WEBVTT

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[SQUEAKING]

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[RUSTLING]

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[CLICKING]

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PROFESSOR: So we're
going to prove

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the Picard-Lindelof theorem.

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And we'll see.

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It may take us--

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we may need to continue
on it also on Tuesday.

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And then when
we're done with it,

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we will just do
review on Tuesday.

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But let's see how far we get.

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So the Picard-Lindelof theorem
is the following theorem.

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And it says that
it's an ODE, so it's

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what's called an ordinary
differential equation.

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And so again, a
differential equation

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is something about an unknown
function and its derivative.

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So a differential equation
just means it's an equation.

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So this here means that it's an
equation in an unknown function

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and its derivative.

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Ordinary, just as we
talked about last time,

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ordinary refers to that
is just of one variable.

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And so the ODE that the
Picard-Lindelof theorem is about

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is--

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so the unknown function
is y, and the ODE

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is this that we
want the derivative

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of this unknown function
to be equal to a function

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of the unknown function,
plus another function that

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just depends on x.

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So y here is the
unknown function,

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and y is a function of x.

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x is a real number.

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And it's just a-- yeah.

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So this is the
differential equation,

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and then we have some
initial condition.

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So at zero, we want it
to take a value "a."

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So this is the
differential equation.

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And what we assume here is--
so f and g are function on R.

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And you should think about those
as being known, and they are--

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and f here is differentiable.

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And the derivative
is continuous,

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and g is just continuous.

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Doesn't need to
be differentiable.

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And the Picard-Lindelof
theorem is--

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so again, the Picard-Lindelof
theorem is the following,

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that given f of g as above and--

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sorry.

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And a, a was this constant.

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It's just a real
number, as above.

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There exists a delta greater
than zero, such that--

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and a solution.

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y defined on the integral
from minus delta to delta

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and a solution y to the ODE.

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And so again, meaning
that the solution--

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that means that at
zero, it takes value a,

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and then is satisfying
that equation.

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And moreover, and I'll get
back to that, but we won't.

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It's quite possible I
won't get to that today.

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Moreover, solutions are unique.

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And so this is like
a standard problem,

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in when you're looking at
differential equations,

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you have a differential equation
that may describe something

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in nature.

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And you wonder, does this
equation have a solution?

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And if it has a solution,
are solutions unique?

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So this is what this
answer in this case.

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And the interesting thing, or
part of the interesting thing,

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so this is a
fundamental question

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used all over science
and engineering.

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And one of the
interesting things

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is that it uses the proof
of this uses metric spaces.

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And so the proof has been used--

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various versions
of The proof have

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been used to prove
existence and uniqueness

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of various
differential equations.

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So the proof uses the theory
of metric spaces, which

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is sort of surprising because
it seems to have nothing

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to do with metric spaces.

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And so it uses, in particular,
the metric space that it's using

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is the continuous functions
on some interval here.

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And on the space of
continuous function,

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we have the metric that we
talked about, the metric.

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So if f and g--

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so f is bad because it's the n.

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g also.

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Let's call it h1 and h2.

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Suppose that these are
continuous functions.

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h1 and h2 are
continuous functions

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on an interval like this.

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Then the distance
is this that we

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have considered various times.

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This is just the maximum
over x in this interval here

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of f of x, of h1--

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sorry.

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h1 of x minus h2 of x, and then
the absolute value of that.

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So this is the distance on the
space of continuous functions

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that we have looked at a lot.

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And it's actually not quite this
space, as I mentioned last time.

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It's a ball in this
space that it's using.

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So what do we need
about this metric space?

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So one thing we've proven
a couple of lectures ago

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is that the space here
of continuous functions

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with this metric here
is Cauchy complete.

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So we're going to use that.

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Another thing we're
going to use is

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this notion of contracting map.

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So another tool will be
that of a contracting map.

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And remember, this is a
number of lectures ago.

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We talked about a
contracting map,

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but we need a more general
notion of contracting map,

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because when we talked about
it, we talked about a map from R

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into R. And then we used this
notion of contracting map

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to finding zeros
using Newton's method.

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But here we're going to use
it for something different,

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and so we need a
more general notion.

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So suppose so a contracting
map uses the general version as

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opposed to the
version that we talked

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about already that was for the
line for R. So contracting map.

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Sorry.

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And so you have a
metric space x, d.

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It could be like
this, but it also just

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could be any metric space.

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And then you have a map from
this metric space into the self.

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And T here is said to be--

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T is said to be contracting.

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If there exists a
constant c less than 1,

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such that if you're looking at
the distance between the images,

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then they are squeezed together.

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So this distance here between
the images under the map

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is less than or equal
to this constant

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that is less than 1
times the distance

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before you apply the map.

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So this means that under the
map, things get closer together.

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So that's a contracting map.

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And so now, we
prove the theorem.

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When we did the Newton's
method, we proved a theorem,

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but we needed
about fixed points.

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And we need a generalized
version of that.

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So if you take a map just
in general from a space

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to a space, then a fixed
point, a fixed point

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is a point x in the space.

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So that T of x.

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So the T leaves x invariant.

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So T of x is equal to x.

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That's a fixed point.

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And so now, if you
have a contracting map,

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so if T here is
contracting, then T

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can have at most
one fixed point.

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Why?

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Because suppose that x-- so
if x and y are both fixed

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points, well, then you have
that T of x is equal to T of y.

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Sorry.

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T of x is equal to x,
and T of y is equal to y.

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And so now you have that
the distance between T of x.

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Let me make a little more space.

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Then you have the--

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actually, we'll just
continue down here.

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So that the distance between
T of x, comma, T of y--

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the map is
contracting, so this is

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less than or equal to this
constant times this year.

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On the other hand,
they're both fixed points.

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So T of x is x.

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This has x, and this has y.

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So if we write this out,
so this is x comma y.

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And so you see that
this thing here

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is some constant less than
1, strictly less than 1,

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times itself.

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So this means, of course,
that this number here,

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this non-negative
number must be zero.

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And so this, of course, implies
by the actions of a metric space

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that x is equal to y.

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So a contracting map has
at most one fixed point.

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Now, the other thing is that
if you take a metric space--

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if you take a metric space, so
this here is Cauchy complete.

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So now I'm going to take a
Cauchy complete metric space.

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So it could be continuous
function on some closed

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interval, and that's
how we will apply it,

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but it works more generally.

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So we have this fine theorem.

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So if this here a Cauchy
complete metric space,

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and T from x into x
is a contracting map,

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then T has a unique fixed point.

00:15:56.800 --> 00:16:01.720 align:middle line:84%
We know it only has at most
one, so this statement really

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is that it has one right.

00:16:05.390 --> 00:16:07.520 align:middle line:90%
So it has a unique fixed point.

00:16:07.520 --> 00:16:13.064 align:middle line:90%


00:16:13.064 --> 00:16:16.695 align:middle line:90%
So let's try to prove this.

00:16:16.695 --> 00:16:19.600 align:middle line:90%


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And you might remember.

00:16:22.420 --> 00:16:24.590 align:middle line:90%
And if you don't, that's fine.

00:16:24.590 --> 00:16:28.700 align:middle line:84%
But you might remember how we
used it in the Newton method

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because the Newton
method was like--

00:16:30.880 --> 00:16:37.130 align:middle line:84%
it was a version of this on
R. So you had a map from R

00:16:37.130 --> 00:16:39.900 align:middle line:84%
to R, and to find
the fixed point.

00:16:39.900 --> 00:16:41.870 align:middle line:84%
And so you wondered
what you were there,

00:16:41.870 --> 00:16:43.610 align:middle line:84%
and your Newton
method was something

00:16:43.610 --> 00:16:47.160 align:middle line:84%
about finding a point
where a function vanishes.

00:16:47.160 --> 00:16:50.960 align:middle line:84%
And that was set up as
a fixed point theorem.

00:16:50.960 --> 00:16:54.530 align:middle line:84%
And so what you did is
you made a good choice,

00:16:54.530 --> 00:16:57.650 align:middle line:84%
I mean, a choice that
looked reasonable.

00:16:57.650 --> 00:17:01.050 align:middle line:84%
This is not exactly where
the function vanishes,

00:17:01.050 --> 00:17:03.870 align:middle line:84%
but something that looks
close to where it vanishes.

00:17:03.870 --> 00:17:06.210 align:middle line:90%
And then you iterate.

00:17:06.210 --> 00:17:10.170 align:middle line:84%
You took the image under the
map and you iterated this.

00:17:10.170 --> 00:17:13.399 align:middle line:84%
And so it's the same
we're going to do here.

00:17:13.399 --> 00:17:18.349 align:middle line:84%
And this time, we don't even
need to make a good choice.

00:17:18.349 --> 00:17:20.720 align:middle line:90%
So we just take a--

00:17:20.720 --> 00:17:27.720 align:middle line:84%
we just take-- let x here be
any point in the metric space.

00:17:27.720 --> 00:17:31.280 align:middle line:84%
So you just fixing some
point in the metric space.

00:17:31.280 --> 00:17:33.360 align:middle line:90%
And now you're looking at--

00:17:33.360 --> 00:17:36.970 align:middle line:84%
so you're looking at
the sequence x, T of x,

00:17:36.970 --> 00:17:41.120 align:middle line:90%
and then you apply T to T of x.

00:17:41.120 --> 00:17:43.250 align:middle line:90%
So I write this as this.

00:17:43.250 --> 00:17:45.790 align:middle line:84%
And then you apply
T to T squared

00:17:45.790 --> 00:17:48.790 align:middle line:90%
of x, so that's like this.

00:17:48.790 --> 00:17:53.890 align:middle line:84%
And so you keep applying
T more and more times,

00:17:53.890 --> 00:17:57.710 align:middle line:84%
and so this gives you
a sequence, and so on.

00:17:57.710 --> 00:18:00.160 align:middle line:90%
So this gives you a sequence.

00:18:00.160 --> 00:18:03.500 align:middle line:84%
And now the claim is
that this sequence here--

00:18:03.500 --> 00:18:15.440 align:middle line:84%
so I claim that this
sequence here converge to--

00:18:15.440 --> 00:18:19.000 align:middle line:84%
so it converge,
and the limit here,

00:18:19.000 --> 00:18:30.100 align:middle line:84%
this here, is a fixed point
for T. So that's the claim.

00:18:30.100 --> 00:18:34.280 align:middle line:90%


00:18:34.280 --> 00:18:41.196 align:middle line:84%
Now, so we wanted to prove
first that is converging.

00:18:41.196 --> 00:18:50.380 align:middle line:90%


00:18:50.380 --> 00:18:52.770 align:middle line:90%
So we're going to prove first--

00:18:52.770 --> 00:19:07.765 align:middle line:84%
so we'll first show that
Tn is a Cauchy sequence.

00:19:07.765 --> 00:19:15.230 align:middle line:90%


00:19:15.230 --> 00:19:17.960 align:middle line:90%
So now let's look at--

00:19:17.960 --> 00:19:20.900 align:middle line:84%
so we're supposed to look-- if
you're looking at a Cauchy--

00:19:20.900 --> 00:19:24.060 align:middle line:84%
if you try to prove that
something is a Cauchy sequence,

00:19:24.060 --> 00:19:28.880 align:middle line:84%
then you're looking at the
distance between elements

00:19:28.880 --> 00:19:33.330 align:middle line:84%
in the sequence where
both of these elements

00:19:33.330 --> 00:19:36.120 align:middle line:90%
is sufficiently far.

00:19:36.120 --> 00:19:39.060 align:middle line:84%
That's what you're
supposed to look at.

00:19:39.060 --> 00:19:42.130 align:middle line:90%
And so let me write the m here.

00:19:42.130 --> 00:19:44.700 align:middle line:84%
So I can think about
one of them as being

00:19:44.700 --> 00:19:46.390 align:middle line:90%
further out than the other one.

00:19:46.390 --> 00:19:48.330 align:middle line:84%
So I'm going to
think about m here

00:19:48.330 --> 00:19:55.020 align:middle line:84%
as being n plus some
number k, some integer k.

00:19:55.020 --> 00:19:57.870 align:middle line:84%
And so I'm interested
in estimating

00:19:57.870 --> 00:20:07.745 align:middle line:84%
the distance between Tn
of x and Tn plus k of x.

00:20:07.745 --> 00:20:12.420 align:middle line:90%


00:20:12.420 --> 00:20:18.330 align:middle line:84%
Now, in order to do
this, let me start

00:20:18.330 --> 00:20:23.340 align:middle line:90%
with something simpler first.

