Affine manifold

In differential geometry, an affine manifold is a differentiable manifold equipped with a flat, torsion-free connection.

Equivalently, it is a manifold that is (if connected) covered by an open subset of {\Bbb R}^n, with monodromy acting by affine transformations. This equivalence is an easy corollary of Cartan–Ambrose–Hicks theorem.

Equivalently, it is a manifold equipped with an atlas—called the affine structure—with all transition functions between charts affine (that is, have constant jacobian matrix);[1] two atlases are equivalent if the manifold admits an atlas subjugated to both, with transitions from both atlases to a smaller atlas being affine. A manifold having a distinguished affine structure is called an affine manifold and the charts which are affinely related to those of the affine structure are called affine charts. In each affine coordinate domain the coordinate vector fields form a parallelization of that domain, so there is an associated connection on each domain. These locally defined connections are the same on overlapping parts, so there is a unique connection associated with an affine structure. Note there is a link between linear connection (also called affine connection) and a web.

Formal definition

An affine manifold M\, is a real manifold with charts \psi_i\colon U_i\to{\Bbb R}^n such that \psi_i\circ\psi_j^{-1}\in {\rm Aff}({\Bbb R}^n) for all i, j\, , where {\rm Aff}({\Bbb R}^n) denotes the Lie group of affine transformations.

An affine manifold is called complete if its universal covering is homeomorphic to {\Bbb R}^n.

In the case of a compact affine manifold M, let G be the fundamental group of M and \tilde M be its universal cover. One can show that each n-dimensional affine manifold comes with a developing map D\colon {\tilde M}\to{\Bbb R}^n, and a homomorphism \varphi\colon G\to {\rm Aff}({\Bbb R}^n), such that D is an immersion and equivariant with respect to \varphi.

A fundamental group of a compact complete flat affine manifold is called an affine crystallographic group. Classification of affine crystallographic groups is a difficult problem, far from being solved. The Riemannian crystallographic groups (also known as Bieberbach groups) were classified by Ludwig Bieberbach, answering a question posed by David Hilbert. In his work on Hilbert's 18-th problem, Bieberbach proved that any Riemannian crystallographic group contains an abelian subgroup of finite index.

Important longstanding conjectures

Geometry of affine manifolds is essentially a network of longstanding conjectures; most of them proven in low dimension and some other special cases.

The most important of them are

Notes

  1. Bishop, R.L.; Goldberg, S.I. (1968), pp. 223–224.
  2. Hirsch M. and Thurston W., Foliated bundles, invariant measures, and flat manifolds, Ann. Math. (2) 101, (1975) 369–390.
  3. Auslander L., The structure of locally complete affine manifolds, Topology 3 (1964), 131–139.
  4. Fried D. and Goldman W., Three dimensional affine crystallographic groups, Adv. Math. 47 (1983), 1–49.
  5. H. Abels, G. A. Margulis and G. A. Soifer, On the Zariski closure of the linear part of a properly discontinuous group of affine transformations, J. Differential Geom., 60 (2002), 315344.
  6. William M. Goldman and Yoshinobu Kamishima, The fundamental group of a compact flat Lorentz space form is virtually polycyclic, J. Differential Geom. Volume 19, Number 1 (1984)
  7. Herbert Abels, Properly Discontinuous Groups of Affine Transformations: A Survey, Geom. Dedicata, 87,. 309–333 (2001)
  8. Kostant B., Sullivan D., The Euler characteristic of an affine space form is zero, Bull. Amer. Math. Soc. 81 (1975), no. 5, 937–938.

References

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