HOME

TheInfoList



OR:

In
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 ...
, an antiunitary transformation, is a bijective
antilinear map In mathematics, a function f : V \to W between two complex vector spaces is said to be antilinear or conjugate-linear if \begin f(x + y) &= f(x) + f(y) && \qquad \text \\ f(s x) &= \overline f(x) && \qquad \text \\ \end hold for all vectors x, y ...
:U: H_1 \to H_2\, between two
complex Complex commonly refers to: * Complexity, the behaviour of a system whose components interact in multiple ways so possible interactions are difficult to describe ** Complex system, a system composed of many components which may interact with each ...
Hilbert spaces 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 naturally ...
such that :\langle Ux, Uy \rangle = \overline for all x and y in H_1, where the horizontal bar represents the
complex conjugate In mathematics, the complex conjugate of a complex number is the number with an equal real part and an imaginary part equal in magnitude but opposite in sign. That is, (if a and b are real, then) the complex conjugate of a + bi is equal to a - ...
. If additionally one has H_1 = H_2 then U is called an antiunitary operator. Antiunitary operators are important in quantum theory because they are used to represent certain symmetries, such as time reversal. Their fundamental importance in quantum physics is further demonstrated by
Wigner's theorem Wigner's theorem, proved by Eugene Wigner in 1931, is a cornerstone of the mathematical formulation of quantum mechanics. The theorem specifies how physical symmetries such as rotations, translations, and CPT are represented on the Hilbert sp ...
.


Invariance transformations

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, ...
, the invariance transformations of complex Hilbert space H leave the absolute value of scalar product invariant: : , \langle Tx, Ty \rangle, = , \langle x, y \rangle, for all x and y in H. Due to
Wigner's theorem Wigner's theorem, proved by Eugene Wigner in 1931, is a cornerstone of the mathematical formulation of quantum mechanics. The theorem specifies how physical symmetries such as rotations, translations, and CPT are represented on the Hilbert sp ...
these transformations can either be
unitary Unitary may refer to: Mathematics * Unitary divisor * Unitary element * Unitary group * Unitary matrix * Unitary morphism * Unitary operator * Unitary transformation * Unitary representation * Unitarity (physics) * ''E''-unitary inverse semigrou ...
or antiunitary.


Geometric Interpretation

Congruences In abstract algebra, a congruence relation (or simply congruence) is an equivalence relation on an algebraic structure (such as a group, ring, or vector space) that is compatible with the structure in the sense that algebraic operations done wi ...
of the plane form two distinct classes. The first conserves the orientation and is generated by translations and rotations. The second does not conserve the orientation and is obtained from the first class by applying a reflection. On the complex plane these two classes correspond (up to translation) to unitaries and antiunitaries, respectively.


Properties

* \langle Ux, Uy \rangle = \overline = \langle y, x \rangle holds for all elements x, y of the Hilbert space and an antiunitary U . * When U is antiunitary then U^2 is unitary. This follows from \left\langle U^2 x, U^2 y \right\rangle = \overline = \langle x, y \rangle . * For unitary operator V the operator VK , where K is complex conjugate operator, is antiunitary. The reverse is also true, for antiunitary U the operator UK is unitary. * For antiunitary U the definition of the
adjoint In mathematics, the term ''adjoint'' applies in several situations. Several of these share a similar formalism: if ''A'' is adjoint to ''B'', then there is typically some formula of the type :(''Ax'', ''y'') = (''x'', ''By''). Specifically, adjoin ...
operator U^* is changed to compensate the complex conjugation, becoming \langle U x,y\rangle = \overline. * The adjoint of an antiunitary U is also antiunitary and U U^* = U^* U = 1. (This is not to be confused with the definition of
unitary operators In functional analysis Functional analysis is a branch of mathematical analysis, the core of which is formed by the study of vector spaces endowed with some kind of limit-related structure (e.g. inner product, norm, topology, etc.) and ...
, as the antiunitary operator U is not complex linear.)


Examples

* The complex conjugate operator K, K z = \overline, is an antiunitary operator on the complex plane. * The operator U = i \sigma_y K = \begin 0 & 1 \\ -1 & 0 \end K, where \sigma_y is the second
Pauli matrix In mathematical physics and mathematics, the Pauli matrices are a set of three complex matrices which are Hermitian, involutory and unitary. Usually indicated by the Greek letter sigma (), they are occasionally denoted by tau () when used in ...
and K is the complex conjugate operator, is antiunitary. It satisfies U^2 = -1 .


Decomposition of an antiunitary operator into a direct sum of elementary Wigner antiunitaries

An antiunitary operator on a finite-dimensional space may be decomposed as a direct sum of elementary Wigner antiunitaries W_\theta, 0 \le \theta \le \pi. The operator W_0:\Complex \to \Complex is just simple complex conjugation on \mathbb :W_0(z) = \overline For 0 < \theta \le \pi, the operator W_\theta acts on two-dimensional complex Hilbert space. It is defined by :W_\theta\left(\left(z_1, z_2\right)\right) = \left(e^ \overline,\; e^\overline\right). Note that for 0 < \theta \le \pi :W_\theta\left(W_\theta\left(\left(z_1, z_2\right)\right)\right) = \left(e^z_1, e^z_2\right), so such W_\theta may not be further decomposed into {{nowrap, W_0's, which square to the identity map. Note that the above decomposition of antiunitary operators contrasts with the spectral decomposition of unitary operators. In particular, a unitary operator on a complex Hilbert space may be decomposed into a direct sum of unitaries acting on 1-dimensional complex spaces (eigenspaces), but an antiunitary operator may only be decomposed into a direct sum of elementary operators on 1- and 2-dimensional complex spaces.


References

*Wigner, E. "Normal Form of Antiunitary Operators", Journal of Mathematical Physics Vol 1, no 5, 1960, pp. 409–412 *Wigner, E. "Phenomenological Distinction between Unitary and Antiunitary Symmetry Operators", Journal of Mathematical Physics Vol1, no5, 1960, pp.414–416


See also

*
Unitary operator 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 co ...
*
Wigner's Theorem Wigner's theorem, proved by Eugene Wigner in 1931, is a cornerstone of the mathematical formulation of quantum mechanics. The theorem specifies how physical symmetries such as rotations, translations, and CPT are represented on the Hilbert sp ...
*
Particle physics and representation theory There is a natural connection between particle physics and representation theory, as first noted in the 1930s by Eugene Wigner. It links the properties of elementary particles to the structure of Lie groups and Lie algebras. According to this con ...
Linear algebra Functional analysis