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GILBERT STRANG: OK,
let me make a start.
On the left, you see
the topic for today.
We're doing pretty well.
This completes my review of the
highlights of linear algebra,
so that's five lectures.
I'll follow up on
those five points,
because the neat part is
it really ties together
the whole subject.
Eigenvalues, energy, A transpose
A, determinants, pivots--
they all come together.
Each one gives a test for
positive and definite matrices.
That's where I'm going.
Claire is hoping to come in
for a little bit of the class
to ask if anybody has
started on the homework.
And got Julia rolling, and got
a yes from the auto grader.
Is anybody like-- no.
You're taking a chance, right?
Julia, in principle, works,
but in practice, it's
always an adventure
the first time.
So we chose this
lab on convolution,
because it was the
first lab last year,
and it doesn't ask
for much math at all.
Really, you're just
creating a matrix
and getting the auto
grader to say, yes,
that's the right matrix.
And we'll see that matrix.
We'll see this
idea of convolution
at the right time, which
is not that far off.
It's signal processing,
and it's early in part
three of the book.
If Claire comes in,
she'll answer questions.
Otherwise, I guess it would
be emailing questions to--
I realize that the deadline
is not on top of you,
and you've got a whole
weekend to make Julia fly.
I'll start on the math then.
We had symmetric-- eigenvalues
of matrices, and especially
symmetric matrices, and
those have real eigenvalues,
and I'll quickly show why.
And orthogonal eigenvectors,
and I'll quickly show why.
But I want to move
to the new idea--
positive definite matrices.
These are the best of
the symmetric matrices.
They are symmetric matrices
that have positive eigenvalues.
That's the easy way to remember
positive definite matrices.
They have positive eigenvalues,
but it's certainly not
the easy way to test.
If I give you a matrix like
that, that's only two by two.
We could actually
find the eigenvalues,
but we would like to have other
tests, easier tests, which
would be equivalent to
positive eigenvalues.
Every one of those five tests--
any one of those five tests
is all you need.
Let me start with that
example and ask you to look,
and then I'm going to discuss
those five separate points.
My question is,
is that matrix s?
It's obviously symmetric.
Is it positive,
definite, or not?
You could compute
its eigenvalues
since it's two by two.
It's energy-- I'll come
back to that, because that's
the most important one.
Number two is
really fundamental.
Number three would ask
you to factor that.
Well, you don't want
to take time with that.
Well, what do you think?
Is it positive,
definite, or not?
I see an expert in the
front row saying no.
Why is it no?
The answer is no.
That's not a positive
definite matrix.
Where does it let us down?
It's got all positive
numbers, but that's not
what we're asking.
We're asking
positive eigenvalues,
positive determinants,
positive pivots.
How does it let us down?
Which is the easy test
to see that it fails?
AUDIENCE: Maybe determinant?
GILBERT STRANG: Determinant.
The determinant is 15
minus 16, so negative.
So how is the determinant
connected to the eigenvalues?
Everybody?
Yep.
AUDIENCE: [INAUDIBLE]
GILBERT STRANG:
It's the product.
So the two eigenvalues of
s, they're real, of course,
and they multiply to give the
determinant, which is minus 1.
So one of them is negative,
and one of them is positive.
This matrix is an
indefinite matrix--
indefinite.
So how could I make
it positive definite?
OK.
We can just play
with an example,
and then we see these
things happening.
Let's see.
OK, what shall I put in
place of the 5, for example?
I could lower the 4, or I
can up the 5, or up the 3.
I can make the diagonal entries.
If I add stuff to
the main diagonal,
I'm making it more positive.
So that's the
straightforward way.
So what number in
there would be safe?
AUDIENCE: 6.
GILBERT STRANG: 6.
OK.
6 would be safe.
If I go up from 5 to
6, I've gotta de--
so when I say here
"leading determinants,"
what does that mean?
That word leading
means something.
It means that I take
that 1 by 1 determinant--
it would have to pass that.
Just the determinant
itself would not do it.
Let me give you an example.
No for-- let me take
minus 3 and minus 6.
That would have the
same determinant.
The determinant would
still be 18 minus 16--
2.
But it fails the
test on the 1 by 1.
And this passes.
This passes the 1 by 1
test and 2 by 2 tests.
So that's what this means here.
Leading determinants
are from the upper left.
You have to check n
things because you've
got n eigenvalues.
And those are the n tests.