00:20:23.340 --> 00:20:28.520 align:middle line:84%
Let me look at the
distance between T of x.

00:20:28.520 --> 00:20:31.180 align:middle line:90%


00:20:31.180 --> 00:20:42.370 align:middle line:84%
Let me look at the distance
between Tl of x and Tl

00:20:42.370 --> 00:20:46.420 align:middle line:90%
plus 1 of x.

00:20:46.420 --> 00:20:50.570 align:middle line:84%
So two consecutive
elements in the sequence.

00:20:50.570 --> 00:20:56.170 align:middle line:84%
Now, I can think that this
thing here, well, this

00:20:56.170 --> 00:21:07.780 align:middle line:84%
is equal to the distance
between T of Tl minus 1 of x.

00:21:07.780 --> 00:21:16.115 align:middle line:84%
And then T of Tl
of x, like that.

00:21:16.115 --> 00:21:17.670 align:middle line:90%
I can write it like that.

00:21:17.670 --> 00:21:21.340 align:middle line:90%


00:21:21.340 --> 00:21:24.130 align:middle line:84%
But now, of course, so
you see here there's

00:21:24.130 --> 00:21:28.310 align:middle line:84%
some elements in
x in the space x.

00:21:28.310 --> 00:21:31.130 align:middle line:90%
Here's has another element.

00:21:31.130 --> 00:21:33.500 align:middle line:90%
They both have T applied to it.

00:21:33.500 --> 00:21:44.620 align:middle line:84%
T is contracting, so you gets
c, Tl minus 1, x, Tl of x.

00:21:44.620 --> 00:21:47.690 align:middle line:90%


00:21:47.690 --> 00:21:52.430 align:middle line:84%
So you see that if you take
two consecutive elements

00:21:52.430 --> 00:21:55.010 align:middle line:84%
and you're taking
the distance, then

00:21:55.010 --> 00:22:02.880 align:middle line:84%
it's bounded by this constant
c times where you have 1 less--

00:22:02.880 --> 00:22:06.840 align:middle line:84%
where you have applied
T 1 less time on both.

00:22:06.840 --> 00:22:09.770 align:middle line:84%
These are, again,
consecutive elements,

00:22:09.770 --> 00:22:12.185 align:middle line:90%
but the highest one is 1 less.

00:22:12.185 --> 00:22:14.810 align:middle line:90%


00:22:14.810 --> 00:22:29.010 align:middle line:84%
So now, if you iterate this, so
iterating this, so let's see.

00:22:29.010 --> 00:22:32.500 align:middle line:84%
Maybe let me wait
with iterating.

00:22:32.500 --> 00:22:35.590 align:middle line:84%
Let me just look
at what we need.

00:22:35.590 --> 00:22:39.090 align:middle line:90%
So we have this thing here.

00:22:39.090 --> 00:22:43.770 align:middle line:90%
And this here I can write as--

00:22:43.770 --> 00:22:50.610 align:middle line:84%
so here you see, here I can
write this as T, the distance T,

00:22:50.610 --> 00:23:03.030 align:middle line:84%
And then Tn minus 1x, and
then T, Tn minus 1 plus kx,

00:23:03.030 --> 00:23:05.916 align:middle line:90%
like this.

00:23:05.916 --> 00:23:12.520 align:middle line:84%
And so here I can use the
same trick that you guys see,

00:23:12.520 --> 00:23:23.160 align:middle line:84%
and then d, Tn minus 1x
comma Tn minus 1 plus k of x.

00:23:23.160 --> 00:23:27.400 align:middle line:90%


00:23:27.400 --> 00:23:28.730 align:middle line:90%
And this one here.

00:23:28.730 --> 00:23:31.450 align:middle line:90%
I can keep going like this.

00:23:31.450 --> 00:23:36.830 align:middle line:84%
I can keep going
until there is the--

00:23:36.830 --> 00:23:40.540 align:middle line:90%
I've used up all my ends.

00:23:40.540 --> 00:23:42.410 align:middle line:90%
And so I can keep going.

00:23:42.410 --> 00:23:45.710 align:middle line:84%
And so this is less or
equal to c to the n.

00:23:45.710 --> 00:23:54.510 align:middle line:84%
And then the last one I get is,
I get x, and then I get Tk of x.

00:23:54.510 --> 00:24:01.200 align:middle line:90%


00:24:01.200 --> 00:24:06.070 align:middle line:84%
I want to show that this
thing here becomes small

00:24:06.070 --> 00:24:11.080 align:middle line:84%
as long as n-- remember, k is
a positive integer as long as n

00:24:11.080 --> 00:24:12.130 align:middle line:90%
is sufficiently large.

00:24:12.130 --> 00:24:14.900 align:middle line:90%


00:24:14.900 --> 00:24:18.490 align:middle line:84%
So this is a hopeful sign,
because when n gets large,

00:24:18.490 --> 00:24:20.560 align:middle line:84%
this here gets
really, really small.

00:24:20.560 --> 00:24:23.800 align:middle line:84%
But I still need to
estimate this here.

00:24:23.800 --> 00:24:25.580 align:middle line:90%
Now, so how do I estimate it?

00:24:25.580 --> 00:24:28.280 align:middle line:90%
By using what I did over here.

00:24:28.280 --> 00:24:35.780 align:middle line:90%
So you're looking at--

00:24:35.780 --> 00:24:45.800 align:middle line:84%
so you have the distance
between x and Tk of x.

00:24:45.800 --> 00:24:49.410 align:middle line:84%
This thing here, I can use
this triangle inequality.

00:24:49.410 --> 00:24:55.640 align:middle line:84%
So I can say that this
is less than dx T of x

00:24:55.640 --> 00:25:07.940 align:middle line:84%
plus dT of x, T
squared of x plus dT

00:25:07.940 --> 00:25:13.080 align:middle line:90%
squared of x, cubed of x.

00:25:13.080 --> 00:25:25.320 align:middle line:84%
And then all the way up to
d, Tk minus 1 of x, Tk of x.

00:25:25.320 --> 00:25:27.480 align:middle line:84%
So this is just the
triangle inequality.

00:25:27.480 --> 00:25:30.360 align:middle line:90%


00:25:30.360 --> 00:25:33.150 align:middle line:84%
Now, this may seem
rather bad estimate,

00:25:33.150 --> 00:25:35.890 align:middle line:90%
but let's see how bad it is.

00:25:35.890 --> 00:25:41.280 align:middle line:84%
So now, this first thing
here, I'm just leaving it.

00:25:41.280 --> 00:25:42.970 align:middle line:90%
I can't do anything about that.

00:25:42.970 --> 00:25:46.650 align:middle line:90%
So I need to just take that.

00:25:46.650 --> 00:25:52.060 align:middle line:84%
This one here, so I'm using this
with between two consecutive.

00:25:52.060 --> 00:25:59.064 align:middle line:84%
So in this case, it's just
bounded by c times dx, Tx.

00:25:59.064 --> 00:26:02.130 align:middle line:90%


00:26:02.130 --> 00:26:05.550 align:middle line:84%
And the next one
here, this one here

00:26:05.550 --> 00:26:12.090 align:middle line:90%
is bounded by c squared, dx, Tx.

00:26:12.090 --> 00:26:18.960 align:middle line:84%
And the next, and so
on, up to this one here

00:26:18.960 --> 00:26:28.560 align:middle line:84%
is bounded by a c,
k minus 1, dx, Tx.

00:26:28.560 --> 00:26:31.940 align:middle line:90%


00:26:31.940 --> 00:26:36.290 align:middle line:84%
And so you see that now,
this here factor out.

00:26:36.290 --> 00:26:38.865 align:middle line:84%
So this here is
this factored out.

00:26:38.865 --> 00:26:41.380 align:middle line:90%


00:26:41.380 --> 00:26:44.320 align:middle line:84%
And then, in this
bracket, you get

00:26:44.320 --> 00:26:51.830 align:middle line:84%
1 plus c plus c squared, plus
all the way up to ck minus 1.

00:26:51.830 --> 00:26:54.980 align:middle line:90%
But this is a geometric series.

00:26:54.980 --> 00:26:57.160 align:middle line:90%
This is a geometric series.

00:26:57.160 --> 00:27:01.670 align:middle line:84%
And this is certainly
less than when I take--

00:27:01.670 --> 00:27:04.040 align:middle line:84%
remember c is
strictly less than 1.

00:27:04.040 --> 00:27:05.600 align:middle line:90%
So it's a geometric series.

00:27:05.600 --> 00:27:07.760 align:middle line:84%
It's a convergent
geometric series.

00:27:07.760 --> 00:27:12.610 align:middle line:84%
So this here is less
than dx, T of x.

00:27:12.610 --> 00:27:16.120 align:middle line:84%
And then this sum,
well, it's less

00:27:16.120 --> 00:27:19.100 align:middle line:84%
than when you're summing
it all the way to infinity.

00:27:19.100 --> 00:27:21.620 align:middle line:90%
So this is less than 1.

00:27:21.620 --> 00:27:24.150 align:middle line:84%
This is the sum of
the geometric series.

00:27:24.150 --> 00:27:27.840 align:middle line:90%
C is strictly less than 1.

00:27:27.840 --> 00:27:30.085 align:middle line:84%
C is positive, and it's
strictly less than 1.

00:27:30.085 --> 00:27:33.596 align:middle line:90%


00:27:33.596 --> 00:27:37.880 align:middle line:90%
So/ you see now that we have--

00:27:37.880 --> 00:27:40.440 align:middle line:90%
so we have that.

00:27:40.440 --> 00:27:42.350 align:middle line:84%
So what we were
interested in is,

00:27:42.350 --> 00:27:44.810 align:middle line:84%
we were interested in
saying that, as long

00:27:44.810 --> 00:27:47.340 align:middle line:84%
as I choose little n
sufficiently large,

00:27:47.340 --> 00:27:51.590 align:middle line:84%
then this thing here
must be very small.

00:27:51.590 --> 00:27:54.540 align:middle line:84%
And we know already that
it's bounded like this.

00:27:54.540 --> 00:27:57.990 align:middle line:84%
And now I fill in this,
and you see this here.

00:27:57.990 --> 00:28:01.110 align:middle line:84%
So this means that
this is less than cn.

00:28:01.110 --> 00:28:08.120 align:middle line:84%
And then what you get here
is 1 minus c, and then

00:28:08.120 --> 00:28:13.680 align:middle line:90%
times dx T of x.

00:28:13.680 --> 00:28:18.540 align:middle line:84%
x is fixed, and so you
see that when n, little n,

00:28:18.540 --> 00:28:21.690 align:middle line:84%
is sufficiently large,
then this whole thing here

00:28:21.690 --> 00:28:24.060 align:middle line:90%
is as small as you want.

00:28:24.060 --> 00:28:27.000 align:middle line:84%
So this means that what
we have proven here

00:28:27.000 --> 00:28:32.465 align:middle line:84%
is that this sequence
here is a Cauchy sequence.

00:28:32.465 --> 00:28:39.570 align:middle line:90%


00:28:39.570 --> 00:28:40.565 align:middle line:90%
So we have proven that.

00:28:40.565 --> 00:28:43.695 align:middle line:90%


00:28:43.695 --> 00:28:46.440 align:middle line:84%
Now, of course, this is
where the assumption comes in

00:28:46.440 --> 00:28:51.490 align:middle line:84%
that this metric space
is Cauchy complete.

00:28:51.490 --> 00:29:10.560 align:middle line:84%
So since x, this metric
space is Cauchy complete,

00:29:10.560 --> 00:29:25.010 align:middle line:84%
and this sequence here
is a Cauchy sequence,

00:29:25.010 --> 00:29:27.206 align:middle line:90%
it is convergent.

00:29:27.206 --> 00:29:31.884 align:middle line:90%


00:29:31.884 --> 00:29:32.658 align:middle line:90%
Yeah.

00:29:32.658 --> 00:29:33.450 align:middle line:90%
STUDENT: I'm sorry.

00:29:33.450 --> 00:29:34.950 align:middle line:84%
Just back to the
end of that repeat.

00:29:34.950 --> 00:29:35.840 align:middle line:90%
PROFESSOR: Yeah.

00:29:35.840 --> 00:29:39.290 align:middle line:84%
STUDENT: Are you able to explain
again how we got that feature,

00:29:39.290 --> 00:29:40.730 align:middle line:90%
or how we were trying to--

00:29:40.730 --> 00:29:46.190 align:middle line:84%
did we find a bound for the dx,
Tx, or we're just saying that--

00:29:46.190 --> 00:29:48.750 align:middle line:84%
PROFESSOR: So I'm
saying that x is fixed.

