A Direct Proof of the Riemann Hypothesis - Part 2: What is the Riemann Hypothesis?

Joseph Lister
3 followers
Good evening, mathematicians and lay mathematical enthusiasts.
Good to have you joining me in this second video.
If you haven't watched the first, you might want to go find
Direct Proof of Riemann Hypothesis Part 1.
Okay? If you've already watched that, then you know
what this one is going to be about.
All right. Again, my name is Jeff Cook,
and about a year and a half ago, I approached Greg Bulk
and Dennis Allen with some
discovery I made, and
this paper that is in preprint now
is the result of a year and a half
of work, of hammering on it, banging away at it.
Have another mathematician look at it.
It is entitled A Direct Proof of the Riemann Hypothesis.
Okay. You can find this preprint by
going to Google, do a search for ResearchGate
Cook Riemann Hypothesis, and it should be the
first link that comes up. You should be able to get the PDF
from there. You do not need
to be a member of ResearchGate to download it.
It is public. If you can't find it
on Google, just kind of
go to ResearchGate.net and do a search
by my name, Jeffrey Cook, or Dennis Allen. Greg Allen
is not there. If you want a little bit more background,
go watch the first video, Background on Us,
or you can check out some
of my and Dennis'
research there if it is public. I am not sure
if all of this is public, but I do believe his profile is.
Okay. Good. All right. Before we get in,
as you know from my other videos, I am a big fan
of dark humor, like Joseph Heller, Catch-22,
all of this. I really like
looking at the world this way because, you know, when something
is not allowed to be laughed at, it just
makes it all the funnier. Okay. So,
if you're interested in that as well,
I am not only into math. I think
the world doesn't need any more stuffy mathematicians.
We have computers for that. If you want a good laugh, please do
check out Woe to the Hunted, the second edition.
It is available at Amazon and
pretty much everywhere else. Okay. It does have
some good reviews from top reviewers at Amazon.
So, Grady Harp is a Hall of Fame
top 50 reviewer. He writes, Jeff Cook pounces
on the literary scene with a fascinating first novel
that is one of the more interesting concepts in storytelling to grace
bookshelves in some time. It is not only
my first novel, it is my only novel. So, I am mainly
into nonfiction, but I do love literary
fiction, particularly dark humor. Daniel Jolly,
super nice guy, and Hall of Fame, Vine Voice
gave five stars, and he writes
Jeff Cook's first novel. Really stands out from the crowd in terms of both
originality and excellent, insightful
writing. Thank you. Alright. I do have another
book. It is nonfiction. It covers, it's called In Light of What
We Are. It covers about everything
kind of from ancient
concept of light to today
and even covers a little bit on Einstein
and his concept of matter
being the condensation of electromagnetic fields.
Also, a lot on Faraday,
Maxwell, and Euler. Also, who
I spoke about in the last video.
A lot about Euler as well. As you know, I love Euler.
Anyway, cool.
Alright, part two.
The Riemann Hypothesis. In the last
video, we were talking about prospecting
for gold, particularly in mathematics.
Okay, so, the sieve of
rap, and if you remember from the video, I'm glad this is the last time
I have to mention this. Eratothenes.
I don't even know how to say his name. I don't care.
He didn't know how to say my name either.
Alright, it's Jeff Cook.
In this part, we're going to get into
the Riemann Hypothesis itself.
I'm going to cover, there are many videos out there
on the zeta function. There are many videos out there
on the Riemann Hypothesis, but none that
I could reference
to give the background of where
we go with the proof.
So, like, Euler was prospecting for his
findings in one area, and everyone else is prospecting
for the Riemann Hypothesis, proof of the Riemann
Hypothesis in other areas, I went a different direction.
So, I kind of have to give
a little background on the Riemann Hypothesis that touches
on the areas where we go.
So, there is a lot of ground
to cover. I'm not going to cover the areas that do not
lead up to the proof.
But, what is...
Oh, before we get into the Riemann Hypothesis...
So, in the last video, also, we kind of got up to
the Riemann zeta function, which is
the analytic continuation of the generalization
of the harmonic series. So, the generalization
of the harmonic series, if you didn't watch the last video, is this.