And have you noticed the
connection to pivots?
So let's just remember
that small item.
What would be the pivots
because we didn't take
a long time on elimination?
So what would be the pivots
for that matrix, 3-4-4-6?
Well, what's the first pivot?
3, sitting there-- the 1-1
entry would be the first pivot.
So the pivots would be 3,
and what's the second pivot?
Well, maybe to
see it clearly you
want me to take that
elimination step.
Why don't I do it just
so you'll see it here?
So elimination would subtract
some multiple of row 1
from row 2.
I would leave 1 one alone.
I would subtract some
multiple to get a 0 there.
And what's the multiple?
What's the multiplier?
AUDIENCE: In that much--
GILBERT STRANG: 4/3.
4/3 times row 1, away from
row 2, would produce that 0.
But 4/3 times the 4,
that would be 16/3.
And we're subtracting
it from 18/3.
I think we've got 2/3 left.
So the pivots, which is
this, in elimination,
are the 3 and the 2/3.
And of course, they're positive.
And actually, you see
the immediate connection.
This pivot is the 2 by 2
determinant divided by the 1
by 1 determinant.
The 2 by 2 determinant,
we figured out--
18 minus 16 was 2.
The 1 by 1 determinant is 3.
And sure enough, that
second pivot is 2/3.
This is not-- so by example,
I'm illustrating what these
different tests--
and again, each test
is all you need.
If it passes one test,
it passes them all.
And we haven't found
the eigenvalues.
Let me do the energy.
Can I do energy here?
OK.
So what's this--
I am saying that this is
really the great test.
That, for me, is the definition
of a positive definite matrix.
And the word "energy"
comes in because it's
quadratic, [INAUDIBLE] kinetic
energy or potential energy.
So that's the energy in the
vector x for this matrix.
So let me compute
it, x transpose Sx.
So let me put in S
here, the original S.
And let me put in of any
vector x, so, say xy or x1.
Maybe-- do you like x--
xy is easier.
So that's our
vector x transposed.
This is our matrix S.
And here's our vector x.
So it's a function of x and y.
It's a pure quadratic function.
Do you know what I get
when I multiply that out?
I get a very simple,
important type of function.
Shall we multiply it out?
Let's see.
Shall I multiply that by that
first, so I get 3x plus 4y?
And 4x plus 6y is what I'm
getting from these two.
And now I'm hitting
that with the xy.
And now I'm going
to see the energy.
And you'll see the pattern.
That's always what
math is about.
What's the pattern?
So I've x times 3x, 3x squared.
And I have y times 6y.
That's 6y squared.
And I have x times 4y.
That's for 4xy.
And I have y times 4x.
That's 4 more xy.
So I've got all those terms.
Every term, every
number in the matrix
gives me a piece of the energy.
And you see that the diagonal
numbers, 3 and 6, those
give me the diagonal pieces,
3x squared and 6y squared.
And then the cross--
or I maybe call them
the cross terms.
Those give me 4xy and
4xy, so, really, 8xy.
So you could call
this thing 8xy.
So that's my function.
That's my quadratic.
That's my energy.
And I believe that
is greater than 0.
Let me graph the thing.
Let me graph that energy.
OK.
So here's a graph of my
function, f of x and y.
Here is x, and here's y.
And of course, that's
on the graph, 0-0.
At x equals 0, y equals 0,
the function is clearly 0.
Everybody's got his eye-- let
me write that function again
here--
3x squared, 6y squared, 8xy.
Actually, you can see--
this is how I think
about that function.
So 3x squared is obviously
carrying me upwards.
It will never go negative.
6y squared will
never go negative.
8xy can go negative, right?
If x and y have opposite
signs, that'll go negative.
But the question is, do
these positive pieces
overwhelm it and make the
graph go up like a bowl?
And the answer is yes, for
a positive definite matrix.
So this is a graph of a
positive definite matrix,
of positive energy, the energy
of a positive definite matrix.
So this is the energy x
transpose Sx that I'm graphing.
And there it is.
This is important.
This is important.
This is the kind of function
we like, x transpose Sx,
where S is positive definite, so
the function goes up like that.
This is what deep
learning is about.
This could be a loss
function that you minimize.
It could depend on
100,000 variables or more.
And it could come from the
error in the difference
between training data and
the number you get it.
The loss would be some
expression like that.
Well, I'll make sense of
those words as soon as I can.
