In mathematics, a function between two complex vector spaces is said to be antilinear or conjugate-linear if
hold for all vectors and every complex number where denotes the complex conjugate of
Antilinear maps stand in contrast to Linear operator, which are that are Homogeneous map rather than conjugate homogeneous. If the vector spaces are real then antilinearity is the same as linearity.
Antilinear maps occur in quantum mechanics in the study of T-symmetry and in spinor calculus, where it is customary to replace the bars over the basis vectors and the components of geometric objects by dots put above the indices. Scalar-valued antilinear maps often arise when dealing with Complex number inner products and .
Definitions and characterizations
A function is called or if it is
Additive map and conjugate homogeneous. An on a vector space
is a scalar-valued antilinear map.
A function is called if
while it is called if
In contrast, a linear map is a function that is additive and homogeneous, where is called if
An antilinear map may be equivalently described in terms of the linear map from to the complex conjugate vector space
Examples
Anti-linear dual map
Given a complex vector space
of rank 1, we can construct an anti-linear dual map which is an anti-linear map
sending an element
for
to
for some fixed real numbers
We can extend this to any finite dimensional complex vector space, where if we write out the standard basis
and each standard basis element as
then an anti-linear complex map to
will be of the form
for
Isomorphism of anti-linear dual with real dual
The anti-linear dual
pg 36 of a complex vector space
is a special example because it is isomorphic to the real dual of the underlying real vector space of
This is given by the map sending an anti-linear map
to
In the other direction, there is the inverse map sending a real dual vector
to
giving the desired map.
Properties
The composite of two antilinear maps is a
linear map. The class of
generalizes the class of antilinear maps by generalizing the field.
Anti-dual space
The vector space of all antilinear forms on a vector space
is called the of
If
is a topological vector space, then the vector space of all antilinear functionals on
denoted by
is called the or simply the of
if no confusion can arise.
When is a normed space then the canonical norm on the (continuous) anti-dual space denoted by is defined by using this same equation:
This formula is identical to the formula for the on the continuous dual space of which is defined by
Canonical isometry between the dual and anti-dual
The complex conjugate of a functional is defined by sending to It satisfies
for every and every
This says exactly that the canonical antilinear Bijective map defined by
as well as its inverse are antilinear Isometry and consequently also .
If then and this canonical map reduces down to the identity map.
Inner product spaces
If is an inner product space then both the canonical norm on and on satisfies the parallelogram law, which means that the polarization identity can be used to define a and also on which this article will denote by the notations
where this inner product makes and into Hilbert spaces.
The inner products and are antilinear in their second arguments. Moreover, the canonical norm induced by this inner product (that is, the norm defined by ) is consistent with the dual norm (that is, as defined above by the supremum over the unit ball); explicitly, this means that the following holds for every
= \langle \,g\, | \,f\, \rangle_{X^{\prime}} \qquad \text{ for all } f, g \in X^{\prime}
and
= \langle \,g\, | \,f\, \rangle_{\overline{X}^{\prime}} \qquad \text{ for all } f, g \in \overline{X}^{\prime}.
See also
Citations
-
Budinich, P. and Trautman, A. The Spinorial Chessboard. Springer-Verlag, 1988. . (antilinear maps are discussed in section 3.3).
-
Horn and Johnson, Matrix Analysis, Cambridge University Press, 1985. . (antilinear maps are discussed in section 4.6).