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Presentation of the work on Prime Numbers. intended for mathematics loving people. Please send comments and suggestions for improvement to [email protected]. More presentations can be found in my website at http://solohermelin.com.
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1
Prime Numbers
SOLO HERMELIN
Updated: 28.10.12 : 12.09.13
2
SOLO
Table of ContentPrimes
Euclid, Euclidean DivisionIntroduction
Prime NumbersEuclid's LemmaFundamental Theorem of ArithmeticPrime Numbers FormulasEuler Zeta Function and the Prime History
Prime Number DistributionPrime Number Theorem (PNT)History of the Asymptotic Law of Distribution of Prime NumbersThe Chebychef Contribution
The Chebyschev Functions (1851)The Chebyschev’s First EstimateThe Chebyschev’s Second Estimate
Riemann's Zeta Function (1859)Riemann Zeta Function ZerosRiemann's Zeta Function PropertiesVon Mangoldt Psi FormulaRiemann's Zeta Function Relations
Abel’s Method of Partial Summation
11 1 1
xdx
xxs
s
ss
s
Möbius Function
3
SOLO
Table of Content (Continue – 1)Primes
The Riemann Prime Number FormulaHadamard Proof of the Prime Number Theorem (1896)Newman’s Proof of the Prime Number Theorem (1980)References End of Presentation
4
SOLO
Table of Content (continue – 2)Primes
AppendicesDefinitionsMellin TransformProof of Riemann's Zeta Function Relations
1Re10
1
zxfordte
tzz
t
tt
z
0
0
1
1sin2
1 i
i
z
de
izz
z
0
0
1
12
sin221
i
i
zz
zz
ide
0
0
1
12
1 i
i
z
dei
zz
zzzzz z
1
2sin22sin2
zzzz zz 112/sin2 1
z
z
z
z zzzz
1
2/12/ 12/12/
Bernoulli Numbers Zeta-Function Values and the Bernoulli Numbers
Zeros of Zeta-Function: ζ (z) = 0
1,1ln1
2ln
12ln
2
1
1
1
2
xasxnnx
xn
n
O
5
SOLO
Table of Content (continue – 3)Primes
Appendices
11
11
1
1
tispn
sprimep
sn
s
Zeta Function ζ (s) and its Derivative ζ‘ (s)
11
1
tizduuuz
z
zzd
d
z ReRe
ic
ic
z
zdz
x
z
z
ix
'
2
1
1,
1ln
2
tisxdxx
xss
s
primepxp
xprimesofnumberx 1:
Hadamard Product of ζ (s)
Perron’s Formula
Auxiliary Tauberian Theorem
Infinite Series
Series of Functions
Absolute Convergence of Series of Functions
Uniformly Convergence of Sequences and Series
6
SOLO
Table of Content (continue – 4)Primes
Appendices
Infinite ProductsThe Mittag-Leffler and Weierstrass Theorems
The Weierstrass Factorization Theorem
The Hadamard Factorization Theorem
Mittag-Leffler’s Expansion Theorem
Generalization of Mittag-Leffler’s Expansion Theorem
Expansion of an Integral Function as an Infinite Product
The Hadamard Factorization Theorem
Hadamard Infinite Product Expansion of Zeta FunctionIntegrationPrime Number Applications
7
SOLO
Introduction
Primes
The start point of this presentation was the book of Marcus de Sautoy , “The Music of the Primes”, 2003, Harper Collins Publisher, which I read during a recreation trip to Crete. The subject was new for me, so to study this topic I turned to the Internet, where I found many related articles. I spend a lot of time trying to partially cover the subject, and this Presentation is the result. It contains no original contributions, but clarifications, in my opinion, of some of the topics.
In order to obtain a coherent presentation and complete some of the proofs more work needs to be done
Return to TOC
8
SOLO Primes
EuclidEuclid ( Eukleidēs), 300 BC, also known as Euclid of Alexandria, was a Greek mathematician, often referred to as the "Father of Geometry". He was active in Alexandria during the reign of Ptoleme I (323–283 BC). His Elements is one of the most influential works in the history of mathematics, serving as the main textbook for teaching mathematics (especially geometry) from the time of its publication until the late 19th or early 20th century. In the Elements, Euclid deduced the principles of what is now called Euclidean geometry from a small set of axioms. Euclid also wrote works on perspective, conic sections, spherical geometry, number theory and rigor.
Euclid" is the anglicized version of the Greek name Εὐκλείδης, meaning "Good Glory".