What I want to say is deep
learning, neural nets, machine
learning, the big computation--
is to minimize an energy--
is to minimize an energy.
Now of course, I
made the minimum
easy to find because
I have pure squares.
Well, that doesn't happen
in practice, of course.
In practice, we have linear
terms, x transpose b,
or nonlinear.
Yeah, the loss function doesn't
have to be a [INAUDIBLE] cross
entropy, all kinds of things.
There is a whole dictionary
of possible loss functions.
But but this is the model.
This is the model.
And I'll make it
the perfect model
by just focusing on that part.
Well, by the way, what would
happen if that was in there?
I shouldn't have X'd
it out so quickly
since I just put it up there.
Let me put it back up.
I thought better of it.
OK.
This is a kind of least squares
problem with some data, b.
Minimize that.
So what would be the
graph of this guy?
Can I just draw the same sort
of picture for that function?
Will it be a bowl?
Yes.
If I have this
term, all that does
is move it off center
here, at x equals 0.
Well, I still get 0.
Sorry.
I still go through that point.
If this is the 0 vector,
I'm still getting 0.
But this, we'll bring it below.
That would produce
a bowl like that.
Actually, it would
just be the same bowl.
The bowl would just be shifted.
I could write that to
show how that happens.
So this is now below 0.
That's the solution
we're after that tells us
the weights in the
neural network.
I'm just using these
words, but we'll soon
have a meaning to them.
I want to find that
minimum, in other words.
And I want to find it for much
more complicated functions
than that.
Of course, if I
minimize the quadratic,
that means setting
derivatives to 0.
I just have linear equations.
Probably, I could write
everything down for that thing.
So let's put in some
nonlinear stuff,
which way to wiggles the
bowl, makes it not so easy.
Can I look a month ahead?
How do you find--
so this is a big
part of mathematics--
applied math,
optimization, minimization
of a complicated function
of 100,000 variables.
That's the biggest computation.
That's the reason machine
learning on big problems
takes a week on a
GPU or multiple GPUs,
because you have
so many unknowns.
More than 100,000
would be quite normal.
In general, let's just have
the pleasure of looking ahead
for one minute, and then
I'll come back to real life
here, linear algebra.
I can't resist thinking aloud,
how do you find the minimum?
By the way, these functions,
both of them, are convex.
So that is convex.
So I want to connect
convex functions, f--
and what does convex mean?
It means, well, that
the graph is like that.
[LAUGHTER]
Not perfect, it could--
but if it's a
quadratic, then convex
means positive
definite, or maybe
in the extreme,
positive semidefinite.
I'll have to mention that.
But convex means it goes up.
But it could have wiggles.
It doesn't have to be
just perfect squares
in linear terms,
but general things.
And for deep learning,
it will include non--
it will go far
beyond quadratics.
Well, it may not be convex.
I guess that's also true.
Yeah.
So deep learning has
got serious problems
because those
functions, they may
look like this but then over
here they could go nonxconvex.
They could dip
down a little more.
And you're looking for this
point or for this point.
Still, I'm determined to tell
you how to find it or a start
on how you find it.
So you're at some point.
Start there, somewhere
on the surface.
Some x, some vector
x is your start, x0--
starting point.
And we're going to just take a
step, hopefully down the bowl.
Well of course, it would
be fantastic to get there
in one step, but that's
not going to happen.
That would be solving a big
linear system, very expensive,
and a big nonlinear system.
So really, that's what
we're trying to solve--
a big nonlinear system.
And I should be on this
picture because here we
can see where the minimum is.
But they just shift.
So what would you do if
you had a starting point
and you wanted to go
look for the minimum?
What's the natural idea?
Compute derivatives.
You've got calculus
on your side.
Compute the first derivatives.
So the first derivatives
with respect to x--
so I would compute the
derivative with respect
to x, and the derivative
of f with respect to y,
and 100,000 more.
And that takes a little while.
And now I've got
the derivatives.
What do I do?
AUDIENCE: [INAUDIBLE]
GILBERT STRANG: I
go-- that tells me
the steepest direction.
That tells me, at
that point, which
way is the fastest way down.
So I would follow--
I would do a gradient descent.
I would follow that gradient.
This is called the gradient,
all the first derivatives.
It's called the gradient of f--
the gradient.
Gradient vector-- it's
a vector, of course,
because f is a function
of lots of variables.
I would start down
in that direction.
And how far to go, that's
the million dollar question
in deep learning.
