A Brief Introduction to Quantum Geometry
Table of Contents
Introduction
From Geometry to Algebra: 1
Part 2
Non-commutative Generalizations
Examples
Spaces With Indistinguishable Points
Quantum Groups and Quantum Bundles
Quantum Tori and Matrix Spaces
Supermanifolds
Quantization of Symplectic Manifolds
C*-Algebraic Extensions and BDF-Theory
Literature
Reformulating Basic Geometrical Concepts [2/2]
Vector Bundles
Let us now assume that X is a compact smooth manifold, and let
be a smooth complex vector bundle over X.
Let
be the space of smooth sections of
.
This space is a finite and projective module over the *-algebra
of smooth functions on X.
Conversely, if
is an arbitrary finite and projective module over
then there exists a unique (up to the isomorphisms) smooth vector bundle
over X such that
.
Vector Fields
Let
be a smooth vector field on X and let
be the corresponding
Lie derivative (the derivation along
).
The map D satisfies the Leibniz rule
in other words it is a derivation on
.
Moreover, D is hermitian in the sense that D*=*D, as long as
is a real vector field.
Conversely, if
is an arbitrary hermitian derivation on
then there exists a unique (real) vector field
on X such that
. In other
words, there exists a natural bijection between vector fields on X and
hermitian derivations on
.
If we relax the hermicity assumption, then we obtain a correspondence between all
derivations on
and complex vector fields on X.
Differential Forms
The algebra
of smooth differential forms over a compact smooth
manifold X can be constructed as follows.
Let us first consider the Lie algebra
of all derivations over
(vector fields, in accordance with the previous paragraph). This algebra
is naturally acting
in
, so we
can construct the Chevalley complex
. This
space possesses a natural graded-differential *-algebra structure. By definition, the elements of
are all possible n-linear antisymmetric maps
The differential in
is given by
where, by definition, the symbols within the hats are omitted from the expression.
The *-algebra structure is defined by
Here
and
is a subset cosisting of all (k+l)-permutations
preserving the orders of the first k, and the last l elements.
By definition, we put
.
The algebra of differential forms
can be viewed as a differential subalgebra of
generated by
. In other words,
the spaces
are additively spanned by the elements of the form
where
.
We can summarize our discussion so far in the following table, which is a kind of
a mini dictionary between geometry and algebra:
|
Elementary Geometry-Algebra Dictionary |
| Compact topological spaces X |
Unital commutative C*-algebras A |
| X=compact topological space |
A=C(X)={complex continuous
functions on X} |
Points
|
Characters
|
Continuous maps between compacts X and
| Unital *-homomorphisms from B to A |
| The direct product X×Y |
The C*-tensor product
|
| Symmetries of X |
Automorphisms of A |
| Group structure on X |
Coproduct map
|
| Probabilty measures on a metrizable compact X |
Positive normalized linear functionals on A |
| Locally-compact noncompact topological spaces X |
Non-unital commutative C*-algebras A |
| Pure measure theory |
Commutative von Neumann algebras |
| X=compact smooth manifold |
={complex smooth functions on
X} |
| Vector bundles over X |
Finite projective modules over
|
| Vector fields on X |
Hermitian derivations on
|
| Differential forms on X |
Graded-Differential algebra
|
[Previous Segment]: Algebraic Reformulations of Points, Maps,
Direct Products, Symmetry, Compact Groups and Probability Measures
[Next Segment]: Non-commutative Generalizations
|