# Hermitian adjoint

In mathematics, specifically in functional analysis, each bounded linear operator on a Hilbert space has a corresponding **adjoint operator**. Adjoints of operators generalize conjugate transposes of square matrices to (possibly) infinite-dimensional situations. If one thinks of operators on a Hilbert space as "generalized complex numbers", then the adjoint of an operator plays the role of the complex conjugate of a complex number.

The adjoint of an operator Template:Mvar may also be called the **Hermitian adjoint**, **Hermitian conjugate** or **Hermitian transpose**^{[1]} (after Charles Hermite) of Template:Mvar and is denoted by *A** or *A*^{†} (the latter especially when used in conjunction with the bra–ket notation).

## Contents

## Definition for bounded operators

Suppose Template:Mvar is a Hilbert space, with inner product . Consider a continuous linear operator *A* : *H* → *H* (for linear operators, continuity is equivalent to being a bounded operator). Then the adjoint of Template:Mvar is the continuous linear operator *A** : *H* → *H* satisfying

Existence and uniqueness of this operator follows from the Riesz representation theorem.^{[2]}

This can be seen as a generalization of the *adjoint* matrix of a square matrix which has a similar property involving the standard complex inner product.

## Properties

The following properties of the Hermitian adjoint of bounded operators are immediate:^{[2]}

*A*** =*A*– involutiveness- If Template:Mvar is invertible, then so is
*A**, with (*A**)^{−1}= (*A*^{−1})* - (
*A*+*B*)* =*A** +*B** - (λ
*A*)* = Template:Overline*A**, where Template:Overline denotes the complex conjugate of the complex number λ – antilinearity (together with 3.) - (
*AB*)* =*B***A**

If we define the operator norm of Template:Mvar by

then

Moreover,

One says that a norm that satisfies this condition behaves like a "largest value", extrapolating from the case of self-adjoint operators.

The set of bounded linear operators on a Hilbert space Template:Mvar together with the adjoint operation and the operator norm form the prototype of a C*-algebra.

## Adjoint of densely defined operators

A densely defined operator Template:Mvar on a Hilbert space Template:Mvar is a linear operator whose domain D(A) is a dense linear subspace of Template:Mvar and whose co-domain is Template:Mvar.^{[3]} Its adjoint *A** has as domain *D*(*A**) the set of all *y* ∈ *H* for which there is a *z* ∈ *H* satisfying

and *A**(*y*) equals the Template:Mvar defined thus.^{[4]}

Properties 1.–5. hold with appropriate clauses about domains and codomains. For instance, the last property now states that (*AB*)* is an extension of *B***A** if Template:Mvar, Template:Mvar and Template:Mvar are densely defined operators.^{[5]}

The relationship between the image of Template:Mvar and the kernel of its adjoint is given by:

- (see orthogonal complement)

Proof of the first equation:^{[6]}

The second equation follows from the first by taking the orthogonal complement on both sides. Note that in general, the image need not be closed, but the kernel of a continuous operator^{[7]} always is.

## Hermitian operators

A bounded operator *A* : *H* → *H* is called Hermitian or self-adjoint if

which is equivalent to

In some sense, these operators play the role of the real numbers (being equal to their own "complex conjugate") and form a real vector space. They serve as the model of real-valued observables in quantum mechanics. See the article on self-adjoint operators for a full treatment.

## Adjoints of antilinear operators

For an antilinear operator the definition of adjoint needs to be adjusted in order to compensate for the complex conjugation. An adjoint operator of the antilinear operator Template:Mvar on a Hilbert space Template:Mvar is an antilinear operator *A** : *H* → *H* with the property:

## Other adjoints

The equation

is formally similar to the defining properties of pairs of adjoint functors in category theory, and this is where adjoint functors got their name from.

## See also

- Mathematical concepts
- Physical applications

## Footnotes

- ↑ {{#invoke:citation/CS1|citation |CitationClass=book }}
- ↑
^{2.0}^{2.1}^{2.2}^{2.3}Template:Harvnb; Template:Harvnb - ↑ See unbounded operator for details.
- ↑ Template:Harvnb; Template:Harvnb
- ↑ Template:Harvnb
- ↑ See Template:Harvnb for the case of bounded operators
- ↑ The same as a bounded operator.
- ↑ Template:Harvnb; Template:Harvnb

## References

- {{#invoke:citation/CS1|citation

|CitationClass=citation }}.

- {{#invoke:citation/CS1|citation

|CitationClass=citation }}.