duality
A bijective mapping
between projective spaces of the same finite dimension such that
implies .
The image of a sum of subspaces under a correlation is the intersection of their images and, conversely, the image of an intersection is the sum of the images. In particular, the image of a point is a hyperplane and vice versa. A necessary and sufficient condition for the existence of a correlation of a projective space
over a division ring
onto a space
over a division ring
is that there exists an anti-isomorphism ,
i.e. a bijective mapping for which ,
;
in that case
is dual to .
Examples of spaces with an auto-correlation, i.e. a correlation onto itself, are the real projective spaces ,
the complex projective spaces
and the quaternion projective spaces .
A polarity is an auto-correlation
satisfying .
A projective space
over a division ring
admits a polarity if and only if
admits an involutory anti-automorphism, i.e. an anti-automorphism
with .
A subspace
is called a null subspace relative to an auto-correlation
if
for any point ,
and strictly isotropic if .
Any strictly isotropic subspace is a null subspace. A polarity relative to which the whole space is a null space is called a null (or symplectic) polarity (see also Polarity).
Let the projective space
over a division ring
be interpreted as the set of linear subspaces of the (left) linear space
over .
A semi-bilinear form on
is a mapping
together with an anti-automorphism
of
such that
In particular, if
is a field and ,
then
is a bilinear form. A semi-bilinear form
is called non-degenerate provided
for all (
all )
implies (
,
respectively). Any auto-correlation
of
can be represented with the aid of a non-degenerate semi-bilinear form
in the following way: for a subspace
of
its image is the orthogonal complement of
with respect to :
(the Birkhoff–von Neumann theorem, ).
is a polarity if and only if
is reflexive, i.e. if
implies .
By multiplying
by a suitable element of
one can bring any reflexive non-degenerate semi-bilinear form
and the corresponding automorphism
in either of the following two forms:
1)
is an involution, i.e. ,
and
In this case one calls
symmetric if (
and hence necessarily
is a field) and Hermitian if .
2) (
and hence
is a field) and
Such an
is called anti-symmetric.
A special example of a correlation is the following. Let
be a projective space over a division ring .
Define the opposite division ring
as the set of elements of
with the same addition but with multiplication
is an anti-isomorphism from
onto
which defines the canonical correlation from
onto .
The (left) projective space ,
which can be identified with the right projective space ,
i.e. with the set of linear subspaces of the -
dimensional right vector space ,
is the (canonical) dual space of (
cf. Projective algebra, the construction of ).
References[edit]
[a1] | R. Baer, "Linear algebra and projective geometry" , Acad. Press (1952) |
[a2] | G. Birkhoff, J. von Neumann, "The logic of quantum mechanics" Ann. of Math. , 37 (1936) pp. 823–843 |
[a3] | J.A. Dieudonné, "La géométrie des groups classiques" , Springer (1963) |
[a4] | D.R. Hughes, F.C. Piper, "Projective planes" , Springer (1972) |