And this is the Euler product of it,
where he used something like the
Ziv of, and I'm not going to say his name,
and in his paper on the number
of primes less than a given magnitude, Riemann
came up with what is often called
the functional equation of the Riemann zeta function.
And it is a product of five different functions.
2 to the power of s times pi to the power of s minus 1
times psi of pi times s over 2
times the gamma function of 1 minus s, which I'm going to
touch on a little bit in this video, and
times the zeta of 1 minus s. And this relationship
between s and 1 minus s is going to be very
important, as you see. So, what is the Riemann Hypothesis?
If you go to any other video, or pretty much
any paper, Wikipedia, you're going to see the statement
the Riemann Hypothesis is that
all the non-trivial zeros of the Riemann zeta function
have a real part 1 half. I might call that
into question a little bit and say that
this statement is an equivalent consequence to the Riemann
Hypothesis, and you will see why.
Alright, let's talk a little bit about
analytic continuation.
Now, I have this belief
that given enough time and the proper
resources, any problem can be solved.
So, how much time did it
take for me to make this discovery
and then to be able to etch out a proof
with these other co-authors? 17 years
for me. 17 years. And many of those were
24-7, 365.
Okay, waking up at 4 in the morning, going to bed at 3,
you know, just getting 2 hours. A little bit obsessive
for many of the years. And then sometimes 10 months off.
But I did look at it for about that long.
And what I found
fairly recently, like I said about 2 years ago,
a year and a half to 2 years ago,
I started becoming clear of what I needed.
I needed a new resource. Not a new,
not some new mathematics, but
something you will see as we go. Now, let's talk a little bit
about the resources that Riemann had.
He did have the Abel-Plana formula, where you can
take certain
functions, f of n,
and when you need to know
the sum of them from n equals 0 to infinity,
many times, many functions will work. We can apply
them to this formula, which I'm going to show you here.
And at the top, up here,
is the Abel-Plana continuation of the Riemann
zeta function. So, any argument we want to apply
at s, s here, s here, it's going to give us some
output, right? So, how does this
formula work? It's very big. It produces
very large, I mean, it's, I mean, look, it's
pretty clunky, you know, equation.
But it's also very manageable.
And the fact that it gives any output
for any input is very nice. Do I? Alright.
In other words, it converges for all s. It's an entire function.
Except for s equals 1. So, how does it work?
Alright, so, f of n would be, in this
case, n to the power of minus s.
And they're asking us to put
n equals 0 there. Well, we could turn
this n equals 0 and change this to n plus 1.
And this was discovered
by Plana in 1826 and about 10-15
years later by Abel, and Riemann wrote his paper
on the number of primes up to a given magnitude
in 1859. So, you see, he did
have this at his disposal.
But this is how it works when we use this, and we're going to
compare it with Riemann's
analytic continuation. Alright.
So, I'm not going to use n to the
power of minus s, okay? I'm not going to. I'm going to use
a different f of n so we can see that it works for just about any.
Alright, and this is
an alternate
form of the generalization of the harmonic
series, okay? Now, my f of n that I came up with,
and I didn't prove it or it's not in the paper, but
I'm using it here just to show how this works. Alright, so my f of n
is not equal to n to the power of minus s,
but as we sum it to infinity, it does result in the same sum.
Alright, so we're going to take this, and we're going to
replace n with x, and we're going to
integrate it, alright? And we're going to end up with
1 over s minus 1, okay?
See how that works? Now we go to the second term, and we're
going to take that. We're going to swap out n
for 0, and we're just going to just consider this to the
right in the red, and everything reduces to 1
at f of 0, and so we just
end up with 1 half in the second term.
And now we're going to do the last one. It's a little trickier,
but nothing you can't handle. We're just going to replace
n with the i t and minus
i t, take the difference of those two functions,
integrate it, and we get the final result
above, okay? So that's how that
works. Neat. Now, in doing this, I'm
particularly interested in this first term.
Now, if you have ever taken a college course,
first-year college course on analytic continuation,
and you probably have seen
this, and you probably use this, or 1 over 1 minus
s, and it's a pretty
easy function to work out with students.