00:29:48.750 --> 00:29:55.001 align:middle line:84%
You pick any point you want,
and I claim that if I--

00:29:55.001 --> 00:29:58.260 align:middle line:84%
it may be a very bad
candidate for the fixed point,

00:29:58.260 --> 00:29:59.370 align:middle line:90%
but it doesn't matter.

00:29:59.370 --> 00:30:00.500 align:middle line:90%
It's OK.

00:30:00.500 --> 00:30:03.270 align:middle line:84%
It may just take you longer
to get to the fixed point.

00:30:03.270 --> 00:30:08.450 align:middle line:84%
But you fix x, and then you're
looking at the sequence.

00:30:08.450 --> 00:30:11.180 align:middle line:84%
And then I claim
that this sequence

00:30:11.180 --> 00:30:14.185 align:middle line:90%
will be a Cauchy sequence.

00:30:14.185 --> 00:30:20.020 align:middle line:84%
And so x is fixed, and so we
have this inequality here.

00:30:20.020 --> 00:30:26.010 align:middle line:84%
And what we need is that when
little n is sufficiently far

00:30:26.010 --> 00:30:31.120 align:middle line:84%
large, then for all k,
k is a positive integer,

00:30:31.120 --> 00:30:33.960 align:middle line:90%
This is further out than in.

00:30:33.960 --> 00:30:35.500 align:middle line:90%
Then for all k--

00:30:35.500 --> 00:30:37.690 align:middle line:84%
and this should be
independent of k--

00:30:37.690 --> 00:30:39.070 align:middle line:90%
this thing here small.

00:30:39.070 --> 00:30:40.080 align:middle line:90%
But this is just--

00:30:40.080 --> 00:30:42.163 align:middle line:84%
STUDENT: Doesn't that get
rid of-- the whole thing

00:30:42.163 --> 00:30:45.420 align:middle line:84%
from the previous step was
now it's not a Tk of x.

00:30:45.420 --> 00:30:52.230 align:middle line:84%
PROFESSOR: Yeah, so since
x is fixed, x is fixed.

00:30:52.230 --> 00:30:53.950 align:middle line:90%
Tx is fixed.

00:30:53.950 --> 00:30:55.275 align:middle line:90%
So this is just a constant.

00:30:55.275 --> 00:31:00.150 align:middle line:90%


00:31:00.150 --> 00:31:01.900 align:middle line:90%
So right.

00:31:01.900 --> 00:31:03.780 align:middle line:90%
So what we have proven is that--

00:31:03.780 --> 00:31:08.560 align:middle line:84%
so we have so we have this
Cauchy complete metric space.

00:31:08.560 --> 00:31:10.740 align:middle line:90%
And we have this sequence.

00:31:10.740 --> 00:31:12.210 align:middle line:90%
X was fixed again.

00:31:12.210 --> 00:31:13.960 align:middle line:90%
That is a Cauchy sequence.

00:31:13.960 --> 00:31:17.330 align:middle line:84%
And so since this metric
space is Cauchy complete,

00:31:17.330 --> 00:31:23.020 align:middle line:84%
this is convergent, and
I can denote the limit.

00:31:23.020 --> 00:31:26.590 align:middle line:84%
So I just called the
limit x infinity.

00:31:26.590 --> 00:31:27.555 align:middle line:90%
So we have this.

00:31:27.555 --> 00:31:30.100 align:middle line:90%


00:31:30.100 --> 00:31:32.141 align:middle line:90%
Now, I want to show that--

00:31:32.141 --> 00:31:34.690 align:middle line:90%


00:31:34.690 --> 00:31:55.684 align:middle line:84%
so the next claim is that x
infinity is a fixed point for T.

00:31:55.684 --> 00:31:58.750 align:middle line:84%
So if I'm looking at
this sequence here,

00:31:58.750 --> 00:32:00.770 align:middle line:90%
suppose I take the sequence.

00:32:00.770 --> 00:32:03.443 align:middle line:84%
And suppose I take
T of this sequence.

00:32:03.443 --> 00:32:08.290 align:middle line:90%


00:32:08.290 --> 00:32:11.890 align:middle line:84%
So if I take T of this
sequence, this here

00:32:11.890 --> 00:32:17.000 align:middle line:84%
is nothing but the next
element in the sequence.

00:32:17.000 --> 00:32:23.660 align:middle line:84%
So this one here will still
converge to x infinity,

00:32:23.660 --> 00:32:27.290 align:middle line:90%
because it's just shifted by 1.

00:32:27.290 --> 00:32:30.845 align:middle line:84%
But then on the other hand,
so now, if you're looking at--

00:32:30.845 --> 00:32:33.620 align:middle line:90%


00:32:33.620 --> 00:32:35.990 align:middle line:90%
so you have that.

00:32:35.990 --> 00:32:41.023 align:middle line:84%
If you're looking at T,
so we want to prove that--

00:32:41.023 --> 00:32:44.060 align:middle line:90%


00:32:44.060 --> 00:32:51.050 align:middle line:84%
so now, if we're looking
at T of x infinity,

00:32:51.050 --> 00:33:05.400 align:middle line:84%
this distance between T of x
infinity and Tn plus 1 of x,

00:33:05.400 --> 00:33:08.945 align:middle line:84%
suppose I'm looking
at this distance here.

00:33:08.945 --> 00:33:13.800 align:middle line:84%
Well, this here I can think
about as the distance between T

00:33:13.800 --> 00:33:20.400 align:middle line:90%
of x infinity and T of Tn of x.

00:33:20.400 --> 00:33:24.010 align:middle line:84%
But here there are now
both of these elements.

00:33:24.010 --> 00:33:26.460 align:middle line:84%
You can think about this
as just some elements.

00:33:26.460 --> 00:33:27.870 align:middle line:90%
Apply T to it.

00:33:27.870 --> 00:33:29.920 align:middle line:90%
Here there's Ts applied to that.

00:33:29.920 --> 00:33:35.490 align:middle line:84%
So this is less than
the distance x infinity

00:33:35.490 --> 00:33:41.400 align:middle line:84%
to Tn as a constant c
less than 1 in front.

00:33:41.400 --> 00:33:49.440 align:middle line:84%
So like this by the
contracting map property.

00:33:49.440 --> 00:33:53.910 align:middle line:84%
But now you see that
as n goes to infinity,

00:33:53.910 --> 00:33:57.280 align:middle line:90%
this thing here goes to zero.

00:33:57.280 --> 00:34:03.300 align:middle line:84%
So this means that this thing
here converges to this point.

00:34:03.300 --> 00:34:05.613 align:middle line:90%
So you have that--

00:34:05.613 --> 00:34:09.000 align:middle line:90%


00:34:09.000 --> 00:34:10.210 align:middle line:90%
so you have that--

00:34:10.210 --> 00:34:20.920 align:middle line:90%


00:34:20.920 --> 00:34:25.100 align:middle line:84%
you have that if
you're looking at--

00:34:25.100 --> 00:34:28.100 align:middle line:90%
if you're looking at--

00:34:28.100 --> 00:34:33.850 align:middle line:90%
again, as n go to--

00:34:33.850 --> 00:34:46.120 align:middle line:84%
as n goes to infinity, since Tn
of x converges to x infinity,

00:34:46.120 --> 00:34:48.310 align:middle line:84%
then we have that
the distance-- this

00:34:48.310 --> 00:34:55.780 align:middle line:84%
is the equivalent to that the
distance here goes to zero.

00:34:55.780 --> 00:35:02.320 align:middle line:84%
And then by this inequality,
it means that the distance here

00:35:02.320 --> 00:35:12.960 align:middle line:84%
Tx infinity and Tn plus
1 of x goes to zero.

00:35:12.960 --> 00:35:16.320 align:middle line:84%
And so this means that this
is just some fixed point.

00:35:16.320 --> 00:35:18.240 align:middle line:84%
It means that this
sequence here--

00:35:18.240 --> 00:35:22.820 align:middle line:84%
so this implies that
this sequence here

00:35:22.820 --> 00:35:27.980 align:middle line:90%
converts to T of x infinity.

00:35:27.980 --> 00:35:30.590 align:middle line:84%
But on the other
hand, we already

00:35:30.590 --> 00:35:36.450 align:middle line:84%
observed that this sequence
also converges to x infinity.

00:35:36.450 --> 00:35:40.830 align:middle line:90%


00:35:40.830 --> 00:35:43.950 align:middle line:84%
So it converges to this
and it converges to that,

00:35:43.950 --> 00:35:47.220 align:middle line:84%
but it can only have one limit,
so those two things are equal.

00:35:47.220 --> 00:35:52.970 align:middle line:84%
So you conclude that x infinity
is equal to T of x infinity.

00:35:52.970 --> 00:35:57.100 align:middle line:84%
And so x infinity
is a fixed point.

00:35:57.100 --> 00:36:01.460 align:middle line:90%


00:36:01.460 --> 00:36:04.040 align:middle line:84%
So this proves
this theorem right.

00:36:04.040 --> 00:36:09.410 align:middle line:84%
And again, we already knew
that the limit was unique.

00:36:09.410 --> 00:36:13.270 align:middle line:90%


00:36:13.270 --> 00:36:20.460 align:middle line:84%
So now, how is this related to
the Picard-Lindelof theorem?

00:36:20.460 --> 00:36:23.290 align:middle line:84%
And so it's related
in the following way.

00:36:23.290 --> 00:36:25.290 align:middle line:84%
And again, this
is something that

00:36:25.290 --> 00:36:28.226 align:middle line:84%
has been used to solve a lot
of differential equations.

00:36:28.226 --> 00:36:36.060 align:middle line:90%


00:36:36.060 --> 00:36:41.580 align:middle line:84%
And so we need to
define a space in a map.

00:36:41.580 --> 00:36:45.910 align:middle line:84%
The spaces initially, but
we have to restrict it.

00:36:45.910 --> 00:36:54.780 align:middle line:84%
But initially, let's think
about some continuous functions

00:36:54.780 --> 00:36:57.480 align:middle line:90%
on some interval.

00:36:57.480 --> 00:36:59.920 align:middle line:84%
Let's start with just
continuous function.

00:36:59.920 --> 00:37:02.130 align:middle line:84%
But it's not quite
going to be the space.

00:37:02.130 --> 00:37:04.480 align:middle line:84%
I will have to
look at a smaller--

00:37:04.480 --> 00:37:05.360 align:middle line:90%
Yeah.

00:37:05.360 --> 00:37:06.110 align:middle line:90%
STUDENT: Question.

00:37:06.110 --> 00:37:09.040 align:middle line:84%
Why is it that you
didn't need to know

00:37:09.040 --> 00:37:13.453 align:middle line:84%
the need before to a
good starting point?

00:37:13.453 --> 00:37:14.870 align:middle line:84%
PROFESSOR: That's
a good question.

00:37:14.870 --> 00:37:16.220 align:middle line:90%
So that's right.

00:37:16.220 --> 00:37:19.400 align:middle line:84%
So this comes with
this Newton method.

00:37:19.400 --> 00:37:22.450 align:middle line:90%
So we used the--

00:37:22.450 --> 00:37:24.940 align:middle line:84%
so we used this
contracting mapping

00:37:24.940 --> 00:37:30.632 align:middle line:84%
for R in the Newton
method to find a zero.

00:37:30.632 --> 00:37:34.060 align:middle line:84%
And to some extent,
there was a great idea.

00:37:34.060 --> 00:37:37.480 align:middle line:84%
Newton was a pretty famous
guy for a good reason.

00:37:37.480 --> 00:37:40.640 align:middle line:84%
But in a way, this is
more ingenious, I think,

00:37:40.640 --> 00:37:42.440 align:middle line:90%
because it's like metric space.

00:37:42.440 --> 00:37:45.602 align:middle line:84%
What the hell does this have to
do with differential equation?

00:37:45.602 --> 00:37:49.550 align:middle line:84%
And the reason why in the other
one, we had to restrict it

00:37:49.550 --> 00:37:54.110 align:middle line:84%
was that the map we defined
wasn't contracting everywhere.

00:37:54.110 --> 00:37:58.030 align:middle line:84%
It needed things to be
pretty close initially

00:37:58.030 --> 00:38:02.720 align:middle line:84%
for there to exist a c
strictly less than 1.

00:38:02.720 --> 00:38:04.620 align:middle line:90%
So that's where it came in.

00:38:04.620 --> 00:38:08.130 align:middle line:90%
It wasn't really because if--

00:38:08.130 --> 00:38:08.630 align:middle line:90%
yeah.