Is it going to hit 0?
Nope.
It's not.
It's not.
So basically, you
go down until it--
so you're traveling here in
the x, along the gradient.
And you're not going to hit 0.
You're all going here
in some direction.
So you keep going down
this thing until it--
oh, I'm not Rembrandt here.
Your path down-- think of
yourself on a mountain.
You're trying to go down hill.
So you take-- as
fast as you can.
So you take the steepest
route down until--
but you have blinkers.
Once you decide on a direction,
you go in that direction.
Of course-- so what will happen?
You'll go down for
a while and then
it will turn up again when
you get to, maybe, close
to the bottom or maybe not.
You're not going to hit here.
And it's going to
miss that and come up.
Maybe I should draw it
over here, whatever.
So it's called a line search,
to decide how far to go there.
And then say, OK stop.
And you can invest a lot
of time or a little time
to decide on that
first stopping point.
And now just tell me,
what do you do next?
So now you're here.
What now?
Recalculate the gradient.
Find the steepest way
down from that point,
follow it until it turns
up or approximately,
then you're at a new point.
So this is gradient descent.
That's gradient descent,
the big algorithm
of deep learning of neural
nets, of machine learning--
of optimization, you could say.
Notice that we didn't
compute second derivatives.
If we computed
second derivatives,
we could have a fancier
formula that could
account for the curve here.
But to compute
second derivatives
when you've got hundreds
and thousands of variables
is not a lot of fun.
So most effectively,
machine learning
is limited to first
derivatives, the gradient.
OK.
So that's the general idea.
But there are lots and
lots of decisions and--
why doesn't that-- how
well does that work,
maybe, is a good
question to ask.
Does this work pretty well or
do we have to add more ideas?
Well, it doesn't
always work well.
Let me tell you
what the trouble is.
I'm way off-- this is
March or something.
But anyway, I'll
finish this sentence.
So what's the problem with
this gradient descent idea?
It turns out, if you're
going down a narrow valley--
I don't know, if you can sort
of imagine a narrow valley
toward the bottom.
So here's the bottom.
Here's your starting point.
And this is-- you have to
have think of this as a bowl.
So the bowl is--
or the two eigenvalues,
you could say--
are 1 and a very small number.
The bowl is long and thin.
Are you with me?
Imagine a long, thin bowl.
Then what happens for that case?
You take the steepest descent.
But you cross the valley,
and very soon, you're
climbing again.
So you take very,
very small steps,
just staggering back
and forth across this
and getting slowly, but too
slowly, toward the bottom.
So that's why things
have got to be improved.
If you have a very small
eigenvalue and a very large
eigenvalue, those tell you the
shape of the bowl, of course.
And many cases will
be like that-- have
a small and a large eigenvalue.
And then you're
spending all your time.
You're quickly going up the
other side, down, up, down, up,
down.
And you need a new idea.
OK, so that's really--
so this is one major reason
why positive definite
is so important because
positive definite gives
pictures like that.
But then, we have
this question of,
are the eigenvalues
sort of the same size?
Of course, if the
eigenvalues are all equal,
what's my bowl like?
Suppose I have the identity.
So then x squared plus y
squared is my function.
Then it's a perfectly
circular bowl.
What will happen?
Can you imagine a
perfectly circular--
like any bowl in the kitchen is
probably, most likely circular.
And suppose I do
gradient descent there.
I start at some point on
this perfectly circular bowl.
I start down.
And where do I
stop in that case?
Do I hit bottom?
I do, by symmetry.
So if I take x squared plus
y squared as my function
and I start somewhere, I
figure out the gradient.
Yeah.
The answer is I'll go
right through the center.
So really positive eigenvalues,
positive definite matrices
give us a bowl.
But if the eigenvalues
are far apart,
that's when we have problems.
OK.
I'm going back to my
job, which is this--
because this is so nice.
Right.
Could you-- well,
the homework that's
maybe going out this minute
for middle of next week
gives you some
exercises with this.
Let me do a couple of things,
a couple of exercises here.
For example, suppose I have a
positive definite matrix, S,
and a positive definite matrix,
T. If I add those matrices,
is the result positive definite?
So there is a perfect
math question,
and we hope to answer it.
So S and T--
positive definite.
What about S plus T?
Is that matrix
positive definite?
OK.
How do I answer such a question?
I look at my five tests
and I think, can I use it?
Which one will be good?
