1547845440-The_Ricci_Flow_-_Techniques_and_Applications_-_Part_III__Chow_

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  1. ALEKSANDROV SPACES WITH CURVATURE BOUNDED FROM BELOW 409


by
expP (v, t) ~ x.

(iii) The cut locus C (p) of p is the set of x E X such that any minimal


geodesic px is not properly contained in another minimal geodesic
starting from p. We define Gp C Op to consist of those equivalence
classes [ ( v, t)] with the property that there exists x E C (p) such
that v is in the direction of some px and t = d (p, x).

Note that given a geodesic 'Y: [a, b] ---+ X in an Aleksandrov space, it is
not always possible to extend 'Y beyond 'Y (b), i.e., X may not be geodesi-
cally complete.
One application of the notion of the space of directions L;P is in defining
the boundary of an Aleksandrov space.


DEFINITION G.51 (Stratification). Let X be a topological space and let

{Xi}! 1 be a collection of subsets of X. Then {Xi}! 1 is called a stratifi-


cation of X into topological manifolds if


(1) Xi are disjoint topological manifolds without boundary and
N

LJxi =X,


i=l

(2) dimX1 > dimX2 > · · · > dimXN,


(3) the set x: ~ U!k xi is closed in x for each k = 1, ... 'N.


We call the Xi strata of X. The following is part of Theorem 10.10.1


in [18].


THEOREM G.52 (Aleksandrov spaces admit stratifications). If X is an


n-dimensional Aleksandrov space of curvature ?: k, then X admits a strati-
fication into topological manifolds.


We can inductively define the boundary of an Aleksandrov space of


curvature ?: k. The boundary of a 1-dimensional Aleksandrov space is de-
fined to be its topological boundary. Now suppose that the boundary has
been defined for Aleksandrov spaces of curvature bounded from below and
dimension:::; n-1. We define the boundary of an n-dimensional Aleksandrov
space X of curvature bounded from below as the set of points p E X where
the space of directions L;P has nonempty boundary (here we used Theorem
G.49(3)).


2.4.2. The distance function and semi-concave functions on Aleksandrov
spaces with curvature bounded from below.
Given any metric space X, the most natural continuous function is the
distance function d ( ·, p) to a given point p E X. This function plays a
prominent role in comparison geometry and geometric analysis. It is well
known that even if the underlying space X is a smooth manifold, the distance

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