00:38:08.630 --> 00:38:13.550 align:middle line:90%


00:38:13.550 --> 00:38:16.610 align:middle line:84%
So now, again, so we
need to relate this.

00:38:16.610 --> 00:38:19.110 align:middle line:84%
That seems to have nothing to
do with differential equation.

00:38:19.110 --> 00:38:21.720 align:middle line:84%
We need to relate it to
the differential equation.

00:38:21.720 --> 00:38:25.280 align:middle line:84%
So again, what is the
space, the metric space

00:38:25.280 --> 00:38:26.880 align:middle line:90%
that we're going to look at?

00:38:26.880 --> 00:38:29.040 align:middle line:84%
And again, it's
not exactly this,

00:38:29.040 --> 00:38:30.750 align:middle line:90%
but it's just a subset of it.

00:38:30.750 --> 00:38:37.130 align:middle line:84%
So it's this space, and
with the usual metric

00:38:37.130 --> 00:38:38.400 align:middle line:90%
that we have talked about.

00:38:38.400 --> 00:38:45.710 align:middle line:84%
That is going to be
the metric space.

00:38:45.710 --> 00:38:49.670 align:middle line:90%
Now, what is the map T?

00:38:49.670 --> 00:38:55.280 align:middle line:84%
And so the map T
is-- so T here is

00:38:55.280 --> 00:39:03.071 align:middle line:84%
going to be a map from
continuous functions

00:39:03.071 --> 00:39:05.426 align:middle line:84%
into the space of
continuous functions.

00:39:05.426 --> 00:39:08.700 align:middle line:90%


00:39:08.700 --> 00:39:15.930 align:middle line:84%
And is going to be
defined as follows.

00:39:15.930 --> 00:39:18.340 align:middle line:84%
And I'll come to
this in a second.

00:39:18.340 --> 00:39:21.730 align:middle line:90%
So T of x, T of y.

00:39:21.730 --> 00:39:25.140 align:middle line:84%
So think about y as being
a continuous function

00:39:25.140 --> 00:39:27.180 align:middle line:90%
on this interval.

00:39:27.180 --> 00:39:35.490 align:middle line:84%
And T of y is now equal to a
plus, and then the integral,

00:39:35.490 --> 00:39:40.420 align:middle line:90%
and then integral.

00:39:40.420 --> 00:39:46.000 align:middle line:84%
So this is a-- so T of y,
y is of an element here.

00:39:46.000 --> 00:39:48.940 align:middle line:84%
This one here is also supposed
to be an element here,

00:39:48.940 --> 00:39:50.730 align:middle line:90%
so this is a function.

00:39:50.730 --> 00:39:54.780 align:middle line:84%
So we want to find out
what the value is at x.

00:39:54.780 --> 00:39:59.820 align:middle line:84%
And this a, this constant
a plus the integral from

00:39:59.820 --> 00:40:12.970 align:middle line:84%
zero to x, and then of
f of y, plus g of x.

00:40:12.970 --> 00:40:18.250 align:middle line:84%
And this here is a function
of x, also, so like this.

00:40:18.250 --> 00:40:23.020 align:middle line:84%
And I shouldn't write x
because I use now x up here.

00:40:23.020 --> 00:40:26.650 align:middle line:90%
So I write it like that. d of x.

00:40:26.650 --> 00:40:30.370 align:middle line:84%
That's how the map is
going to be defined.

00:40:30.370 --> 00:40:33.020 align:middle line:90%
So again, if you take--

00:40:33.020 --> 00:40:38.800 align:middle line:84%
so y here, so y is going--
so y is a continuous function

00:40:38.800 --> 00:40:41.320 align:middle line:90%
on this interval.

00:40:41.320 --> 00:40:43.780 align:middle line:84%
And I will have to
restrict it, and this

00:40:43.780 --> 00:40:47.780 align:middle line:84%
is exactly when you're asking
what in Newton's method,

00:40:47.780 --> 00:40:51.380 align:middle line:84%
why did we have to
pick this good choice.

00:40:51.380 --> 00:40:56.410 align:middle line:84%
It's exactly like this that
this map is not contracting

00:40:56.410 --> 00:40:57.770 align:middle line:90%
on this whole space.

00:40:57.770 --> 00:41:02.020 align:middle line:84%
So we have to-- in a way, we
have to do the same stuff.

00:41:02.020 --> 00:41:04.360 align:middle line:84%
We have to make a
good choice first.

00:41:04.360 --> 00:41:06.610 align:middle line:84%
And so that's why we have
to restrict the space.

00:41:06.610 --> 00:41:09.990 align:middle line:90%
And it actually is--

00:41:09.990 --> 00:41:13.210 align:middle line:84%
part of the beauty is that
it's pretty much optimal,

00:41:13.210 --> 00:41:16.920 align:middle line:84%
this stuff, this sort
of general principle.

00:41:16.920 --> 00:41:18.600 align:middle line:90%
We can come back to that.

00:41:18.600 --> 00:41:22.920 align:middle line:84%
So this is the map T.
And so the first thing

00:41:22.920 --> 00:41:27.600 align:middle line:90%
that you observe is that T--

00:41:27.600 --> 00:41:32.680 align:middle line:84%
so this gives you
this function here.

00:41:32.680 --> 00:41:39.400 align:middle line:84%
Remember that so if y is
continuous, g is continuous.

00:41:39.400 --> 00:41:42.190 align:middle line:84%
Well, if y is continuous
f is continuous.

00:41:42.190 --> 00:41:43.990 align:middle line:90%
Everything here is continuous.

00:41:43.990 --> 00:41:47.290 align:middle line:84%
And so this means that by the
fundamental theorem of calculus,

00:41:47.290 --> 00:41:52.890 align:middle line:84%
this function here is
actually even differentiable.

00:41:52.890 --> 00:41:55.930 align:middle line:84%
And the derivative of
this is just a constant.

00:41:55.930 --> 00:41:59.260 align:middle line:84%
So this function here
is differentiable,

00:41:59.260 --> 00:42:00.710 align:middle line:90%
let alone continuous.

00:42:00.710 --> 00:42:06.940 align:middle line:84%
So it's definitely in the space
and the derivative of this map.

00:42:06.940 --> 00:42:09.440 align:middle line:84%
By the fundamental
theorem of calculus--

00:42:09.440 --> 00:42:21.850 align:middle line:90%


00:42:21.850 --> 00:42:23.780 align:middle line:84%
so by the fundamental
theorem of calculus,

00:42:23.780 --> 00:42:26.660 align:middle line:84%
the derivative is just
what is inside here.

00:42:26.660 --> 00:42:36.280 align:middle line:84%
So this is just f
of y plus g of x.

00:42:36.280 --> 00:42:39.445 align:middle line:84%
And if you want to write x in,
then it should be like this.

00:42:39.445 --> 00:42:47.660 align:middle line:90%


00:42:47.660 --> 00:42:50.330 align:middle line:84%
And then one more
thing you observe,

00:42:50.330 --> 00:42:55.810 align:middle line:84%
which is also immediate, that if
you take a continuous function

00:42:55.810 --> 00:42:58.800 align:middle line:84%
like this, and now
you evaluate this,

00:42:58.800 --> 00:43:01.490 align:middle line:90%
now you evaluate this at zero.

00:43:01.490 --> 00:43:05.060 align:middle line:84%
But if x is zero
within this integral,

00:43:05.060 --> 00:43:07.020 align:middle line:90%
it's over just a point.

00:43:07.020 --> 00:43:08.400 align:middle line:90%
So this here is zero.

00:43:08.400 --> 00:43:10.760 align:middle line:84%
So this means that
the value here is a.

00:43:10.760 --> 00:43:15.615 align:middle line:90%


00:43:15.615 --> 00:43:20.553 align:middle line:84%
And so now, the next thing
you observe is that--

00:43:20.553 --> 00:43:31.850 align:middle line:90%


00:43:31.850 --> 00:43:40.870 align:middle line:84%
so the next thing we observe is
that if you have a fixed point.

00:43:40.870 --> 00:43:43.873 align:middle line:90%


00:43:43.873 --> 00:43:45.290 align:middle line:84%
I think this is
another nice thing

00:43:45.290 --> 00:43:50.840 align:middle line:84%
is that the way it's set
up is that you just need

00:43:50.840 --> 00:43:54.270 align:middle line:90%
to use continuous functions.

00:43:54.270 --> 00:43:57.250 align:middle line:84%
But of course, if you
want a solution to this,

00:43:57.250 --> 00:44:00.400 align:middle line:84%
it means that the function
must have a derivative.

00:44:00.400 --> 00:44:00.900 align:middle line:90%
Yeah.

00:44:00.900 --> 00:44:04.020 align:middle line:84%
STUDENT: So how do you
know that [INAUDIBLE]?

00:44:04.020 --> 00:44:06.250 align:middle line:84%
PROFESSOR: Yeah we
don't know that yet.

00:44:06.250 --> 00:44:07.950 align:middle line:90%
That's a major point, actually.

00:44:07.950 --> 00:44:10.270 align:middle line:84%
And again, just like
in Newton's methods,

00:44:10.270 --> 00:44:12.850 align:middle line:84%
we have to restrict where
we're looking at it.

00:44:12.850 --> 00:44:14.200 align:middle line:90%
Yeah.

00:44:14.200 --> 00:44:16.410 align:middle line:84%
But the first thing
I want to observe

00:44:16.410 --> 00:44:31.200 align:middle line:84%
is that if y is a fixed point,
well, then T of y is equal to y.

00:44:31.200 --> 00:44:33.510 align:middle line:90%
And so what does this mean?

00:44:33.510 --> 00:44:36.100 align:middle line:90%
Well, the derivative.

00:44:36.100 --> 00:44:46.350 align:middle line:84%
So it means that if this is the
case, then we have that T of y

00:44:46.350 --> 00:44:47.710 align:middle line:90%
is of this form.

00:44:47.710 --> 00:44:51.220 align:middle line:84%
So it has a derivative, and
that derivative is this.

00:44:51.220 --> 00:44:54.590 align:middle line:84%
So this means that y would have
it, because y is equal to this.

00:44:54.590 --> 00:44:59.625 align:middle line:84%
So y is differentiable, and the
derivative is equal to this.

00:44:59.625 --> 00:45:02.890 align:middle line:90%


00:45:02.890 --> 00:45:04.930 align:middle line:90%
And we always have--

00:45:04.930 --> 00:45:06.850 align:middle line:84%
whether it's a
fixed point or not,

00:45:06.850 --> 00:45:14.095 align:middle line:84%
we always have that
Ty of zero is a.

00:45:14.095 --> 00:45:18.590 align:middle line:84%
And since it is a fixed
point, this is also this.

00:45:18.590 --> 00:45:22.210 align:middle line:84%
So you see that if it
is a fixed point, then

00:45:22.210 --> 00:45:24.435 align:middle line:84%
it is a solution to the
differential equation.

00:45:24.435 --> 00:45:27.490 align:middle line:90%


00:45:27.490 --> 00:45:31.880 align:middle line:90%
Now, then the point comes in.

00:45:31.880 --> 00:45:36.430 align:middle line:84%
The key point comes
in with proving

00:45:36.430 --> 00:45:38.340 align:middle line:90%
that the map is contracting.

00:45:38.340 --> 00:46:04.635 align:middle line:90%


00:46:04.635 --> 00:46:10.070 align:middle line:84%
And so now, so we
need to prove--

00:46:10.070 --> 00:46:19.090 align:middle line:84%
need to show that T
is a contracting map.

00:46:19.090 --> 00:46:29.480 align:middle line:90%


00:46:29.480 --> 00:46:34.700 align:middle line:90%
So set.

00:46:34.700 --> 00:46:37.160 align:middle line:84%
I have to define a
number of things,

00:46:37.160 --> 00:46:39.980 align:middle line:90%
because again, I have to--

00:46:39.980 --> 00:46:42.830 align:middle line:84%
T is not going to be
contracting on the space

00:46:42.830 --> 00:46:44.160 align:middle line:90%
of continuous functions.

00:46:44.160 --> 00:46:47.880 align:middle line:84%
So I have to look at some
subset of continuous function.

00:46:47.880 --> 00:46:50.580 align:middle line:84%
And the right subset
is just a ball.

00:46:50.580 --> 00:46:52.270 align:middle line:90%
It's its a close ball.