And one that won't tell
me much is the eigenvalues
because the
eigenvalues of S plus T
are not immediately clear from
the eigenvalues of S and T
separately.
I don't want to use that test.
This is my favorite test,
so I'm going to use that.
What about the energy in--
so look at the energy.
So I look at x
transpose, S plus T x.
And what's my question
in my mind here?
Is that a positive number
or not, for every x?
And how am I going to
answer that question?
Just separate those
into two pieces, right?
It's there in front of me.
It's this one plus this one.
And both of those are positive,
so the answer is yes, it
is positive definite.
Yes.
You see how the
energy was right.
I don't want to compute the
pivots or any determinants.
That would be a nightmare trying
to find the determinants for S
plus T. But this one
just does it immediately.
What else would be a good
example to start with?
What about S inverse?
Is that positive definite?
So let me ask S
positive definite,
and I want to ask
about its inverse.
So its inverse is
a symmetric matrix.
And is it positive definite?
And the answer-- yes.
Yes.
I've got five tests, 20% chance
at picking the right one.
Determinants is not good.
The first one is great.
The first one is the good
one for this question
because the eigenvalues.
So the answer is yes.
Yes, this has-- eigenvalues.
So what are the
eigenvalues of S inverse?
1 over lambda?
So-- yes, positive
definite, positive definite.
Yep.
What about-- let me
ask you just one more
question of the same sort.
Suppose I have a matrix, S,
and suppose I multiply it
by another matrix.
Oh, well.
OK.
Suppose-- do I want
to ask you this?
Suppose I asked you about
S times another matrix,
M. Would that be
positive definite or not?
Now I'm going to
tell you the answer
is that the question wasn't
any good because that matrix is
probably not symmetric,
and I'm only dealing
with symmetric matrices.
Matrices have to be
symmetric before I
know they have real eigenvalues
and I can ask these questions.
So that's not good.
But I could-- oh, let's see.
Let me put it in
an orthogonal guy.
Well, still that's
not symmetric.
But if I put the--
it's transpose over there.
Then I made it symmetric.
Oh, dear, I may be getting
myself in trouble here.
So I'm starting with
a positive definite S.
I'm hitting it with
an orthogonal matrix
and its transpose.
And my instinct carried
me here because I know
that that's still symmetric.
Right?
Everybody sees that?
If I transpose this, Q
transpose will come here,
S, Q will go there.
It'll be symmetric.
Now is that positive definite?
Ah, yes.
We can answer that.
Can we?
Is that positive definite?
So remember that this
is an orthogonal matrix,
so also, if you wanted me to
write it that way, I could.
And what about
positive-definiteness
of that thing?
Answer, I think, is yes.
Do you agree?
It is positive definite?
Give me a reason, though.
Why is this positive definite?
So that word similar, this
is a similar matrix to S?
Do you remember what similar
means from last time?
It means that sum
M and its inverse
are here, which they are.
And so what's the
consequence of being similar?
What do I know about a
matrix that's similar to S?
It has--
AUDIENCE: Same [INAUDIBLE]
GILBERT STRANG:
Same eigenvalues.
And therefore, we're good.
Right?
Or I could go this way.
I like energy, so
let me try that one.
x transpose, Q transpose, SQx--
that would be the energy.
And what am I trying to show?
I'm trying to show
it's positive.
So, of course, as
soon as I see that,
it's just waiting for me to--
let Qx be something
called y, maybe.
And then what will this be?
AUDIENCE: y [INAUDIBLE]
GILBERT STRANG: y transpose.
So this energy would be the
same as y transpose, Sy.
And what do I know about that?
It's positive because
that's an energy in the y,
for the y vector.
So one way or another,
we get the answer yes
to that question.
OK.
OK.
Let me introduce the
idea of semidefinite.
Semidefinite is the borderline.
So what did we have?
We had 3, 4, 4.
And then when it was 5,
you told me indefinite,
a negative eigenvalue.
When it was 6, you told me
2 positive eigenvalues--
definite.
What's the borderline?
What's the borderline there?
It's not going to be an integer.
What do I mean?
What am I looking
for, the borderline?
So tell me again?
AUDIENCE: 16 over--
GILBERT STRANG: 16/3,
that sounds right.
Why is that the borderline?
AUDIENCE: [INAUDIBLE]
GILBERT STRANG: Because
now the determinant is--
AUDIENCE: 0.
GILBERT STRANG: 0.
It's singular.
It has a 0 eigenvalue.