Alright, it is the analytic continuation of
the geometric series minus s to the power of n.
Geometric series converge for the absolute
value of s less than 1, as does this one,
and basically anything geometric series is
anything times s to the power of n. So here we have
minus 1 times s to the power of n. We could do
58 times s to the power of n, whatever it is, and that's
going to come out, that's going to be a geometric series. Alright,
well, why is that interesting? Well, note here
also we can get this really quick, before I go, why it's interesting.
It also, you can get this by integrating
fn in the traditional sense of n to the power of minus s.
But why is this interesting to me?
Alright, so if Euler was
kind of like you saw last video,
and if not, go listen to it for this analogy, because I'm going to carry
it through a little bit. So if Euler is a
kind of, how would you say,
kind of approaches mathematics like a gold prospector
would, and other mathematicians have as well.
Riemann,
he does things a little differently.
He's going for a different result, and right now we have
a very different problem. Alright, so Riemann
hypothesis is a very different problem, and we're going to show it.
So I'm going to give an introduction before I show how this is done. I'm going to give you
the insight that I had into this.
If this is a big, chunky rock,
and it has gold in it, I don't see any primes, right?
So if it has gold in it,
then I want to
break this apart a little. I want to chip away at this
to reveal the gold beneath.
Alright, now the zeros of the zeta function, as you're going to learn,
relate to the prime numbers.
And so I think you can consider both of them
as significant and valuable, something we're looking for.
Alright, so we're going to chip away out of here,
break off a piece, and this is showing what's underneath.
We see that geometric series.
Now this is the way I see it. Alright, so I'm flipping back
between these two, and I see this as
chipping away the irrational functions
and irrational properties of this functional equation.
And what I want to do is chip it away to leave
just the skeleton of this function underneath.
And when I look at the Apoplano formula
in comparison, I see
geometric series underneath.
I understand there are rational functions,
1 over s minus 1 is analytic continuation of geometric series,
but I see that in there. And yes, of course, 2 is not
a function. Maybe there's something else that cancels out that leads to
here. And what my thought is,
after going down every other road,
is what if we just keep chipping this away and take all of these rational
functions and put them into
one function, and leave that
function an algebraic factor
of the zeta function. And maybe
if we can do that, it can tell us something about the zeros.
Maybe we will see the gold underneath. And indeed, that is what we
get. Alright, so
by returning to Riemann's functional
equation, we have to understand what we're dealing with here.
Alright, so when he gets his functional equation, what do you think
the first number he'd apply to s
would be? Okay, so it would probably be the first
number ever applied to the generalization
of the harmonic series, which is 2. Alright, so we know
that zeta of 2 equals pi squared over 6,
but applying that to the functional equation,
we end up with minus infinity. It's a little bit of a problem
since how do we say that pi squared over 6
is equal to minus infinity? Okay, so
this is a problem. We know how it's a problem the way
Riemann wrote about it. He didn't just gloss over it
and say, well, we have all of these simple
poles and all of the positive
arguments. No, he wanted to eliminate
it. And I'll show you why I think that's neat and important
because by doing so,
he was led to the Riemann hypothesis
and his final result. So let's see what he did.
Alright, so in order to
do this, he had to not eliminate the gamma
function, but do something which you might think
is more ingenious, but I'm going to say
not really. Anyone could do it, and you're going to do it right about
now. Alright, so take a look. We're finding out where the
problem is. The problem is the gamma function of 1
minus s, which happens to equal the factorial of minus
s, which ends up being minus infinity
for all natural numbers greater than 0.
Alright, so what does he do? Well, everything you're going to do right now
is pick a number between 0 and 1.
The number that comes to mind is 1 half, doesn't it?
I think so. Maybe you're thinking
of maybe some other number between 0 and 1 like the Euler-Mascaroni
constant. I don't know. Probably not. Probably
you're going to say, well, 1 and 2 and 3
and all of these don't work, but maybe right down the middle, let's go
try those. Of course, we know that gamma function converges
for these, and so
what is the gamma function of 1 minus 1 half?