00:46:52.270 --> 00:46:56.100 align:middle line:90%
So it's going to be--

00:46:56.100 --> 00:47:00.570 align:middle line:84%
so we're going to-- maybe I'll
just say first that we're going

00:47:00.570 --> 00:47:07.360 align:middle line:84%
to restrict T. So T here
will be restricted now to--

00:47:07.360 --> 00:47:14.910 align:middle line:84%
we will think about it as a
map on some ball into itself.

00:47:14.910 --> 00:47:18.120 align:middle line:84%
But it's not at all
clear that this map

00:47:18.120 --> 00:47:21.282 align:middle line:90%
takes a ball into itself.

00:47:21.282 --> 00:47:23.350 align:middle line:90%
And what do I mean by ball?

00:47:23.350 --> 00:47:25.300 align:middle line:90%
So I have this bar up here.

00:47:25.300 --> 00:47:32.220 align:middle line:84%
So I just means
that this thing here

00:47:32.220 --> 00:47:36.336 align:middle line:84%
is going to be the function
y that is continuous.

00:47:36.336 --> 00:47:40.230 align:middle line:90%


00:47:40.230 --> 00:47:43.630 align:middle line:84%
And then it's not quite
going to be this either.

00:47:43.630 --> 00:47:45.480 align:middle line:90%
I have to restrict.

00:47:45.480 --> 00:47:47.940 align:middle line:84%
But I'll get to
this in a second.

00:47:47.940 --> 00:47:50.200 align:middle line:84%
So at the moment, you
can think about it

00:47:50.200 --> 00:47:53.300 align:middle line:84%
as being continuous
function on the interval,

00:47:53.300 --> 00:48:00.830 align:middle line:84%
so that the norm of y at
each point x is less than

00:48:00.830 --> 00:48:04.930 align:middle line:84%
or equal to R. And
this bar here refers

00:48:04.930 --> 00:48:09.890 align:middle line:90%
to that equal is also allowed.

00:48:09.890 --> 00:48:14.290 align:middle line:84%
Now, this here is
really like the ball.

00:48:14.290 --> 00:48:16.070 align:middle line:90%
These are functions.

00:48:16.070 --> 00:48:18.670 align:middle line:84%
If you're thinking
about the function

00:48:18.670 --> 00:48:23.570 align:middle line:84%
in the space of continuous
function that is constant zero,

00:48:23.570 --> 00:48:27.310 align:middle line:84%
then these are the functions
whose distance-- this

00:48:27.310 --> 00:48:32.350 align:middle line:84%
is the same as the space
of continuous functions

00:48:32.350 --> 00:48:37.780 align:middle line:84%
whose distance to the constant
function zero is, at most,

00:48:37.780 --> 00:48:43.600 align:middle line:90%
R. This is the zero function.

00:48:43.600 --> 00:48:45.350 align:middle line:84%
It's less than or
equal to R. Sorry.

00:48:45.350 --> 00:48:47.142 align:middle line:84%
This is getting a little
smaller over here.

00:48:47.142 --> 00:48:53.930 align:middle line:90%


00:48:53.930 --> 00:48:56.510 align:middle line:90%
And again, it's going to be--

00:48:56.510 --> 00:48:59.810 align:middle line:84%
I will have to restrict
the interval here

00:48:59.810 --> 00:49:02.670 align:middle line:84%
to make sure that the
map is contracting.

00:49:02.670 --> 00:49:05.825 align:middle line:90%


00:49:05.825 --> 00:49:09.440 align:middle line:84%
But first, I want to
define this radius here.

00:49:09.440 --> 00:49:12.680 align:middle line:90%
And so the radius is--

00:49:12.680 --> 00:49:14.990 align:middle line:90%
I'm setting R here equal--

00:49:14.990 --> 00:49:16.550 align:middle line:90%
a was just a constant.

00:49:16.550 --> 00:49:20.005 align:middle line:84%
I take the absolute value
of a and I add 2 to it.

00:49:20.005 --> 00:49:22.580 align:middle line:90%


00:49:22.580 --> 00:49:27.650 align:middle line:84%
Then I define two other areas,
and there's no way around it.

00:49:27.650 --> 00:49:29.510 align:middle line:90%
You have to define.

00:49:29.510 --> 00:49:32.995 align:middle line:84%
We will require to define
several constants first.

00:49:32.995 --> 00:49:35.690 align:middle line:90%


00:49:35.690 --> 00:49:40.490 align:middle line:84%
L1, capital L1, is going
to be another constant.

00:49:40.490 --> 00:49:43.250 align:middle line:90%
It's going to be the maximum.

00:49:43.250 --> 00:49:52.560 align:middle line:84%
And then you take off over z,
where z here is less than R,

00:49:52.560 --> 00:49:57.815 align:middle line:84%
and then you take
the value like this.

00:49:57.815 --> 00:50:00.404 align:middle line:90%


00:50:00.404 --> 00:50:03.040 align:middle line:90%
Remember, f is continuous.

00:50:03.040 --> 00:50:08.470 align:middle line:84%
So looking at where the
norm of x is less than

00:50:08.470 --> 00:50:13.560 align:middle line:84%
or equal to some constant,
then this, the maximum

00:50:13.560 --> 00:50:15.120 align:middle line:90%
is achieved on this.

00:50:15.120 --> 00:50:18.630 align:middle line:84%
So this is just
some real number,

00:50:18.630 --> 00:50:22.980 align:middle line:84%
positive real,
non-negative real number.

00:50:22.980 --> 00:50:32.760 align:middle line:84%
And then I define L2 to be
the maximum of where I--

00:50:32.760 --> 00:50:38.130 align:middle line:84%
of maximum on this unit ball
here, and where norm of x

00:50:38.130 --> 00:50:43.340 align:middle line:84%
is less than 1 of
g of x, like that.

00:50:43.340 --> 00:50:48.095 align:middle line:90%


00:50:48.095 --> 00:50:53.320 align:middle line:90%
And now, what I want to do is--

00:50:53.320 --> 00:50:55.990 align:middle line:90%
so the first step is--

00:50:55.990 --> 00:50:58.250 align:middle line:84%
so the first step
is the following.

00:50:58.250 --> 00:51:09.580 align:middle line:90%


00:51:09.580 --> 00:51:19.660 align:middle line:84%
So first step in the proof
is to prove the following,

00:51:19.660 --> 00:51:32.560 align:middle line:90%
that there exists delta zero.

00:51:32.560 --> 00:51:36.760 align:middle line:84%
This is not the delta that
I will use eventually.

00:51:36.760 --> 00:51:38.980 align:middle line:84%
I would have to
restrict it further.

00:51:38.980 --> 00:51:44.670 align:middle line:84%
There exists delta zero, so that
if you're looking at this space,

00:51:44.670 --> 00:51:50.360 align:middle line:84%
if y here is in the space
of continuous functions

00:51:50.360 --> 00:52:00.770 align:middle line:84%
on this interval
here, then T of y--

00:52:00.770 --> 00:52:01.610 align:middle line:90%
sorry.

00:52:01.610 --> 00:52:08.365 align:middle line:84%
If y is in this here, and
y is in the unit ball--

00:52:08.365 --> 00:52:11.030 align:middle line:90%


00:52:11.030 --> 00:52:18.240 align:middle line:84%
not in the unit ball, then y
here is less or equal to R.

00:52:18.240 --> 00:52:20.850 align:middle line:84%
So it's a continuous
function on this interval,

00:52:20.850 --> 00:52:23.220 align:middle line:84%
and the norm is
less or equal to R.

00:52:23.220 --> 00:52:26.690 align:middle line:84%
So this means that so this is,
of course, the same as saying

00:52:26.690 --> 00:52:31.550 align:middle line:84%
that y is in this
ball here when I'm now

00:52:31.550 --> 00:52:34.290 align:middle line:90%
thinking about this as a space.

00:52:34.290 --> 00:52:37.310 align:middle line:84%
But you can forget
about that if you want.

00:52:37.310 --> 00:52:38.040 align:middle line:90%
It's the same.

00:52:38.040 --> 00:52:42.410 align:middle line:90%


00:52:42.410 --> 00:52:46.220 align:middle line:84%
And I want to show that T
of y is in the same space.

00:52:46.220 --> 00:52:51.130 align:middle line:90%
So T of y.

00:52:51.130 --> 00:52:53.300 align:middle line:90%
So I want to show--

00:52:53.300 --> 00:53:07.960 align:middle line:84%
so I want to show that
T of y at each x here,

00:53:07.960 --> 00:53:10.780 align:middle line:90%
the norm is less or equal to 1.

00:53:10.780 --> 00:53:16.450 align:middle line:84%
Then if I have that, I already
know that this function T of y

00:53:16.450 --> 00:53:17.420 align:middle line:90%
is continuous.

00:53:17.420 --> 00:53:20.470 align:middle line:84%
It's actually even
differentiable.

00:53:20.470 --> 00:53:23.530 align:middle line:84%
But it's, in
particular, continuous.

00:53:23.530 --> 00:53:27.370 align:middle line:84%
And if I have this, then
I know that this space

00:53:27.370 --> 00:53:28.470 align:middle line:90%
is taken into itself.

00:53:28.470 --> 00:53:33.580 align:middle line:90%


00:53:33.580 --> 00:53:37.150 align:middle line:90%
So now, how do I do that?

00:53:37.150 --> 00:53:42.500 align:middle line:84%
So that's where I need to
restrict the interval that I'm

00:53:42.500 --> 00:53:43.500 align:middle line:90%
looking on.

00:53:43.500 --> 00:53:47.130 align:middle line:84%
And again, we'll
come back to it,

00:53:47.130 --> 00:53:51.180 align:middle line:84%
but there's a good reason
that we have to restrict.

00:53:51.180 --> 00:53:53.290 align:middle line:84%
Otherwise, it couldn't
possibly be true.

00:53:53.290 --> 00:53:56.355 align:middle line:90%


00:53:56.355 --> 00:53:56.855 align:middle line:90%
Yeah.

00:53:56.855 --> 00:53:58.700 align:middle line:84%
STUDENT: To be
contracting, do we need

00:53:58.700 --> 00:54:00.710 align:middle line:90%
it to be strictly less than 1?

00:54:00.710 --> 00:54:03.020 align:middle line:84%
PROFESSOR: So
remember, contracting

00:54:03.020 --> 00:54:09.200 align:middle line:84%
means that there exists a
constant c strictly less than 1.

00:54:09.200 --> 00:54:12.300 align:middle line:84%
This here has nothing to
do with the constant c.

00:54:12.300 --> 00:54:17.460 align:middle line:84%
This here is just the space that
we're looking at the map on.

00:54:17.460 --> 00:54:21.120 align:middle line:90%
And the reason why I make here--

00:54:21.120 --> 00:54:24.180 align:middle line:84%
so again, so this has
nothing to do with that c.

00:54:24.180 --> 00:54:27.380 align:middle line:84%
But the reason why I want
this less than or equal to

00:54:27.380 --> 00:54:33.850 align:middle line:84%
is that I want to have that
the space is Cauchy complete.

00:54:33.850 --> 00:54:34.350 align:middle line:90%
Sorry.

00:54:34.350 --> 00:54:36.930 align:middle line:84%
So let me just try
to make that clear.

00:54:36.930 --> 00:54:43.270 align:middle line:84%
So to get a fixed point
for a contracting map,

00:54:43.270 --> 00:54:46.470 align:middle line:84%
you need a space that
is Cauchy complete

00:54:46.470 --> 00:54:49.150 align:middle line:84%
when we prove this
for the metric space.

00:54:49.150 --> 00:54:51.330 align:middle line:90%
We have a good candidate.

00:54:51.330 --> 00:54:54.930 align:middle line:84%
We have the candidate
of continuous functions

00:54:54.930 --> 00:54:57.340 align:middle line:84%
on some closed
interval like this.

00:54:57.340 --> 00:55:01.440 align:middle line:84%
This is Cauchy complete
with the usual metric.

00:55:01.440 --> 00:55:03.600 align:middle line:84%
But I'm not going to
look at that space

00:55:03.600 --> 00:55:07.000 align:middle line:84%
because my map is not actually
contracting on the space.

00:55:07.000 --> 00:55:09.520 align:middle line:90%
It's contracting on a subset.

00:55:09.520 --> 00:55:11.890 align:middle line:90%
And so I need that subset.

00:55:11.890 --> 00:55:16.090 align:middle line:84%
So in the end, I'm sort
of not working on this,

00:55:16.090 --> 00:55:18.622 align:middle line:90%
but I'm working on a subset.

00:55:18.622 --> 00:55:22.390 align:middle line:84%
And I need that subset
to be Cauchy complete.

