In functional analysis, a unitary operator is a surjective bounded operator on a Hilbert space that preserves the inner product.
Non-trivial examples include rotations, reflections, and the Fourier operator.
Unitary operators generalize unitary matrix.
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.
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 weaker condition, , defines a coisometry. Thus a unitary operator is a bounded linear operator that 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:
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is surjective, and
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preserves the inner product of the Hilbert space, . In other words, for all vector space and in we have:
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:
The notion of isomorphism in the Category theory of Hilbert spaces is captured if domain and range are allowed to differ in this definition. Isometries preserve ; 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:
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the range of is dense set in , and
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preserves the inner product of the Hilbert space, . In other words, for all vectors and in we have:
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:
To see that definitions 1 and 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 of Hilbert spaces, i.e., they preserve the structure (the vector 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
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The identity function is trivially a unitary operator.
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Rotation 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 . In even higher dimensions, this can be extended to the Givens rotation.
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Reflections, like the Householder transformation.
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times a Hadamard matrix.
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In general, any operator in a Hilbert space that acts by permuting an orthonormal basis is unitary. In the finite dimensional case, such operators are the permutation matrices.
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On the vector space of , 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 .
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The Fourier operator is a unitary operator, i.e. the operator that performs the Fourier transform (with proper normalization). This follows from Parseval's theorem.
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Quantum logic gates are unitary operators. Not all gates are Hermitian.
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More generally, unitary matrix are precisely the unitary operators on finite-dimensional , 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 .
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The bilateral shift on the Lp space indexed by the is unitary.
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The unilateral shift (right shift) is an isometry; its conjugate (left shift) is a coisometry.
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Unitary operators are used in unitary representations.
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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 multiplicative identity element.
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Any composition of the above.
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:
\| \lambda U(x) -U(\lambda x) \|^2 &= \langle \lambda U(x) -U(\lambda x), \lambda U(x)-U(\lambda x) \rangle \\5pt
&= \| \lambda U(x) \|^2 + \| U(\lambda x) \|^2 - \langle U(\lambda x), \lambda U(x) \rangle - \langle \lambda U(x), U(\lambda x) \rangle \\5pt
&= |\lambda|^2 \| U(x)\|^2 + \| U(\lambda x) \|^2 - \overline{\lambda} \langle U(\lambda x), U(x) \rangle - \lambda \langle U(x), U(\lambda x) \rangle \\5pt
&= |\lambda|^2 \| x \|^2 + \| \lambda x \|^2 - \overline{\lambda} \langle \lambda x, x \rangle - \lambda \langle x, \lambda x \rangle \\5pt
&= 0
\end{align}
Analogously we obtain
Properties
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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 . 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.
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A linear map is unitary if it is surjective and isometric. (Use Polarization identity to show the only if part.)
See also
Footnotes