Sufficient condition for global flatness

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Discussion Overview

The discussion revolves around identifying sufficient conditions for global flatness in compact, orientable n-dimensional Riemannian manifolds. Participants explore theoretical aspects, including connections to the generalized Gauss-Bonnet theorem, holonomy groups, and properties of geodesically complete spaces.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants suggest that a Levi-Civita connection is flat if parallel transport around null homotopic loops is the identity map, implying that the global holonomy group is finite.
  • Others mention that if the Riemannian connection is flat, then the holonomy group must be finite, citing examples like the flat Klein bottle and flat torus.
  • One participant proposes that the exponential map serves as a covering of the manifold by Euclidean space and is a local isometry, noting that the necessary condition from the Gauss-Bonnet theorem is only part of the overall picture.
  • Another participant raises the idea that if the connection is not compatible with any Riemannian metric, it may still be flat while having a non-zero Euler class.
  • Discussion includes the assertion that geodesically complete spaces must be space forms, which are Euclidean modulo a crystallographic group of isometries.
  • Some participants argue that the fundamental group must be an extension of a full lattice by a finite group, which is isomorphic to the holonomy group of the manifold.
  • There is a mention of the Hopf-Rinow theorem in relation to open subsets of geodesically complete spaces.
  • One participant expresses the need to understand the reasoning and proof behind the space form concept, while acknowledging its clarity.
  • Another participant notes that zero holonomy for null homotopic loops should be straightforward and discusses the implications of the exponential map having no singularities.

Areas of Agreement / Disagreement

Participants present multiple competing views regarding sufficient conditions for global flatness, with no consensus reached on a definitive answer. The discussion remains unresolved with various hypotheses and conditions proposed.

Contextual Notes

Limitations include the dependence on definitions of flatness and holonomy, as well as unresolved mathematical steps regarding the implications of various conditions discussed.

tom.stoer
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given a compact, orientable, n-dim. Riemann manifold, what is a sufficient condition for globally vanishing curvature i.e. global flatness?

I can get necessary conditions from the generalized Gauss-Bonnet theorem, but not sufficient ones

thanks in advance
 
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tom.stoer said:
given a compact, orientable, n-dim. Riemann manifold, what is a sufficient condition for globally vanishing curvature i.e. global flatness?

I can get necessary conditions from the generalized Gauss-Bonnet theorem, but not sufficient ones

thanks in advance
I think that a Levi-Civita connection is flat if and only if paralllel translation around null homotopic loops is the identity map. I think one can show that this means that the global holonomy group is finite. In any case, it is true that if the Riemannian connection is flat then the holonomy group is finite.

For instance the flat Klein bottle has holonomy group equal to Z/2Z and the flat torus has trivial holonomy group. One can easily generalize the Klein bottle to make an orientable three manifold whose holonomy group is Z/2Z.

I also think that you should be able to show that the exponential map is a covering of the manifold by Euclidean space and is a local isometry. It you find a proof let me know. The necessary condition that the Gauss Bonnet form is zero is only part of the story. All of the Pontryagin forms are also zero. However, the Stiefel-Whitney classes may not be zero as in the case of the Klein bottle. I will try to construct a flat 4 manifold that has non-zero second Stiefel_Whitney class.

BTW: If the connection is not compatible with any Riemannain metric then it may be flat and still have non-zero Euler class. In such a case, the Euler class can not be expressed in term of the curvature 2 form,
 
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If your space is geodesically complete, then it must be a space form:
See http://en.wikipedia.org/wiki/Space_form

In other words, the space must be Euclidean modulo a crystallographic group of isometries.

Spaces that are not geodesically complete are open subsets of geodesically complete spaces?? I think this is true, but I can't recall the proof. See the Hopf Rinow theorem.
 
Vargo said:
If your space is geodesically complete, then it must be a space form:
See http://en.wikipedia.org/wiki/Space_form

In other words, the space must be Euclidean modulo a crystallographic group of isometries.

The fundamental group must be an extension of a full lattice by a finite group. It must be torsion free and the action of the finite group on the lattice(under conjugation) is a faithful Z-representation of the finite group. The finite group is isomorphic to the holonomy group of the manifold.

Another way of saying this is that the manifold is the quotient of a flat torus by a properly discontinuous action of a finite group of isometries.

This means that the manifold is a K(π,1), that is all of its homotopy groups are zero except its fundamental group.
 
This is great, thanks; I have to invest some time to understand the reasoning and proof behind the space form, but the result is clear and simple
 
tom.stoer said:
This is great, thanks; I have to invest some time to understand the reasoning and proof behind the space form, but the result is clear and simple

- Zero holonomy for null homotopic loops should be the easiest.

- It is clear that the exponential map can have no singularities since there are no conjugate points. But this would also be true for manifolds of negative curvature.

- A properly discontinuous finite group of isometries on a flat torus clearly makes a flat manifold and the fundamental group is an extension the the lattice of covering transformations of the torus. If any of the isometries is a pure translation I suppose you can just mod out by them first to get another flat torus and then you are left with a finite group that acts non-trivially on the torus's tangent plane. The group of isometries of Euclidean space that covers this manifold is clearly torsion free.
 
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