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| | == Simply Connected Spaces == | | == Simply Connected Spaces == |
| | === Intuition === | | === Intuition === |
| − | The easiest topological spaces to deal with, from the standpoint of the fundamental group, are the '''simply connected''' spaces. A space is termed simply connected if every loop in the space is [[homotopy|homotopic]] to a constant loop. The intuition behind this definition is simple: imagine a rubber band is immersed in the topological space. In a simply connected space, the rubber band may contract to a point, while remaining entirely within the space. For example, no matter how a rubber band is arranged on a [[sphere]], it may always be shrunk down while remaining on the sphere. In contrast, it is possible to place a rubber band on a torus in such a way that no such contraction is possible. A few other spaces which have the property of being simply connected are: | + | The easiest topological spaces to deal with, from the standpoint of the fundamental group, are the '''simply connected''' spaces. A space is termed simply connected if every loop in the space is [[homotopy|homotopic]] to a constant loop. The intuition behind this definition is simple: imagine a rubber band is immersed in the topological space. IA simply connected space is one in which the rubber band may always be contracted to a point, while remaining entirely within the space. For example, no matter how a rubber band is arranged on a [[sphere]], it may always be shrunk down while remaining on the sphere. In contrast, it is possible to place a rubber band on a torus in such a way that no such contraction is possible. A few other spaces which have the property of being simply connected are: |
| | * Euclidean space <math>\mathbb R^n</math>. This includes the cases familiar cases of the line (<math>\mathbb R^1</math>), the plane (<math>\mathbb R^2</math>), and 3-dimensional space (<math>\mathbb R^3</math>). | | * Euclidean space <math>\mathbb R^n</math>. This includes the cases familiar cases of the line (<math>\mathbb R^1</math>), the plane (<math>\mathbb R^2</math>), and 3-dimensional space (<math>\mathbb R^3</math>). |
| | * [[Convex]] subsets of Euclidean space. This includes, for example, the unit disk in the plane. | | * [[Convex]] subsets of Euclidean space. This includes, for example, the unit disk in the plane. |
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| | which satisfies | | which satisfies |
| | ::<math>H(t,0)=\gamma_1(t)</math>, <math>H(t,1)=\gamma_2(t)</math>, <math>H(0,s)=H(1,s)=*</math> | | ::<math>H(t,0)=\gamma_1(t)</math>, <math>H(t,1)=\gamma_2(t)</math>, <math>H(0,s)=H(1,s)=*</math> |
| − | The intuition is this: for every value of <math>s \in [0,1]</math>, we get a path <math>\gamma_s(t) : [0,1] \to X</math>, and at <math>s=0</math> and <math>s=1</math>, these are the two paths in question. Thus <math>H</math> provides a smoothly-varying set of paths in <math>X</math>, parametrized by a variable <math>t</math>, starting with <math>\gamma_0</math>, and ending with <math>\gamma_1</math>. | + | The intuition is this: for every value of <math>s \in [0,1]</math>, we get a path <math>\gamma_s(t) : [0,1] \to X</math>, and at <math>s=0</math> and <math>s=1</math>, these are the two paths in question. Thus <math>H</math> provides a smoothly-varying set of paths in <math>X</math>, parametrized by a variable <math>s</math>, starting with <math>\gamma_0</math>, and ending with <math>\gamma_1</math>. |
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| | The constant path is defined by <math>\gamma_c(t) = *</math>, for all <math>t</math>. A space is said to be simply-connected if every path based at <math>*</math> is homotopic to the constant path. This definition serves to make the intuition in terms of shrinking rubber bands precise. | | The constant path is defined by <math>\gamma_c(t) = *</math>, for all <math>t</math>. A space is said to be simply-connected if every path based at <math>*</math> is homotopic to the constant path. This definition serves to make the intuition in terms of shrinking rubber bands precise. |