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We will consider some more examples of convergence in metrics.
First, we look at some examples of convergence in spaces of sequences.
x1 = (1/1 , 1/2 , 1/3 , ... ), x2 = (1/12 , 1/22 , 1/32 , ... ), x3 = (1/13 , 1/23 , 1/33 , ... ) , ...
Then this sequence of sequences converges to the sequence y = (1 , 0 , 0 , 0 , ... ) in d∞.
Proof
d∞(xn, y) = lub { 0 , 1/2n, 1/3n, ... } = 1/2nand this is small when n is large.
Take the sequence in X given by:
x1 = (1 , 0 , 0 , ... ), x2 = (0 , 1 , 0 , ... ), x3 = (0 , 0 , 1 , 0 , ... ), ...
Then although the "sequence of first components", the "sequence of second components", the "sequence of third components", ... all converge to 0, the sequence xn does not converge to the zero sequence: 0, since d∞(xn, 0) = 1 for all n.
So the theorem proved for finite dimensional spaces in the last section does not hold for this infinite dimensional space.
Proof
The maximum of the function |fn(x) - 0| is at x = 1 and is 1/n. Thus the real sequence (d∞(fn, 0))→ 0 and so the 0-function is the limit.
Remarks
We can get a "picture" of what convergence in the metric d∞ "Looks like".
Given a function g on (say) [0, 1], we can draw "An ε-band" around its graph.
Then a function is within ε of g provided its graph lies in this ε band.
Thus a sequence (fn)→ g in d∞ if the graphs of every function "far enough down" the sequence lie in an arbitrarily small ε band.
Define fn(x) by:
Then (fn)→ the 0-function in the metric d1.
Proof
d1(fn, 0) = the area under the curve = 1/n and so (d1(fn, 0))→ 0 and the sequence converges.
Note however, that this sequence does not converge to the 0-function in d∞ since the graph of fn "sticks out" of any small ε band of the 0-function.
Thus it can happen that a sequence which converges in one metric may fail to converge in another.
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