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John Stillwell - Naive Lie Theory.pdf - Index of

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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

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