two vectors in the space is a scalar, often ...
on \mathbb^m , and similarly for \langle\cdot,\cdot\rangle_n.


Generalizations

The last property given above shows that if one views \boldsymbol as a linear transformation from
Hilbert space In mathematics, Hilbert spaces (named after David Hilbert) allow generalizing the methods of linear algebra and calculus from (finite-dimensional) Euclidean vector spaces to spaces that may be infinite-dimensional. Hilbert spaces arise natural ...
\mathbb^n to \mathbb^m , then the matrix \boldsymbol^\mathrm corresponds to the adjoint operator of \boldsymbol A. The concept of adjoint operators between Hilbert spaces can thus be seen as a generalization of the conjugate transpose of matrices with respect to an orthonormal basis. Another generalization is available: suppose A is a linear map from a complex
vector space In mathematics and physics, a vector space (also called a linear space) is a set whose elements, often called '' vectors'', may be added together and multiplied ("scaled") by numbers called ''scalars''. Scalars are often real numbers, but can ...
V to another, W, then the
complex conjugate linear map In mathematics, the complex conjugate of a complex vector space V\, is a complex vector space \overline V, which has the same elements and additive group structure as V, but whose scalar multiplication involves conjugation of the scalars. In other ...
as well as the transposed linear map are defined, and we may thus take the conjugate transpose of A to be the complex conjugate of the transpose of A. It maps the conjugate dual of W to the conjugate dual of V.


See also

*
Complex dot product In mathematics, the dot product or scalar productThe term ''scalar product'' means literally "product with a scalar as a result". It is also used sometimes for other symmetric bilinear forms, for example in a pseudo-Euclidean space. is an algebr ...
* Hermitian adjoint * Adjugate matrix


References


External links

* {{springer, title=Adjoint matrix, id=p/a010850 Linear algebra Matrices