John Stillwell - Naive Lie Theory.pdf - Index of
John Stillwell - Naive Lie Theory.pdf - Index of
John Stillwell - Naive Lie Theory.pdf - Index of
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
8.6 Paths and path-connectedness 173<br />
Exercises<br />
The above pro<strong>of</strong> <strong>of</strong> uniform continuity is complicated by the possibility that K is<br />
at least two-dimensional. This forces us to use triangles and the triangle inequality.<br />
If we have K =[0,1] then a more straightforward pro<strong>of</strong> exists.<br />
8.5.1 Suppose that N δ(P1 )(P 1 ) ∪ N δ(P2 )(P 2 ) ∪···∪N δ(Pk )(P k ) is a finite union <strong>of</strong><br />
open intervals that contains [0,1].<br />
Use the finitely many endpoints <strong>of</strong> these intervals to define a number δ > 0<br />
such that any two points P,Q ∈ [0,1] with |P − Q| < δ lie in the same<br />
interval N δ(Pi )(P i ).<br />
8.5.2 Deduce from Exercise 8.5.1 that any continuous function on [0,1] is uniformly<br />
continuous.<br />
8.6 Paths and path-connectedness<br />
The idea <strong>of</strong> a “curve” or “path” has evolved considerably over the course<br />
<strong>of</strong> mathematical history. The old term locus (meaning place in Latin),<br />
shows that a curve was once considered to be the (set <strong>of</strong>) places occupied<br />
by points satisfying a certain geometric condition. For example, a circle is<br />
the locus <strong>of</strong> points at a constant distance from a particular point, the center<br />
<strong>of</strong> the circle. Later, under the influence <strong>of</strong> dynamics, a curve came to be<br />
viewed as the orbit <strong>of</strong> a point moving according to some law <strong>of</strong> motion,<br />
such as Newton’s law <strong>of</strong> gravitation. The position p(t) <strong>of</strong> the moving point<br />
at any time t is some continuous function <strong>of</strong> t.<br />
In topology today, we take the function itself to be the curve. That is,<br />
a curve or path in a space S is a continuous function p : [0,1] → S .The<br />
interval [0,1] plays the role <strong>of</strong> the time interval over which the point is in<br />
motion—any interval would do as well, and it is sometimes convenient to<br />
allow arbitrary closed intervals, as we will do below. More importantly,<br />
thepathisthefunction p and not just its image. A case in which the<br />
image fails quite spectacularly to reflect the function is the space-filling<br />
curve discovered by Peano in 1890. The image <strong>of</strong> Peano’s curve is a square<br />
region <strong>of</strong> the plane, so the image cannot tell us even the endpoints A = f (0)<br />
and B = f (1) <strong>of</strong> the curve, let alone how the curve makes its way from A<br />
to B.<br />
In <strong>Lie</strong> theory, paths give a way to distinguish groups that are “all <strong>of</strong> a<br />
piece,” such as the circle group SO(2), from groups that consist <strong>of</strong> “separate<br />
pieces,” such as O(2). In Chapter 3 we showed connectedness by