It is the square root of pi. Now, I have
a hunch that he was going to try to
reapply this square root of pi in there to cancel
out the pi's, get them out of the way, also
maybe reduce this to purely rational
functions, but it's not that
easy, and what he got stuck at is something
far more important and far more beautiful, and that
is this. Alright, so
he took S, he divided it by 2 for all, and he's just
redefining the function here by dividing S's
by 2 in this way, and what he found is that
this function cannot see the difference between
S and 1 minus S.
They end up being the same. So this function
doesn't care. You can plug in S or 1 minus
S, and it's going to give you the same result, and
why is that so extremely important?
Because it says that the
zeros of the zeta functions are reflections
of each other through the real point 1 half
right here. So, if this is over here,
rho h is a hypothetical
non-trivial zero. We draw a line between
it and this other hypothetical non-trivial
zero, 1 minus rho h. We're going to go right through the
point 1 half. See that? And of course, with any
complex number, you have this complex conjugate,
and it's going to go to his little
partner over here, right through the real point
1 half. Now, let's give a little background
on complex arithmetic really quick for anyone who's
coming here and going, I have no idea what I'm looking at here.
Alright, you know all
of the numbers, right? The real numbers.
1, 0, 1, 2, 3,
minus 1, 1 half.
Pi is a real number, so pi would be somewhere
on the real line just past 3 somewhere.
Okay? So those are all real numbers, and you've seen
these number lines. Alright, so a complex number has two parts.
Think of it as a combo. Alright, it's a combination.
Two parts. A real part and an imaginary
part. And this imaginary, calling it an imaginary
part is a very bad term, but you will get used to it.
So a complex number has a real part
plus an imaginary part. And what makes it imaginary?
It's multiplied by the letter i.
And the letter i is equal to the
square root of minus 1. Does it have a value? No, there's
no value for the square root of minus 1. We just call it i.
So, anything, any real
number plus an imaginary number is a complex
number. And with those complex numbers, we can do
anything that we can do with real numbers.
Add, subtract, raise to powers, all of that.
We can do so much more. So instead of plotting on a real
line a complex number, we count over its real part
and then up or down its imaginary part.
So, let's suppose we have
a number, a complex number, 1
plus i1, or 1 plus i.
Okay? So we would just simply count over 1 and up
1. And we put a little point there and say that number
is plotted on the complex plane. So,
real 1 is also on the complex plane right here.
And the real number 1 half
is right here. And 0 is here and so on and so forth.
So, this area between 0
and 1 is a very important area
in terms of the Riemann Hypothesis. It's called
the critical strip. And so you imagine
this area going all the way up to
positive imaginary infinity and all the way down to
negative imaginary infinity. And it's all within that
area of, between
0 and 1. Now, the dead
center of that critical strip is called the
critical line, obviously, because it's kind of centered.
And it's, all of these would have a real part
1 half. Okay? So they have
a real part 1 half. So let's say we go over a real part
1 half plus i. Then we count up 1.
So we plot it right around here somewhere.
Okay? So every complex number has what's called the complex
conjugate. So, if this is 1 third
plus 1 fifth, well then 1 third minus
1 third plus i 1 fifth and
1 third minus i fifth would be its complex conjugate.
I'm just kind of guessing based on where we're looking at here.
And we denote its complex
conjugate by putting this little line over the top of it.
Alright? So, we see the importance
of that function right here.
This equality. Because we can
actually, and we're going to show how, see the
relationship between the zeros
of the zeta function.
Now, they're not just the
zeros. Alright? So, there's apparently
in Mathematics there's many types of zeros.
They're not just zeros. Alright? So,
there are certain types of zeros
that are referred to as roots.
And these tell a lot about the function itself.
And in the case of the zeta function,
the roots tell us a lot about the prime numbers.
Alright? Now, there are other zeros.
They look like zeros, but they're not non-trivial
zeros. Alright? So, they look just like a zero.
They arrive at the negative even
integers. Minus 2, minus 4, minus
6, all the way out there. Those also
send the zeta function to 0, but they tell us
nothing about the prime numbers. Okay? So, you see the
little difference. Those are called the trivial zeros.
The non-trivial zeros are
all in the critical strip.
