Tangent Spaces Topology for Computing
Theorem 5.2 Integral lines have the following properties:
a Two integral lines are either disjoint or the same. b The integral lines cover all of M.
c And the limits org p and dest p are critical points of h. The properties follow from standard differential calculus.
Definition 5.14 stable and unstable manifolds The stable manifold S p and
the unstable manifold U p of a critical point p are defined as
S p = {p} ∪ {y ∈ M | y ∈ im γ, dest γ = p},
5.4 U
p = {p} ∪ {y ∈ M | y ∈ im γ, org γ = p}, 5.5
where im γ is the image of the path γ ∈ M.
Both sets of manifolds decompose M into open cells.
Definition 5.15 open cell An open d-cell
σ is a space homeomorphic to R
d
. We can predict the dimension of the open cell associated to a critical point p.
Theorem 5.3 The stable manifold S p of a critical point p with index i = ip
is an open cell of dimension dim S
p = i. The unstable manifolds of h are the stable manifolds of
−h as ∇−h = −∇h. Therefore, the two types of manifolds have the same structural properties.
That is, the unstable manifolds of h are also open cells, but with dimension dimU
p = 2 − i, where i is the index of a critical point. The closure of a stable or unstable manifold, however, is not necessarily homeomorphic to a
closed ball. We see this in Figure 5.4, where a stable 2-cell is pinched at a minimum.
By the properties in Theorem 5.2, the stable manifolds are pairwise disjoint and decompose M into open cells. The cells form a complex, as the bound-
ary of every cell S a is a union of lower dimensional cells. We may view a
cellular complex as a generalization of a simplicial complex, where we allow for arbitrarily shaped cells and relax restrictions on how they are connected to
each other. The unstable manifolds similarly decompose M into a complex dual to the
complex of stable manifolds: For a , b ∈ M, dim Sa = 2 − dimUa and Sa
is a face of S b iff Ub is a face of Ua.
Example 5.1 manifolds Figure 5.4 displays the stable and unstable mani- folds of a sphere and a Morse function h. We show an uncompactified sphere:
The boundary of the terrain is a minimum at negative infinity. Note that the stable manifold of a minimum and the unstable manifold of a maximum, are
the critical points themselves, respectively. On the other hand, both the unsta- ble manifold of a minimum and the stable manifold of a maximum are 2-cells.
A saddle has 1-cells as both stable and unstable manifolds. Also, observe that the stable manifolds of the saddles decompose M into the stable manifolds of
the maxima. The unstable manifolds provide such a decomposition for the minima.