Atiyah algebroid explained
In mathematics, the Atiyah algebroid, or Atiyah sequence, of a principal
-bundle
over a manifold
, where
is a Lie group, is the Lie algebroid of the gauge groupoid of
. Explicitly, it is given by the following short exact sequence of vector bundles over
:0\toP x Gakg\toTP/G\toTM\to0.
It is named after
Michael Atiyah, who introduced the construction to study the existence theory of
complex analytic connections.
[1] It plays a crucial example in the integrability of (transitive) Lie algebroids, and it has applications in
gauge theory and
geometric mechanics.
Definitions
As a sequence
over a manifold
, the
differential
of the projection
defines a short exact sequence:
0\toVP\toTP\xrightarrow{d\pi}\pi*TM\to0
of vector bundles over
, where the
vertical bundle
is the kernel of
.
If
is a principal
-bundle, then the group
acts on the vector bundles in this sequence. Moreover, since the vertical bundle
is isomorphic to the trivial vector bundle
, where
is the Lie algebra of
, its quotient by the diagonal
action is the adjoint bundle
. In conclusion, the quotient by
of the exact sequence above yields a short exact sequence: of vector bundles over
, which is called the Atiyah sequence of
.As a Lie algebroid
Recall that any principal
-bundle
has an associated Lie groupoid, called its gauge groupoid, whose objects are points of
, and whose morphisms are elements of the quotient of
by the diagonal action of
, with source and target given by the two projections of
. By definition, the Atiyah algebroid of
is the Lie algebroid
of its gauge groupoid.It follows that
, while the anchor map
is given by the differential
, which is
-invariant. Last, the kernel of the anchor is isomorphic precisely to
.
The Atiyah sequence yields a short exact sequence of
-modules by taking the space of sections of the vector bundles. More precisely, the sections of the Atiyah algebroid of
is the Lie algebra of
-invariant vector fields on
under Lie bracket, which is an extension of the Lie algebra of vector fields on
by the
-invariant vertical vector fields. In algebraic or analytic contexts, it is often convenient to view the Atiyah sequence as an exact sequence of sheaves of local sections of vector bundles.Examples
- The Atiyah algebroid of the principal
-bundle
is the Lie algebra
- The Atiyah algebroid of the principal
-bundle
is the tangent algebroid
-action on
, the Atiyah algebroid of the principal bundle
, with structure group the isotropy group
of the action at an arbitrary point, is the action algebroid
is the general linear algebroid
(sometimes also called Atiyah algebroid of
)Properties
Transitivity and integrability
The Atiyah algebroid of a principal
-bundle
is always:- Transitive (so its unique orbit is the entire
and its isotropy Lie algebra bundle is the associated bundle
)- Integrable (to the gauge groupoid of
)
Note that these two properties are independent. Integrable Lie algebroids does not need to be transitive; conversely, transitive Lie algebroids (often called abstract Atiyah sequences) are not necessarily integrable.
While any transitive Lie groupoid is isomorphic to some gauge groupoid, not all transitive Lie algebroids are Atiyah algebroids of some principal bundle. Integrability is the crucial property to distinguish the two concepts: a transitive Lie algebroid is integrable if and only if it is isomorphic to the Atiyah algebroid of some principal bundle.
Relations with connections
of the Atiyah sequence of a principal bundle
are in bijective correspondence with principal connections on
. Similarly, the curvatures of such connections correspond to the two forms
\Omega\sigma\in\Omega2(M,P[ak{g}])
defined by:
Morphisms
Any morphism
of principal bundles induces a Lie algebroid morphism
between the respective Atiyah algebroids.
References
Notes and References
- Atiyah. M. F.. 1957. Complex analytic connections in fibre bundles. Transactions of the American Mathematical Society. en. 85. 1. 181–207. 10.1090/S0002-9947-1957-0086359-5. 0002-9947. free.