Okay? And so far today, all of them
are known to have a real part
one-half. So, that's where
people get the equivalent consequence of that
statement, of the real part all in one-half.
We're going to show you what the Riemann hypothesis
actually states, which, again, is interesting
if you want to take the search for prospecting
in a different area. Alright. The Riemann hypothesis
is that t is real whenever
xi of t equals 0. Well, there's no t in there, so what am I talking
about? Well, so he liked this function so much,
you know, he kind of, a little modification
multiplied by s minus 1. But he
defined this as xi function. He
demanded and mandated that all of the real parts
of s equal one-half, and then he
defines xi over a function of
t. So, t is the input. And t could be real.
t could be a complex number. It could
be, I don't know, quaternion. It could be any number.
Alright? But it's that number that is multiplied by i
in this thing. Now, why
is this a very important equation?
Particularly to Riemann, and
it should be to you as well. Solve for the imaginary
part of t, and come back at about
pause this video, and come back at about a thousand years
when you've realized that there are no solutions.
Actually, it didn't take a thousand years. By the rules of
complex arithmetic, you can determine
that there
are no solutions exist.
And so, I'm not going to go ahead and rearrange
to show you because I'm going to do it in a different way with something new
in the next video. Okay? So we're going to remember
this equation, how very important it is,
and we're going to do something similar which will lead
to the proof. Alright? So the hypothesis
then is that, you know, he
demanded that the real part equals one-half.
Alright. He defined, and his
final result will end up having the real part in there.
But, the
hypothesis is that, I'm being
distracted by coffee, I'm sorry. The hypothesis
is that t is real for all of the
zeros of psi. Okay? So there's zeros
of the zeta function, and there's zeros of
the psi function. And there's also trivial
and non-trivial. In fact, psi of t shares
all of the trivial and non-trivial zeros. It is just
the multiplicative factor of the zeta function. But
this is the function that is of most interest
to Riemann, and it is because of this property
how the imaginary part ends up being equal
to zero when the real part of S equals
one-half. Alright? Now.
Okay. So.
Makes sense? Are you lost?
Well, just remember that you can't be found until you're first lost.
So, you'll be found. Don't worry. Let's first ask
the question, why might t be real
when psi of t equals zero? Why does he suspect it?
At this point in the paper, he didn't have his final result.
He went on to explain. You can't have a hypothesis
without a reasoning. So, you can't just say,
I believe that, you know, big newtons will grow wings
and fly to the moon. Okay? Why?
Well, you have to have a reason why. So, his reason why was this.
A value of S whose real part is greater than one
and log of zeta function of S equals minus
sum of log times one minus pi to the power of minus S
p to the power of minus S, sorry, not pi
remains finite, and since the same holds for the logarithms
of the other factors of psi of t, psi of t only
vanishes with this region minus
i over two and i over two.
If you weren't lost before, come on and admit it.
Alright, I'm going to just kind of summarize a little bit of this.
Alright, so the Riemann hypothesis is
a hypothesis on absolutes.
Okay, what is the dead center region between here?
Alright, forget all this. I didn't mean to do all this.
What is the dead center region? Alright?
It is zero. Alright? So, if the imaginary
part goes to zero, that complex
number becomes real. Alright? So, we can plot real numbers on the
complex plane, but the dead center is
zero.
Now, there's some
So, he's saying that the building blocks of everything
that is going to lead to all of, connect the zeros
to the primes, all of that is going to be
an absolute. It's not going to balance. It's
symmetric, but it's only going to be symmetric on
the dead center of zero. Alright? Yes,
it's in this region. You know, you can prove that it's within this
region, and that region connects to the critical
strip of the zeta function,
but how do you prove it? That's his question.
He worked on it a little bit, and like I said
before, I do believe he had all of the resources
at hand to prove the Riemann hypothesis,
but I don't believe he applied
enough time to it. So, remember I said I believe that
having enough resources and enough time, you can solve
any problem. And like Euler,
it's just a matter of kind of sometimes getting lucky
or having the right resources. I think it has
to do with having the right resources. So, this is
Riemann's final result. Pretty
big equation. Very important.
