Unitary operators

In functional analysis, a unitary operator is a surjective bounded operator on a Hilbert space that preserves the inner product. Unitary operators are usually taken as operating ''on'' a Hilbert space, but the same notion serves to define the concept of isomorphism ''between'' Hilbert spaces.

A unitary element is a generalization of a unitary operator. In a unital algebra, an element of the algebra is called a unitary element if ,
where is the identity element.

Definition

Definition 1. A ''unitary operator'' is a bounded linear operator on a Hilbert space that satisfies , where is the adjoint of , and is the identity operator.

The weaker condition defines an ''isometry''. The other condition, , defines a ''coisometry''. Thus a unitary operator is a bounded linear operator which is both an isometry and a coisometry, or, equivalently, a surjective isometry.

An equivalent definition is the following:

Definition 2. A ''unitary operator'' is a bounded linear operator on a Hilbert space for which the following hold:
* is surjective, and
* preserves the inner product of the Hilbert space, . In other words, for all vectors and in we have:
*:$\langle Ux, Uy \rangle_H = \langle x, y \rangle_H.$

The notion of isomorphism in the category of Hilbert spaces is captured if domain and range are allowed to differ in this definition. Isometries preserve Cauchy sequences, hence the completeness property of Hilbert spaces is preserved

The following, seemingly weaker, definition is also equivalent:

Definition 3. A ''unitary operator'' is a bounded linear operator on a Hilbert space for which the following hold:
*the range of is dense in , and
* preserves the inner product of the Hilbert space, . In other words, for all vectors and in we have:
*:$\langle Ux, Uy \rangle_H = \langle x, y \rangle_H.$

To see that Definitions 1 & 3 are equivalent, notice that preserving the inner product implies is an isometry (thus, a bounded linear operator). The fact that has dense range ensures it has a bounded inverse . It is clear that .

Thus, unitary operators are just automorphisms of Hilbert spaces, i.e., they preserve the structure (the linear space structure, the inner product, and hence the topology) of the space on which they act. The group of all unitary operators from a given Hilbert space to itself is sometimes referred to as the ''Hilbert group'' of , denoted or .

Examples

* The identity function is trivially a unitary operator.
* Rotations in are the simplest nontrivial example of unitary operators. Rotations do not change the length of a vector or the angle between two vectors. This example can be expanded to .
* On the vector space of complex numbers, multiplication by a number of absolute value , that is, a number of the form for , is a unitary operator. is referred to as a phase, and this multiplication is referred to as multiplication by a phase. Notice that the value of modulo does not affect the result of the multiplication, and so the independent unitary operators on are parametrized by a circle. The corresponding group, which, as a set, is the circle, is called .
* More generally, unitary matrices are precisely the unitary operators on finite-dimensional Hilbert spaces, so the notion of a unitary operator is a generalization of the notion of a unitary matrix. Orthogonal matrices are the special case of unitary matrices in which all entries are real. They are the unitary operators on .
* The bilateral shift on the sequence space indexed by the integers is unitary. In general, any operator in a Hilbert space which acts by permuting an orthonormal basis is unitary. In the finite dimensional case, such operators are the permutation matrices.
* The unilateral shift (right shift) is an isometry; its conjugate (left shift) is a coisometry.
* The Fourier operator is a unitary operator, i.e. the operator which performs the Fourier transform (with proper normalization). This follows from Parseval's theorem.
* Unitary operators are used in unitary representations.
* Quantum logic gates are unitary operators. Not all gates are Hermitian.

Linearity

The linearity requirement in the definition of a unitary operator can be dropped without changing the meaning because it can be derived from linearity and positive-definiteness of the scalar product:

:$\begin \, \lambda U(x) -U(\lambda x) \, ^2 &= \langle \lambda U(x) -U(\lambda x), \lambda U(x)-U(\lambda x) \rangle \\ &= \, \lambda U(x) \, ^2 + \, U(\lambda x) \, ^2 - \langle U(\lambda x), \lambda U(x) \rangle - \langle \lambda U(x), U(\lambda x) \rangle \\ &= , \lambda, ^2 \, U(x)\, ^2 + \, U(\lambda x) \, ^2 - \overline \langle U(\lambda x), U(x) \rangle - \lambda \langle U(x), U(\lambda x) \rangle \\ &= , \lambda, ^2 \, x \, ^2 + \, \lambda x \, ^2 - \overline \langle \lambda x, x \rangle - \lambda \langle x, \lambda x \rangle \\ &= 0 \end$

Analogously you obtain

:$\, U(x+y)-(Ux+Uy)\, = 0.$

Properties

* The spectrum of a unitary operator lies on the unit circle. That is, for any complex number in the spectrum, one has . This can be seen as a consequence of the spectral theorem for normal operators. By the theorem, is unitarily equivalent to multiplication by a Borel-measurable on , for some finite measure space . Now implies , -a.e. This shows that the essential range of , therefore the spectrum of , lies on the unit circle.
* A linear map is unitary if it is surjective and isometric. (Use Polarization identity to show the only if part.)

See also

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Footnotes

References

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{{Hilbert space

Operator theory
Unitary operators