00:55:22.390 --> 00:55:25.440 align:middle line:84%
So basically, what I
have is that this here

00:55:25.440 --> 00:55:28.570 align:middle line:84%
is the giant metric
space I start with.

00:55:28.570 --> 00:55:32.160 align:middle line:84%
Then I'm looking
at a ball in this.

00:55:32.160 --> 00:55:36.270 align:middle line:84%
And if I take the
closed ball and it

00:55:36.270 --> 00:55:37.960 align:middle line:84%
happened to be at
the origin, but it

00:55:37.960 --> 00:55:40.120 align:middle line:90%
could be just at any point.

00:55:40.120 --> 00:55:43.300 align:middle line:84%
If you take a metric space
and you're checking something

00:55:43.300 --> 00:55:47.060 align:middle line:84%
like this, if the metric
space is Cauchy complete,

00:55:47.060 --> 00:55:49.870 align:middle line:84%
then this subset is
also Cauchy complete.

00:55:49.870 --> 00:55:55.820 align:middle line:84%
But this require I have
less than or equal to--

00:55:55.820 --> 00:55:58.360 align:middle line:84%
because I also could kind
of converge to something

00:55:58.360 --> 00:56:01.904 align:middle line:90%
where you got equality.

00:56:01.904 --> 00:56:06.855 align:middle line:84%
So that was why I
do it like that.

00:56:06.855 --> 00:56:09.800 align:middle line:90%
So let's see.

00:56:09.800 --> 00:56:12.760 align:middle line:90%
So we are trying.

00:56:12.760 --> 00:56:18.430 align:middle line:84%
We have already defined
this radius, capital R.

00:56:18.430 --> 00:56:23.650 align:middle line:84%
And then we have these
two constants, L1 and L2.

00:56:23.650 --> 00:56:28.390 align:middle line:84%
And what I need to prove is--
the first step here is to prove

00:56:28.390 --> 00:56:29.620 align:middle line:90%
that if--

00:56:29.620 --> 00:56:31.670 align:middle line:90%
I'm going to look again.

00:56:31.670 --> 00:56:35.870 align:middle line:84%
So the first step is
that I need to restrict.

00:56:35.870 --> 00:56:38.280 align:middle line:90%
So I need to restrict.

00:56:38.280 --> 00:56:44.870 align:middle line:84%
So I'm going to look at a
subset of these spaces of--

00:56:44.870 --> 00:56:47.970 align:middle line:84%
this is a subset of the
continuous functions.

00:56:47.970 --> 00:56:51.410 align:middle line:84%
And I need to prove
that if y is in here,

00:56:51.410 --> 00:56:54.070 align:middle line:84%
then the image is
in the same space.

00:56:54.070 --> 00:56:58.590 align:middle line:90%


00:56:58.590 --> 00:57:03.740 align:middle line:84%
And so this is the statement
that if y is continuous,

00:57:03.740 --> 00:57:09.750 align:middle line:84%
the norm of this function
is less than or equal to R.

00:57:09.750 --> 00:57:14.840 align:middle line:84%
So at each point, each x,
the absolute value of y of x

00:57:14.840 --> 00:57:18.170 align:middle line:84%
is less or equal to R.
Then you have the same

00:57:18.170 --> 00:57:20.010 align:middle line:90%
for the image under T.

00:57:20.010 --> 00:57:23.960 align:middle line:84%
We already know, again, that
the image under the T of y

00:57:23.960 --> 00:57:25.400 align:middle line:90%
is continuous.

00:57:25.400 --> 00:57:29.762 align:middle line:90%


00:57:29.762 --> 00:57:36.840 align:middle line:84%
And so what I can do is I
can restrict my interval.

00:57:36.840 --> 00:57:42.880 align:middle line:84%
So I will restrict the
interval as follows.

00:57:42.880 --> 00:57:54.990 align:middle line:84%
So I'm going to pick delta
zero to be the minimum of 1

00:57:54.990 --> 00:57:57.930 align:middle line:90%
over L plus 1.

00:57:57.930 --> 00:57:59.650 align:middle line:90%
L is non-negative.

00:57:59.650 --> 00:58:01.330 align:middle line:90%
In principle, it could be zero.

00:58:01.330 --> 00:58:04.890 align:middle line:84%
I don't want to worry about
that, so I just add 1.

00:58:04.890 --> 00:58:09.540 align:middle line:84%
And L2 could also be zero,
although it is pretty unlikely

00:58:09.540 --> 00:58:10.630 align:middle line:90%
that any of them are zero.

00:58:10.630 --> 00:58:12.900 align:middle line:84%
But just to be safe,
I'm just adding

00:58:12.900 --> 00:58:16.050 align:middle line:90%
so I don't divide by zero.

00:58:16.050 --> 00:58:17.350 align:middle line:90%
So that's why.

00:58:17.350 --> 00:58:21.580 align:middle line:84%
And the first
thing is that I'm--

00:58:21.580 --> 00:58:25.300 align:middle line:84%
and then I'm going to look
at the interval from this.

00:58:25.300 --> 00:58:27.550 align:middle line:84%
And this is not
going to be my final.

00:58:27.550 --> 00:58:30.570 align:middle line:84%
I will have to do some
further restriction.

00:58:30.570 --> 00:58:34.240 align:middle line:84%
But I'm going to look at
this interval initially.

00:58:34.240 --> 00:58:37.540 align:middle line:84%
And the 1 here, it
just comes in that I

00:58:37.540 --> 00:58:42.340 align:middle line:84%
want this here to be a
subset of this unit interval.

00:58:42.340 --> 00:58:50.104 align:middle line:90%


00:58:50.104 --> 00:58:52.640 align:middle line:90%
So now, let's try.

00:58:52.640 --> 00:58:54.435 align:middle line:84%
So now we are in
good shape here.

00:58:54.435 --> 00:59:04.240 align:middle line:90%


00:59:04.240 --> 00:59:06.400 align:middle line:90%
So now, let's look at Ty.

00:59:06.400 --> 00:59:09.790 align:middle line:90%


00:59:09.790 --> 00:59:13.270 align:middle line:84%
And we need to estimate
this at each x.

00:59:13.270 --> 00:59:19.750 align:middle line:84%
And we want to say that the
norm is less than capital--

00:59:19.750 --> 00:59:21.680 align:middle line:90%
less or equal to capital R.

00:59:21.680 --> 00:59:24.160 align:middle line:84%
Well, let's just
look at what this is.

00:59:24.160 --> 00:59:28.090 align:middle line:84%
This thing here is
equal to this function.

00:59:28.090 --> 00:59:32.810 align:middle line:84%
T of y is defined to be a
plus the integral from zero

00:59:32.810 --> 00:59:49.640 align:middle line:84%
to x of f of y of
s, plus g of s, ds.

00:59:49.640 --> 00:59:53.450 align:middle line:84%
And then I have to have an
absolute value like that.

00:59:53.450 --> 00:59:56.570 align:middle line:84%
And now I can just use the
triangle inequality, of course,

00:59:56.570 --> 00:59:57.830 align:middle line:90%
trivially.

00:59:57.830 --> 01:00:01.700 align:middle line:84%
I get absolute value of
this, and then plus, and then

01:00:01.700 --> 01:00:05.215 align:middle line:90%
the integral here, like that.

01:00:05.215 --> 01:00:09.330 align:middle line:90%


01:00:09.330 --> 01:00:09.830 align:middle line:90%
Oops.

01:00:09.830 --> 01:00:15.650 align:middle line:90%


01:00:15.650 --> 01:00:20.750 align:middle line:84%
And then I can just take
this absolute value in under.

01:00:20.750 --> 01:00:27.990 align:middle line:84%
So I get less than or equal to
a plus, and then the integral,

01:00:27.990 --> 01:00:33.780 align:middle line:84%
and then the absolute
value of f of y of s.

01:00:33.780 --> 01:00:37.740 align:middle line:84%
And here I can also
take the absolute value

01:00:37.740 --> 01:00:40.930 align:middle line:84%
using the triangle inequality
on each individually.

01:00:40.930 --> 01:00:45.240 align:middle line:90%


01:00:45.240 --> 01:00:48.480 align:middle line:90%
So I can write it like this.

01:00:48.480 --> 01:00:52.750 align:middle line:90%
Now, this is where I use--

01:00:52.750 --> 01:00:59.550 align:middle line:84%
so s here will have to
lie between zero and x.

01:00:59.550 --> 01:01:01.783 align:middle line:90%
And so x is between--

01:01:01.783 --> 01:01:05.940 align:middle line:90%


01:01:05.940 --> 01:01:07.990 align:middle line:90%
let me just draw it here.

01:01:07.990 --> 01:01:11.610 align:middle line:90%
So here I have zero.

01:01:11.610 --> 01:01:13.890 align:middle line:90%
Here I have delta zero.

01:01:13.890 --> 01:01:18.270 align:middle line:84%
And then I have-- this is zero,
and here I have x somewhere.

01:01:18.270 --> 01:01:21.910 align:middle line:90%


01:01:21.910 --> 01:01:25.500 align:middle line:90%
So this means that--

01:01:25.500 --> 01:01:33.280 align:middle line:84%
this means that so here you have
x, but x itself, x has to lie--

01:01:33.280 --> 01:01:40.180 align:middle line:84%
x has to lie between delta
zero minus delta zero,

01:01:40.180 --> 01:01:41.510 align:middle line:90%
and delta zero.

01:01:41.510 --> 01:01:45.290 align:middle line:84%
And s has to lie
between zero and x.

01:01:45.290 --> 01:01:49.730 align:middle line:84%
So this means that s
here lies between--

01:01:49.730 --> 01:01:53.505 align:middle line:84%
x will lie in this
interval, also.

01:01:53.505 --> 01:01:58.889 align:middle line:90%


01:01:58.889 --> 01:02:01.466 align:middle line:90%
But now you see that--

01:02:01.466 --> 01:02:06.400 align:middle line:90%


01:02:06.400 --> 01:02:13.040 align:middle line:84%
so now if we're looking
at-- so we have T of y in x.

01:02:13.040 --> 01:02:18.700 align:middle line:84%
Again, remember that
x here is less than

01:02:18.700 --> 01:02:20.860 align:middle line:90%
or equal to delta zero.

01:02:20.860 --> 01:02:24.040 align:middle line:84%
So we have that
this thing here is

01:02:24.040 --> 01:02:28.700 align:middle line:84%
less than or equal to a plus,
and then the integral from zero

01:02:28.700 --> 01:02:44.510 align:middle line:84%
to x of f of y of
s, plus g of s ds.

01:02:44.510 --> 01:02:48.500 align:middle line:84%
And the first thing I
observe is that s here

01:02:48.500 --> 01:02:53.270 align:middle line:84%
is also, just because
x was in that interval,

01:02:53.270 --> 01:02:56.690 align:middle line:90%
you also have that s--

01:02:56.690 --> 01:03:01.850 align:middle line:84%
because x is in that interval,
s is also in this interval.

01:03:01.850 --> 01:03:06.860 align:middle line:84%
The second thing I
observe is that I'm

01:03:06.860 --> 01:03:12.320 align:middle line:84%
assuming that the function
that I start with at each point

01:03:12.320 --> 01:03:20.450 align:middle line:84%
have no less than R. Now, if
I'm using these two things,

01:03:20.450 --> 01:03:22.800 align:middle line:90%
then I have that--

01:03:22.800 --> 01:03:30.520 align:middle line:84%
so this means that g
of s, this one here,

01:03:30.520 --> 01:03:35.820 align:middle line:84%
this is how we defined L2
because this interval here

01:03:35.820 --> 01:03:40.270 align:middle line:84%
is contained in the interval
between minus 1 and 1.

01:03:40.270 --> 01:03:42.970 align:middle line:84%
This here is contained in the
interval between negative,

01:03:42.970 --> 01:03:45.720 align:middle line:90%
minus 1 and 1.

01:03:45.720 --> 01:03:51.690 align:middle line:84%
So we have that g of s
is less than this L2,

01:03:51.690 --> 01:03:52.865 align:middle line:90%
less than or equal to L2.

01:03:52.865 --> 01:03:56.502 align:middle line:90%


01:03:56.502 --> 01:04:03.240 align:middle line:84%
The second thing we observe is
that because we have this here,

01:04:03.240 --> 01:04:06.140 align:middle line:90%
for each s, we have this.

