Understanding Contractible Curves

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Contractible curves on a manifold are defined as closed curves that can be continuously shrunk to a point within the manifold itself. If a manifold has a trivial topology, it allows for the global extension of a single neighborhood, making its geometry trivial. However, non-contractible curves, such as those on a torus, cannot be contracted to a point, indicating more complex topology. It's crucial to note that the contraction must occur within the manifold's space, as embedding in a larger space can alter contractibility. Understanding these concepts is essential for grasping local and global geometric properties of manifolds.
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I read some text to find it's definition
Is it possible to tell me it's definition?


I read below statements about local and global geometry and I didn't understand it. is it possible tell me it.
"If M ( a manifold) has a trivial topology, a single neighborhood can be extended globally, and geometry is indeed trivial; but if M contains non-contractible curves, such as extension may not be possible."
 
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hi sadegh4137! :smile:

(if C1 is the unit circle, ie [0,1] with 0 and 1 the same point)

a closed curve f:C1 -> M on a manifold M is contractible if it can be contracted to a point,

ie if there's a continuous function g:[0,1] -> C1M such that each g(t) is continuous, g(0) is a single point, and g(1) is f

eg the surface of a torus is not contractible, since a circle that "loops" the hole cannot be shrunk to a point!
 
tiny-tim said:
hi sadegh4137! :smile:

(if C1 is the unit circle, ie [0,1] with 0 and 1 the same point)

a closed curve f:C1 -> M on a manifold M is contractible if it can be contracted to a point,

ie if there's a continuous function g:[0,1] -> C1M such that each g(t) is continuous, g(0) is a single point, and g(1) is f

eg the surface of a torus is not contractible, since a circle that "loops" the hole cannot be shrunk to a point!

Sorry to nitpick, Tiny Tim, but I think it is important to note that the contraction must be done

within the space ( I thinks this follows from your definition of g , but I think it is important to say it any way, since I think it brings room for confusion ), in case the space is embedded somewhere else. As an example, if we have

## S^1 ## embedded in ## \mathbb R^2 ## , then note that ## S^1 ## --and any curve in it--

can be contracted to a point if we can work in ## \mathbb R^2 ## , but not so if, while doing the deformation , we must stay within ## S^1 ## .
 
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