There's a 0 eigenvalue.
So that's what
semidefinite means.
Lambdas are equal to 0.
Wait a minute.
That has a 0 eigenvalue
because it's determinant is 0.
How do I know that the other
eigenvalue is positive?
Could it be that the
other ei-- so this
is the semidefinite
case we hope.
But we'd better
finish that reasoning.
How do I know that the other
eigenvalue is positive?
AUDIENCE: Trace.
GILBERT STRANG: The
trace, because adding
3 plus 16/3, whatever
the heck that might give,
it certainly gives
a positive number.
And that will be
lambda 1 plus lambda 2.
That's the trace.
But lambda 2 is 0.
We know from this it's singular.
So we know lambda 2 is 0.
So lambda 1 must be 3 plus 5--
5 and 1/3.
The lambdas must be 8 and
1/3, 3 plus 5 and 1/3, and 0.
So that's a positive
semidefinite.
If you think of the
positive definite matrices
as some clump in matrix space,
then the positive semidefinite
definite ones are sort of
the edge of that clump.
There the boundary of
the clump, the ones
that are not quite inside
but not outside either.
They're lying right on the edge
of positive definite matrices.
Let me just take a--
so what about a
matrix of all 1s?
What's the story on that
one-- positive definite, all
the numbers are positive,
or positive semidefinite,
or indefinite?
What do you think here?
1-1, all 1.
AUDIENCE: Semi--
GILBERT STRANG: Semidefinite
sounds like a good guess.
Do you know what the eigenvalues
of this matrix would be?
AUDIENCE: 0 [INAUDIBLE]
GILBERT STRANG: 3, 0, and
0-- why did you say that?
AUDIENCE: Because 2 [INAUDIBLE]
GILBERT STRANG: Because we
only have-- the rank is?
AUDIENCE: 1.
GILBERT STRANG: Yeah,
we introduced that key
where the rank is 1.
So there's only one
nonzero eigenvalue.
And then the trace tells
me that number is 3.
So this is a positive
semidefinite matrix.
So all these tests change
a little for semidefinite.
The eigenvalue is
greater or equal to 0.
The energy is greater
or equal to 0.
The A transpose A-- but
now I don't require--
oh, I didn't discuss this.
But semidefinite would
allow dependent columns.
By the way, you've
got to do this for me.
Write that matrix as A
transpose times A just
to see that it's
semidefinite because--
so write that as A
transpose A. Yeah.
If it's a rank 1 matrix, you
know what it must look like.
A transpose A, how many terms
am I going to have in this?
And now I'm thinking back to the
very beginning of this course
if I pulled off the pieces.
In general, this is lambda 1
times the first eigenvector,
times the first
eigenvector transposed.
AUDIENCE: Would it just
be a vector of three 1s?
GILBERT STRANG: Yeah, it would
just be a vector of three 1s.
Yeah.
So this would be
the usual picture.
This is the same as the
Q lambda, Q transpose.
This is the big fact for
any symmetric matrix.
And this is symmetric,
but its rank is only 1,
so that lambda 2 is
0 for that matrix.
Lambda 3 is 0 for that matrix.
And the one eigenvector
is the vector 1-1-1.
And the eigen-- so this
would be 3 times 1-1-1.
Oh, I have to do--
yeah.
So I was going to do 3
times 1-1-1, times 1-1-1.
But that gives me 3-3-3.
That's not right.
AUDIENCE: Normalize them.
GILBERT STRANG: I have
to normalize them.
That's right.
Yeah.
So that's a vector whose
length is the square root of 3.
So I have to divide by
that, and divide by it.
And then the 3 cancels
the square root of 3s,
and I'm just left
with 1-1-1, 1-1-1.
Yeah.
AUDIENCE: [INAUDIBLE]
GILBERT STRANG: So
there is a matrix--
one of our building-block
type matrices because it only
has one nonzero eigenvalue.
Its rank is 1, so it could
not be positive definite.
It's singular.
But it is positive semidefinite
because that eigenvalue
is positive.
OK.
So you've got the idea of
positive definite matrices.
Again, any one of
those five tests
is enough to show that
it's positive definite.
And so what's my goal next week?
It's the singular value
decomposition and all
that that leads us to.
We're there now,
ready for the SVD.
OK.
Have a good weekend,
and see you--
oh, I see you on
Tuesday, I guess.
Right-- not Monday
but Tuesday next week.