01:04:06.140 --> 01:04:09.420 align:middle line:90%


01:04:09.420 --> 01:04:16.360 align:middle line:84%
Then it means, you
see, by the first--

01:04:16.360 --> 01:04:25.460 align:middle line:84%
by the definition of
L1 that f of y of s,

01:04:25.460 --> 01:04:28.150 align:middle line:84%
this thing here,
is less than L1.

01:04:28.150 --> 01:04:30.920 align:middle line:90%


01:04:30.920 --> 01:04:35.572 align:middle line:90%
L1 and L2 are now fixed numbers.

01:04:35.572 --> 01:04:39.350 align:middle line:84%
And so you see that this
second thing here, I

01:04:39.350 --> 01:04:42.660 align:middle line:90%
can bound this thing here by--

01:04:42.660 --> 01:04:45.657 align:middle line:84%
so this is less
than or equal to a.

01:04:45.657 --> 01:04:47.490 align:middle line:84%
And that should have
been an absolute value.

01:04:47.490 --> 01:04:52.610 align:middle line:84%
Somehow I lost it when I
copied it from this line.

01:04:52.610 --> 01:04:55.190 align:middle line:90%
a, absolute value of a.

01:04:55.190 --> 01:04:59.390 align:middle line:84%
And then on the first one
here, the length of this

01:04:59.390 --> 01:05:05.100 align:middle line:84%
interval, but that is, of
course, bounded by delta zero.

01:05:05.100 --> 01:05:11.450 align:middle line:84%
So this is plus delta zero, and
then the maximum possible value

01:05:11.450 --> 01:05:14.360 align:middle line:90%
of this, that would be L1.

01:05:14.360 --> 01:05:17.900 align:middle line:84%
And then likewise, the length of
this interval you're integrating

01:05:17.900 --> 01:05:20.160 align:middle line:90%
over is at most delta zero.

01:05:20.160 --> 01:05:23.700 align:middle line:84%
And this one here cannot
be larger than L2.

01:05:23.700 --> 01:05:24.855 align:middle line:90%
So you have this.

01:05:24.855 --> 01:05:27.660 align:middle line:90%


01:05:27.660 --> 01:05:31.900 align:middle line:84%
And now, remember
what delta zero was.

01:05:31.900 --> 01:05:33.510 align:middle line:90%
And I will just--

01:05:33.510 --> 01:05:37.570 align:middle line:84%
I have just on the
bottom, below here.

01:05:37.570 --> 01:05:39.630 align:middle line:90%
But let me just write it here.

01:05:39.630 --> 01:05:44.220 align:middle line:84%
This here was what delta
zero was chosen to be,

01:05:44.220 --> 01:05:54.110 align:middle line:84%
the minimum, 1 over L1
plus 1, 1 over L2 plus 1.

01:05:54.110 --> 01:06:03.520 align:middle line:90%


01:06:03.520 --> 01:06:11.910 align:middle line:84%
So now, we have that this thing
here is less than this here.

01:06:11.910 --> 01:06:16.260 align:middle line:90%
We just keep this thing here.

01:06:16.260 --> 01:06:24.010 align:middle line:84%
Well, delta is, in particular,
less than this thing here.

01:06:24.010 --> 01:06:31.420 align:middle line:84%
So you see that if you plug in
this, so it's like plus 1, L1

01:06:31.420 --> 01:06:34.300 align:middle line:90%
plus 1 times L1.

01:06:34.300 --> 01:06:37.910 align:middle line:84%
Likewise, over here,
you're using this.

01:06:37.910 --> 01:06:42.500 align:middle line:84%
So you're getting 1
over L2 plus 1 L2.

01:06:42.500 --> 01:06:45.710 align:middle line:84%
And now you see that this
thing here is less than 1.

01:06:45.710 --> 01:06:47.480 align:middle line:90%
This is less than 1.

01:06:47.480 --> 01:06:49.780 align:middle line:90%
So this is less than a.

01:06:49.780 --> 01:06:52.450 align:middle line:84%
It's actually strictly less,
but it doesn't really matter.

01:06:52.450 --> 01:06:59.230 align:middle line:90%
a plus 2 like this.

01:06:59.230 --> 01:07:05.320 align:middle line:90%


01:07:05.320 --> 01:07:07.840 align:middle line:90%
So this means that--

01:07:07.840 --> 01:07:12.670 align:middle line:84%
so then, but this
here, this was exactly

01:07:12.670 --> 01:07:17.750 align:middle line:84%
the definition of capital
R. And so you have that.

01:07:17.750 --> 01:07:20.060 align:middle line:84%
And when I copied
it over, I also

01:07:20.060 --> 01:07:23.780 align:middle line:84%
forgot to put absolute
value sign here.

01:07:23.780 --> 01:07:27.270 align:middle line:84%
So you have that
if-- so have that

01:07:27.270 --> 01:07:31.310 align:middle line:84%
if-- so the conclusion
here is that if y here

01:07:31.310 --> 01:07:41.060 align:middle line:84%
is a continuous function
on this interval here,

01:07:41.060 --> 01:07:47.420 align:middle line:84%
and the norm of y at each point
is less or equal to r, well,

01:07:47.420 --> 01:07:58.010 align:middle line:84%
then you have that T of y at
each point is less than R.

01:07:58.010 --> 01:08:02.780 align:middle line:84%
It's actually strictly less,
but we don't care about that.

01:08:02.780 --> 01:08:09.920 align:middle line:90%
So what you have now is--

01:08:09.920 --> 01:08:14.960 align:middle line:84%
so what we now have proven
is that we have this map T.

01:08:14.960 --> 01:08:17.250 align:middle line:84%
And now I'm going to
think about this map--

01:08:17.250 --> 01:08:26.220 align:middle line:84%
sorry-- on the space of y that
is continuous on this interval

01:08:26.220 --> 01:08:26.720 align:middle line:90%
here.

01:08:26.720 --> 01:08:32.220 align:middle line:90%


01:08:32.220 --> 01:08:35.340 align:middle line:84%
And what you have
is-- and also, sorry.

01:08:35.340 --> 01:08:40.149 align:middle line:84%
And I'm thinking about with
the norm at each point.

01:08:40.149 --> 01:08:41.819 align:middle line:90%
This here is less than R.

01:08:41.819 --> 01:08:45.340 align:middle line:84%
And again, this is really a
ball in this metric space,

01:08:45.340 --> 01:08:48.569 align:middle line:84%
but let me just write
it out like this.

01:08:48.569 --> 01:08:50.970 align:middle line:84%
And what you have
is that-- sorry.

01:08:50.970 --> 01:08:56.340 align:middle line:84%
This is the space, and
you have that T of y.

01:08:56.340 --> 01:09:01.090 align:middle line:84%
If y is in this space, then
T of y is in the same space.

01:09:01.090 --> 01:09:06.919 align:middle line:84%
So T of y is also
continuous on that interval.

01:09:06.919 --> 01:09:09.490 align:middle line:90%


01:09:09.490 --> 01:09:16.200 align:middle line:84%
And T of y at each point
x is less or equal to R.

01:09:16.200 --> 01:09:19.275 align:middle line:84%
So the map mapped this
space into itself.

01:09:19.275 --> 01:09:22.495 align:middle line:90%


01:09:22.495 --> 01:09:28.120 align:middle line:84%
Now, the next thing
we want to prove

01:09:28.120 --> 01:09:30.496 align:middle line:90%
is that the map is contracting.

01:09:30.496 --> 01:09:46.900 align:middle line:90%


01:09:46.900 --> 01:09:49.029 align:middle line:90%
You see that you need--

01:09:49.029 --> 01:09:52.640 align:middle line:84%
you know if this
space is not stable.

01:09:52.640 --> 01:09:57.550 align:middle line:84%
So imagine that you
take-- so we're starting

01:09:57.550 --> 01:09:59.210 align:middle line:90%
with some giant metric space.

01:09:59.210 --> 01:10:02.550 align:middle line:84%
This is the continuous
function, say, on this interval.

01:10:02.550 --> 01:10:09.040 align:middle line:90%


01:10:09.040 --> 01:10:12.470 align:middle line:84%
And then we're looking
at some subspace of that.

01:10:12.470 --> 01:10:14.785 align:middle line:84%
So these are continuous
on a smaller interval.

01:10:14.785 --> 01:10:19.740 align:middle line:90%


01:10:19.740 --> 01:10:23.600 align:middle line:90%
And then we have to find a map.

01:10:23.600 --> 01:10:29.090 align:middle line:84%
But if somehow the
map was taking us

01:10:29.090 --> 01:10:31.950 align:middle line:84%
out of the space where
it's contracting,

01:10:31.950 --> 01:10:35.970 align:middle line:84%
then we couldn't keep
applying the contracting map.

01:10:35.970 --> 01:10:38.420 align:middle line:90%
It wouldn't anymore be--

01:10:38.420 --> 01:10:41.370 align:middle line:84%
And the thing is that
you want to just iterate.

01:10:41.370 --> 01:10:42.290 align:middle line:90%
You want to keep.

01:10:42.290 --> 01:10:44.360 align:middle line:84%
You want to pick some
point, and then you

01:10:44.360 --> 01:10:47.610 align:middle line:84%
want to keep applying
the contracting map.

01:10:47.610 --> 01:10:51.360 align:middle line:84%
So you want it to stay in the
space where it is contracting.

01:10:51.360 --> 01:10:53.750 align:middle line:84%
And so this is
what we did in one.

01:10:53.750 --> 01:10:56.660 align:middle line:84%
But we haven't yet proved
that the map is contracting.

01:10:56.660 --> 01:11:00.440 align:middle line:84%
And so now, to prove that
the map is contracting,

01:11:00.440 --> 01:11:05.175 align:middle line:84%
we're going to further
restrict the interval.

01:11:05.175 --> 01:11:08.600 align:middle line:84%
And so this is-- so
I'm going to set.

01:11:08.600 --> 01:11:11.400 align:middle line:84%
I'm going to define
now one more constant.

01:11:11.400 --> 01:11:13.130 align:middle line:90%
Sorry about that.

01:11:13.130 --> 01:11:15.750 align:middle line:90%
So this is M here.

01:11:15.750 --> 01:11:21.660 align:middle line:84%
And M is going to be
just the max of f prime--

01:11:21.660 --> 01:11:24.450 align:middle line:90%


01:11:24.450 --> 01:11:29.460 align:middle line:84%
of f prime of z,
absolute value of this,

01:11:29.460 --> 01:11:35.563 align:middle line:84%
where z here is less or
equal to R. So this is my--

01:11:35.563 --> 01:11:41.730 align:middle line:90%


01:11:41.730 --> 01:11:44.315 align:middle line:84%
well, almost the second
last constant function.

01:11:44.315 --> 01:11:48.090 align:middle line:90%


01:11:48.090 --> 01:11:50.640 align:middle line:84%
And now I'm going
to define this.

01:11:50.640 --> 01:11:54.540 align:middle line:84%
So the last constant is
going to be the interval

01:11:54.540 --> 01:11:55.870 align:middle line:90%
that I'm going to work with.

01:11:55.870 --> 01:11:58.170 align:middle line:84%
So remember, what
I'm trying to do

01:11:58.170 --> 01:12:03.970 align:middle line:84%
is, I have this
differential equation.

01:12:03.970 --> 01:12:11.230 align:middle line:84%
And I want to say that, near
zero, there is a solution.

01:12:11.230 --> 01:12:14.830 align:middle line:84%
But near zero just means that
there exists some tiny interval

01:12:14.830 --> 01:12:17.090 align:middle line:84%
around zero where
I have a solution.

01:12:17.090 --> 01:12:20.350 align:middle line:84%
And again, if I have time,
I also will do it next time.

01:12:20.350 --> 01:12:24.610 align:middle line:84%
I will give an example where you
can see that, in general, you

01:12:24.610 --> 01:12:27.430 align:middle line:84%
would need to look at a
very tiny interval for this

01:12:27.430 --> 01:12:28.250 align:middle line:90%
to have a solution.

01:12:28.250 --> 01:12:30.720 align:middle line:84%
Otherwise, it doesn't have a
solution on a very large set.

01:12:30.720 --> 01:12:34.370 align:middle line:90%


01:12:34.370 --> 01:12:36.500 align:middle line:90%
So I define it like this.

01:12:36.500 --> 01:12:38.960 align:middle line:90%
And then I define delta here.

01:12:38.960 --> 01:12:44.680 align:middle line:84%
So delta is now going to be
the minimum of delta zero,

01:12:44.680 --> 01:12:50.340 align:middle line:84%
the one from before, and
then 1 over 2M plus 1.

