Antilinear map explained

f:V\toW

between two complex vector spaces is said to be antilinear or conjugate-linear if \beginf(x + y) &= f(x) + f(y) && \qquad \text \\f(s x) &= \overline f(x) && \qquad \text \\\endhold for all vectors

x,y\inV

and every complex number

s,

where

\overline{s}

denotes the complex conjugate of

s.

Antilinear maps stand in contrast to linear maps, which are additive maps that are homogeneous 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 time reversal 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 inner products and Hilbert spaces.

Definitions and characterizations

A function is called or if it is additive and conjugate homogeneous. An on a vector space

V

is a scalar-valued antilinear map.

A function

f

is called iff(x + y) = f(x) + f(y) \quad \text x, ywhile it is called if f(ax) = \overline f(x) \quad \text x \text a. In contrast, a linear map is a function that is additive and homogeneous, where

f

is called iff(ax) = a f(x) \quad \text x \text a.

An antilinear map

f:V\toW

may be equivalently described in terms of the linear map

\overline{f}:V\to\overline{W}

from

V

to the complex conjugate vector space

\overline{W}.

Examples

Anti-linear dual map

Given a complex vector space

V

of rank 1, we can construct an anti-linear dual map which is an anti-linear map l:V \to \Complex sending an element

x1+iy1

for

x1,y1\in\R

to x_1 + iy_1 \mapsto a_1 x_1 - i b_1 y_1 for some fixed real numbers

a1,b1.

We can extend this to any finite dimensional complex vector space, where if we write out the standard basis

e1,\ldots,en

and each standard basis element as e_k = x_k + iy_k then an anti-linear complex map to

\Complex

will be of the form \sum_k x_k + iy_k \mapsto \sum_k a_k x_k - i b_k y_k for

ak,bk\in\R.

Isomorphism of anti-linear dual with real dual

The anti-linear dual[1] pg 36 of a complex vector space

V

\operatorname_(V,\Complex) is a special example because it is isomorphic to the real dual of the underlying real vector space of

V,

Hom\R(V,\R).

This is given by the map sending an anti-linear map \ell: V \to \Complexto \operatorname(\ell) : V \to \R In the other direction, there is the inverse map sending a real dual vector \lambda : V \to \R to \ell(v) = -\lambda(iv) + i\lambda(v) giving the desired map.

Properties

The composite of two antilinear maps is a linear map. The class of semilinear maps generalizes the class of antilinear maps.

Anti-dual space

The vector space of all antilinear forms on a vector space

X

is called the of

X.

If

X

is a topological vector space, then the vector space of all antilinear functionals on

X,

denoted by \overline^, is called the or simply the of

X

if no confusion can arise.

When

H

is a normed space then the canonical norm on the (continuous) anti-dual space \overline^, denoted by \|f\|_, is defined by using this same equation: \|f\|_ ~:=~ \sup_ |f(x)| \quad \text f \in \overline^.

X\prime

of

X,

which is defined by\|f\|_ ~:=~ \sup_ |f(x)| \quad \text f \in X^.

Canonical isometry between the dual and anti-dual

\overline{f}

of a functional

f

is defined by sending

x\in\operatorname{domain}f

to \overline. It satisfies \|f\|_ ~=~ \left\|\overline\right\|_ \quad \text \quad \left\|\overline\right\|_ ~=~ \|g\|_for every

f\inX\prime

and every g \in \overline^. This says exactly that the canonical antilinear bijection defined by\operatorname ~:~ X^ \to \overline^ \quad \text \quad \operatorname(f) := \overline as well as its inverse

\operatorname{Cong}-1~:~\overline{X}\prime\toX\prime

are antilinear isometries and consequently also homeomorphisms.

If

F=\R

then

X\prime=\overline{X}\prime

and this canonical map

\operatorname{Cong}:X\prime\to\overline{X}\prime

reduces down to the identity map.

Inner product spaces

If

X

is an inner product space then both the canonical norm on

X\prime

and on

\overline{X}\prime

satisfies the parallelogram law, which means that the polarization identity can be used to define a and also on

\overline{X}\prime,

which this article will denote by the notations \langle f, g \rangle_ := \langle g \mid f \rangle_ \quad \text \quad \langle f, g \rangle_ := \langle g \mid f \rangle_ where this inner product makes

X\prime

and

\overline{X}\prime

into Hilbert spaces. The inner products \langle f, g \rangle_ and \langle f, g \rangle_ are antilinear in their second arguments. Moreover, the canonical norm induced by this inner product (that is, the norm defined by f \mapsto \sqrt) 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

f\inX\prime:

\sup_ |f(x)| = \|f\|_ ~=~ \sqrt ~=~ \sqrt.

If

X

is an inner product space then the inner products on the dual space

X\prime

and the anti-dual space \overline^, denoted respectively by \langle \,\cdot\,, \,\cdot\, \rangle_ and \langle \,\cdot\,, \,\cdot\, \rangle_, are related by\langle \,\overline\, | \,\overline\, \rangle_ = \overline = \langle \,g\, | \,f\, \rangle_ \qquad \text f, g \in X^and\langle \,\overline\, | \,\overline\, \rangle_ = \overline = \langle \,g\, | \,f\, \rangle_ \qquad \text f, g \in \overline^.

References

Notes and References

  1. Book: Birkenhake, Christina. Complex Abelian Varieties . 2004 . Springer Berlin Heidelberg. Herbert Lange . 978-3-662-06307-1. Second, augmented. Berlin, Heidelberg. 851380558.