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Vol. 10 No 6 - Pi Mu Epsilon

Vol. 10 No 6 - Pi Mu Epsilon

Vol. 10 No 6 - Pi Mu Epsilon

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468 PI MU EPSILON JOURNAL<br />

VISUAL REPRESENTATION OF THE SEQUENCE SPACE 469<br />

Define Yn: (En, d.,) -<br />

(R", dG) by<br />

y n (a 0<br />

a 1<br />

••• a.,_J = (s 0 , s 1<br />

, ••• , sn_ 1 )<br />

ai<br />

w h ere s 1 = 1<br />

.<br />

2<br />

We will prove that y n is an isometry and thus that its image is a model<br />

of :E.. in (It", dG) •<br />

For example, consider El . The image of L 1<br />

points, as pictured in Figure l(a.).<br />

l D D<br />

Figure 1<br />

contains only two<br />

<strong>No</strong>w let us consider ~ . Its image consists of four points in the plane<br />

arranged as shown in Figure l(b.). y 3 (L ) 3<br />

is pictured in Figure l(c.).<br />

Continuing this way we could easily model Ln in n-space. However this<br />

n-dimensional model is more difficult to visualize for large n, and the<br />

analogous model for :E would be a subspace of Reo, hardly an easy thing<br />

to visualize. So we would like to find a way of "compressing" the entire<br />

space into three or fewer dimensions. In fact we will be able to fit it into<br />

two dimensions.<br />

To do this we should first consider y 3 (L 3<br />

). Think of it as a box sitting<br />

on the floor in front of you. The box has length one unit, width one half<br />

unit, and height one quarter unit. You can find the distance between any<br />

two points in ~ by measuring the length of any shortest path which travels<br />

along the edges of the box between the corresponding points in y 3 (L 3<br />

)·<br />

<strong>No</strong>w take your Swiss Army knife out of your pocket and cut off the 1 /2 by<br />

1.4 sides. Step on the box gently. Don't bend the sides; let it bend at the<br />

edges. You have just transformed a three dimensional model into a two<br />

dimensional model. In an analogous manner we can "crush" our higher<br />

dimensional models of :E.. into R 2 •<br />

In this paper we develop a model which "crushes" :E into the real<br />

e in an analogous manner. However, before we consider this model we<br />

look at a model for a much simpler space to develop our intuition for<br />

we mean by a "geometric model."<br />

Modeling the Discrete Metric<br />

To illustrate the kind of geometric model we have in mind, let us first<br />

ider a similar model for a simpler metric space: the discrete metric on<br />

a set X. Under the discrete metric the distance between any two distinct<br />

- ts of X is one. Our model will have four key ingredients: 1) a set of<br />

• ts, p (corresponding to the points of X),2) a set of line segments<br />

viding paths between any two points),3) a definition of a unique<br />

per" path between any two points, and 4) a metric induced on P (by<br />

ring the Euclidean lengths of the line segments in the proper path<br />

·een two points). In the case of the discrete metric we can define these<br />

items as follows.<br />

Points<br />

Let the set of points, P C R 2 , consist of the n equally spaced points on<br />

circle of radius 1 /z (that is, in polar coordinates<br />

p = { ( t , 6) I t = ~ and 6 = 2 : , x E 0, 1, ... , n - 1})<br />

shown in Figure 2(a.) for x = 8.<br />

•<br />

• •<br />

• •<br />

•<br />

•<br />

•<br />

(a.) p<br />

(b.) P and S<br />

Figure 2 ·.

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