Alright, this is his, I guess you could say,
equivalent to prime counting function. We can give x
any value, and it's going to output the number of primes up to
that value. Isn't that amazing? I think
it is. And let's kind of break it down one
term by term. Okay, so the
first term here is the logarithmic integral, and
you see it's nothing you can't handle. It's just
an integral. You can plug this into any online calculator, and it's
going to give you a value if you apply
x to here. So, you integrate up to x, and it's
going to give you some value. Alright, we also have
the logarithmic integral in the second term,
and this is the one to look at.
Alright, so these halves, you saw
them in the other,
they're cemented in. You can't change them.
Alright, they're locked in. Alright, we can't
manipulate them, call them, give them another real part,
nothing. Alright, so what is
alpha here? Those are the roots of xi function.
Alright, and he says that
he thinks they're all real. That's the Riemann hypothesis.
Alright, he believes alpha is always real.
Got it? But here,
he's not saying that. He's just saying, I just know that this
works. So he's going to start applying, and he knows because he found
the first few of them, so he was able to
see that his function worked.
Also, because this first term
is so very close already to the
prime counting function. Immediately
you add this other sum, and you're going to, this is the second
term, and you're going to
get closer, and before I get
to these next two terms, let's talk a little bit more about this.
Alright, so you take all of the zeros
and you add
some of these two logarithmic integrals.
You got the complex number, and you got the complex conjugate.
See, 1 half plus i alpha,
and then 1 minus s, you know,
is equivalent in this sense. So we have to do the complex conjugate
1 over 2, 1 half
minus i alpha. And we're going to add those
together, and for every alpha, we're going to sum
that to infinity, or at least he doesn't know if there's
an infinite number of non-trivial zeros, but for all the zeros that they
are, are going to add up and give them some value,
and we're going to add this to
that. Now, let's continue.
The next term, I'm not going to get into it.
There's some elements of trigonometry
in this, actually. I'm not going to get into it here, but I may do another video on it.
And this is very closely related
to the logarithmic integral as well.
But we're not going to get into it
too much, because we don't have too much time.
But the value that is output from here is very small, and it
works very rapidly. This term, I do want to talk a little bit.
Now, you remember when we did the Abel-Plana
continuation, and it asked for, we let go of
n, and we made it equal to zero.
A lot similar way is
resulting here in his analytic continuation,
where he has xi of zero. So we drop out
its value of t,
which we remember, and we're going to just replace
t with zero, and its value
is one-half. Okay, so
the log of one-half also is equal to
minus log of two, which
isn't terribly interesting, except
that that is how mathematicians
today have replaced the xi
function, sent it offstage left,
and to replace it with the zeta function.
And this is the result of doing that.
Pretty neat. We can,
instead of taking the zeros of the xi function,
we now can take the zeros of the zeta function,
which we're going to give a name, call them rho.
Alright, so now we're not making
the assumption the real part in there is one-half,
because we don't know for sure at this point.
So we're just calling them rho. We do know that
all of the roots
do have real part one-half up until the trillions.
I think they're now coming up with so many of them.
So we do know a lot of them
have real part one-half far enough
towards infinity that we can at least calculate
our number of primes less than a given magnitude.
Okay, so does that make sense?
Got it? Alright, so again,
it's kind of like the analytic continuation,
we're stuck with all these terms that give a result
for any argument x.
But what he has done here,
this is the big thing, the gold is in here,
the prime numbers, now he knows the number of primes
up to a given magnitude. Very important.
And what did he connect it to? The zeros of the zeta function.
Alright? The zeros of the zeta function
relate to the prime numbers, namely the number of primes.
But if you know the number of primes,
you can actually manipulate to find if a number is prime or not.
So it's just a matter of basic arithmetic at that point.
But knowing them up to a very large number is complicated
solved with this wonderful equation.
Alright? Make sense?
Alright, how do you prove it?
How do you prove the Riemann Hopf balance?
That I'll have to show in a different video.
Thank you so much. Please check the next video.
That is where it's going to have all of the information that is new.
This right here is a review of the hypothesis
and the history of the zeta function.
The next video, we're going to get into the result that leads to the proof.
And I thank you so much for watching.