01:12:50.340 --> 01:12:53.320 align:middle line:90%


01:12:53.320 --> 01:12:58.360 align:middle line:84%
And now I want to
look at the space.

01:12:58.360 --> 01:13:02.320 align:middle line:84%
So I want to look
at T. And then T

01:13:02.320 --> 01:13:07.400 align:middle line:84%
is going to be a map from
the continuous functions.

01:13:07.400 --> 01:13:10.720 align:middle line:84%
So y here is a
continuous function

01:13:10.720 --> 01:13:14.250 align:middle line:90%
on, now, this little interval.

01:13:14.250 --> 01:13:19.010 align:middle line:84%
So this interval here, because
you have the minimum of this,

01:13:19.010 --> 01:13:22.040 align:middle line:84%
this interval is contained
in the corresponding interval

01:13:22.040 --> 01:13:23.730 align:middle line:90%
with delta zero.

01:13:23.730 --> 01:13:28.880 align:middle line:84%
So it's y in this space, such
that the norm here at each point

01:13:28.880 --> 01:13:31.490 align:middle line:84%
is less than or
equal to R. That's

01:13:31.490 --> 01:13:33.330 align:middle line:90%
the space I'm going to look at.

01:13:33.330 --> 01:13:39.540 align:middle line:84%
And we already know that T
maps this space into itself,

01:13:39.540 --> 01:13:41.570 align:middle line:84%
because there's really
no new statement.

01:13:41.570 --> 01:13:43.860 align:middle line:90%
If the function is--

01:13:43.860 --> 01:13:48.390 align:middle line:84%
so as long as you have this
here, and you apply T on it,

01:13:48.390 --> 01:13:50.490 align:middle line:84%
T, when you apply
T on a function,

01:13:50.490 --> 01:13:52.200 align:middle line:84%
it's defined on
the same interval.

01:13:52.200 --> 01:13:55.280 align:middle line:84%
So it will automatically define
on this smaller interval.

01:13:55.280 --> 01:13:58.890 align:middle line:84%
And we already
have this property.

01:13:58.890 --> 01:14:03.170 align:middle line:84%
So T maps this space
here into itself.

01:14:03.170 --> 01:14:06.260 align:middle line:90%


01:14:06.260 --> 01:14:08.780 align:middle line:90%
And now I want to prove.

01:14:08.780 --> 01:14:10.570 align:middle line:90%
I want to estimate.

01:14:10.570 --> 01:14:14.850 align:middle line:84%
So I take two elements
in this space.

01:14:14.850 --> 01:14:17.230 align:middle line:90%
So I have y1 and y2.

01:14:17.230 --> 01:14:18.850 align:middle line:90%
So you're looking at--

01:14:18.850 --> 01:14:25.800 align:middle line:90%
so y1 and y2 are in this space.

01:14:25.800 --> 01:14:35.240 align:middle line:84%
And you want to look at what is
the distance between y1 and y2.

01:14:35.240 --> 01:14:39.450 align:middle line:90%


01:14:39.450 --> 01:14:42.960 align:middle line:84%
So we want this
here, and we want--

01:14:42.960 --> 01:14:47.400 align:middle line:84%
what I want to prove is
that it's contracting.

01:14:47.400 --> 01:14:48.755 align:middle line:90%
So we want to show.

01:14:48.755 --> 01:14:54.030 align:middle line:90%


01:14:54.030 --> 01:14:55.470 align:middle line:90%
And I want to prove.

01:14:55.470 --> 01:14:58.020 align:middle line:90%
I'm going to prove it.

01:14:58.020 --> 01:15:00.700 align:middle line:90%
My constant c will be explicit.

01:15:00.700 --> 01:15:06.510 align:middle line:84%
It will be just one half, so
that certainly is less than 1.

01:15:06.510 --> 01:15:07.970 align:middle line:90%
And this is what I want.

01:15:07.970 --> 01:15:12.601 align:middle line:90%


01:15:12.601 --> 01:15:20.595 align:middle line:90%
So now, let's look at them.

01:15:20.595 --> 01:15:26.320 align:middle line:90%


01:15:26.320 --> 01:15:31.380 align:middle line:90%
So T of y1 minus T of y2.

01:15:31.380 --> 01:15:34.090 align:middle line:90%


01:15:34.090 --> 01:15:38.110 align:middle line:84%
This thing here,
T of y1 is defined

01:15:38.110 --> 01:15:40.850 align:middle line:90%
to be a plus the integral.

01:15:40.850 --> 01:15:41.440 align:middle line:90%
Sorry.

01:15:41.440 --> 01:15:42.470 align:middle line:90%
And let me write.

01:15:42.470 --> 01:15:44.290 align:middle line:84%
So I'm going to--
let me just make

01:15:44.290 --> 01:15:45.770 align:middle line:90%
it a little more space here.

01:15:45.770 --> 01:15:49.150 align:middle line:84%
I worry that I'm running
out of time, but let's see.

01:15:49.150 --> 01:15:53.320 align:middle line:84%
So this thing here,
minus T of y2.

01:15:53.320 --> 01:15:56.690 align:middle line:84%
And I'm just looking at
the difference in some x.

01:15:56.690 --> 01:15:59.890 align:middle line:90%
And again, x here is now in--

01:15:59.890 --> 01:16:03.880 align:middle line:90%
x here will be in the integral.

01:16:03.880 --> 01:16:11.580 align:middle line:84%
You were looking at x in the
integral, in this integral.

01:16:11.580 --> 01:16:15.580 align:middle line:84%
And so I'm just writing down
first here what this is.

01:16:15.580 --> 01:16:29.030 align:middle line:84%
This is the integral from a to
x of f of y1, s plus g of s.

01:16:29.030 --> 01:16:33.660 align:middle line:90%


01:16:33.660 --> 01:16:36.420 align:middle line:90%
And then you have minus.

01:16:36.420 --> 01:16:39.750 align:middle line:90%
This is what you get for y2.

01:16:39.750 --> 01:16:43.040 align:middle line:90%
a, so minus this thing here.

01:16:43.040 --> 01:16:56.760 align:middle line:90%


01:16:56.760 --> 01:17:00.690 align:middle line:90%
So this is this difference.

01:17:00.690 --> 01:17:02.730 align:middle line:84%
And what you see
is the first thing

01:17:02.730 --> 01:17:06.370 align:middle line:84%
you observe is that
this a here cancels.

01:17:06.370 --> 01:17:11.090 align:middle line:84%
But not only does this cancel,
but this term here also cancel.

01:17:11.090 --> 01:17:13.480 align:middle line:84%
And actually, there
was a good reason

01:17:13.480 --> 01:17:15.460 align:middle line:90%
that there are lower order.

01:17:15.460 --> 01:17:20.380 align:middle line:84%
And the point here is
that by-- the main point

01:17:20.380 --> 01:17:23.660 align:middle line:84%
is in the unknown
function anyway.

01:17:23.660 --> 01:17:29.290 align:middle line:84%
And it's what's called
a non-linear equation.

01:17:29.290 --> 01:17:33.598 align:middle line:90%
So that's a difficulty.

01:17:33.598 --> 01:17:37.150 align:middle line:84%
But what you then get
when you write down,

01:17:37.150 --> 01:17:40.150 align:middle line:84%
when you have-- after
the cancellation, what

01:17:40.150 --> 01:17:55.520 align:middle line:84%
you get is f of y1 of s
minus f of y2 of s, ds.

01:17:55.520 --> 01:17:57.700 align:middle line:90%
So you have that.

01:17:57.700 --> 01:18:05.970 align:middle line:84%
Now, I will look at this thing
here and that thing here.

01:18:05.970 --> 01:18:07.220 align:middle line:90%
And I'm going to--

01:18:07.220 --> 01:18:10.530 align:middle line:90%
and you have to now abstract.

01:18:10.530 --> 01:18:13.790 align:middle line:84%
So now I'm going to look
at this difference here.

01:18:13.790 --> 01:18:18.170 align:middle line:84%
And then now, the thing is that
you have to abstract from it,

01:18:18.170 --> 01:18:23.540 align:middle line:84%
and you have to think
about s as being--

01:18:23.540 --> 01:18:28.040 align:middle line:84%
if you think about
s as being fixed,

01:18:28.040 --> 01:18:31.790 align:middle line:90%
then this is just two numbers.

01:18:31.790 --> 01:18:37.970 align:middle line:84%
You could think about this
as z1 and this here as z2.

01:18:37.970 --> 01:18:40.950 align:middle line:90%
This is z1, and this is z2.

01:18:40.950 --> 01:18:46.105 align:middle line:84%
So it's like f of
z1 minus f of z2.

01:18:46.105 --> 01:18:48.671 align:middle line:90%


01:18:48.671 --> 01:18:52.910 align:middle line:84%
Now, the mean value theorem
tells us that this thing here

01:18:52.910 --> 01:18:59.810 align:middle line:84%
is equal to the derivative
at some intermediate point,

01:18:59.810 --> 01:19:12.570 align:middle line:84%
let's say, z3, where z3
is between z1 and z2,

01:19:12.570 --> 01:19:17.640 align:middle line:90%
and then times z1 minus z2.

01:19:17.640 --> 01:19:23.400 align:middle line:90%


01:19:23.400 --> 01:19:30.210 align:middle line:84%
So this is just for
any xs, you have this.

01:19:30.210 --> 01:19:33.150 align:middle line:90%
But this means that--

01:19:33.150 --> 01:19:36.240 align:middle line:84%
this means that-- are we
are almost out of time?

01:19:36.240 --> 01:19:42.960 align:middle line:84%
So this means that when you're
looking at the norm of this,

01:19:42.960 --> 01:19:54.850 align:middle line:84%
f of y1 of s minus f of y2
of s, that the norm here is--

01:19:54.850 --> 01:20:04.390 align:middle line:84%
so the norm is equal to
f prime at z3 times z1.

01:20:04.390 --> 01:20:05.840 align:middle line:90%
And z1 I can write in.

01:20:05.840 --> 01:20:07.010 align:middle line:90%
It's really this.

01:20:07.010 --> 01:20:13.030 align:middle line:90%
And this is z2.

01:20:13.030 --> 01:20:16.210 align:middle line:84%
This thing here,
remember, z is some point

01:20:16.210 --> 01:20:18.380 align:middle line:90%
in between those two points.

01:20:18.380 --> 01:20:22.430 align:middle line:84%
But both of these points,
both of these points here,

01:20:22.430 --> 01:20:28.810 align:middle line:84%
both this one here and that
one here have norm less than R.

01:20:28.810 --> 01:20:31.850 align:middle line:90%
So this here is--

01:20:31.850 --> 01:20:37.390 align:middle line:84%
but now where the way
that M was defined,

01:20:37.390 --> 01:20:41.380 align:middle line:84%
and it should have
been on the same board.

01:20:41.380 --> 01:20:49.570 align:middle line:84%
So M here was defined to be
the maximum of f prime of z,

01:20:49.570 --> 01:20:53.860 align:middle line:90%
where z was less or equal to 1.

01:20:53.860 --> 01:20:57.520 align:middle line:84%
And so you see that
this thing here where

01:20:57.520 --> 01:21:01.850 align:middle line:84%
you take the derivative
that is bounded by M.

01:21:01.850 --> 01:21:12.635 align:middle line:84%
So this thing here is less than
M y1 s minus y2 of s, like that.

01:21:12.635 --> 01:21:14.720 align:middle line:84%
So I'm not sure
where we should stop.

01:21:14.720 --> 01:21:17.280 align:middle line:84%
We over, and I probably
need a few more minutes.

01:21:17.280 --> 01:21:18.530 align:middle line:90%
Maybe we should stop.

01:21:18.530 --> 01:21:25.520 align:middle line:84%
And it's not a great place to
stop, but that's how it goes.

01:21:25.520 --> 01:21:29.990 align:middle line:84%
So I will keep
you in suspension,

01:21:29.990 --> 01:21:37.020 align:middle line:84%
and so we'll pick up
from here on Tuesday.

01:21:37.020 --> 01:21:41.480 align:middle line:84%
And so I want anyway to
explain to you why, actually,

01:21:41.480 --> 01:21:45.530 align:middle line:84%
this method, which seems
a little crazy in a way

01:21:45.530 --> 01:21:48.650 align:middle line:84%
because it's bringing in all
these things, why it turned out

01:21:48.650 --> 01:21:51.980 align:middle line:90%
to be basically optimal.

01:21:51.980 --> 01:21:56.830 align:middle line:84%
And then we'll do a review the
rest of the time on Tuesday.

01:21:56.830 --> 01:21:59.000 align:middle line:90%