Euclid of Alexandria Born: about 325 BCDied: about 265 BC
in Alexandria, Egypt
9
SOLO Primes
Euclidean Division
In mathematics, and more particularly in arithmetic, the Euclidean division is the usual process of division of integers producing a quotient and a remainder. It can be specified precisely by a theorem stating that these exist uniquely with given properties.
Given two integers a and b, with b ≠ 0, there exist unique integers q and r such that a = bq + r and 0 ≤ r < |b|, where |b| denotes the absolute value of b
Statement of the Theorem
Proof1. Existence
Statue of Euclid in the Oxford University Museum
of Natural History
Consider first the case b < 0. Setting b' = −b and q' = −q, the equation a = bq + r may be rewritten a = b'q' + r and the inequality 0 < r < |b| may be rewritten 0 < r < |b' |. This reduces the existence for the case b < 0 to that of the case b > 0.Similarly, if a < 0 and b > 0, setting a' = −a, q' = −q − 1 and r' = b − r, the equation a = bq + r may be rewritten a' = bq' + r' and the inequality 0 < r < b may be rewritten 0 < r' < b. Thus the proof of the existence is reduced to the case a ≥ 0 and b > 0 and we consider only this case in the remainder of the proof.Let q1 and r1, both nonnegative, such that a = bq1 + r1, for example q1 = 0 and r1 = a. If r1 < b, we are done. Otherwise q2 = q1 + 1 and r2 = r1 − b satisfy a = bq2 + r2 and 0 < r2 < r1. Repeating this process one gets eventually q = qk and r = rk such that a = bq + r and 0 < r < b.This proves the existence and also gives an algorithm to compute the quotient and the remainder. However this algorithm needs q steps and is thus not efficient.
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SOLO Primes
Euclidean Division
In mathematics, and more particularly in arithmetic, the Euclidean division is the usual process of division of integers producing a quotient and a remainder. It can be specified precisely by a theorem stating that these exist uniquely with given properties.
Given two integers a and b, with b ≠ 0, there exist unique integers q and r such that a = bq + r and 0 ≤ r < |b|, where |b| denotes the absolute value of b
Statement of the Theorem
Proof (continue)
2. Uniqueness
Statue of Euclid in the Oxford University Museum
of Natural History
Suppose there exists q, q' , r, r' with 0 ≤ r, r' < |b| such that a = bq + r and a = bq' + r' . Adding the two inequalities 0 ≤ r < |b| and −|b| < −r' ≤ 0 yelds −|b| < r − r' < |b|, that is |r − r' | < |b|.Subtracting the two equations yields: b(q' − q) = (r − r' ). Thus |b| divides |r − r' |. If |r − r' | ≠ 0 this implies |b| < |r − r' |, contradicting previous inequality. Thus, r = r' and b(q' − q) = 0. As b ≠ 0, this implies q = q' , proving uniqueness.
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11
SOLO Primes
Prime Numbers
Prime Number Definition:A positive integer number p is prime if for all positive integers 1≤ a ≤p, we have for all the Euclidean Divisions
p = a q + rthe reminder r = 0 only for (q=p, a=1) or (q=1, a=p).A Prime Number is divisible only by 1 or by itself.
Proposition 20, Book IX of the Euclide’s Elements: “There are Infinitely many Primes”
Euclid's proof
Consider any finite set S of primes. The key idea is to consider the product of all these numbers plus one:
Sp
pN 1
Like any other natural number, N is divisible by at least one prime number (it is possible that N itself is prime).
None of the primes by which N is divisible can be members of the finite set S of primes with which we started, because dividing N by any of these leaves a remainder of 1. Therefore the primes by which N is divisible are additional primes beyond the ones we started with. Thus any finite set of primes can be extended to a larger finite set of primes.
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SOLO Primes
Prime Numbers
2 3 5 7 11 13 17 19 23 29 31 37 41 43 47 53 59 61 67
71 73 79 83 89 97 101 103 107 109 113 127 131 137 139 149 151 157 163
167 173 179 181 191 193 197 199 211 223 227 229 233 239 241 251 257 263 269
271 277 281 283 293 307 311 313 317 331 337 347 349 353 359 367 373 379 383
389 397 401 409 419 421 431 433 439 443 449 457 461 463 467 479 487 491 499
503 509 521 523 541 547 557 563 569 571 577 587 593 599 601 607 613 617 619
631 641 643 647 653 659 661 673 677 683 691 701 709 719 727 733 739 743 751
757 761 769 773 787 797 809 811 821 823 827 829 839 853 857 859 863 877 881
883 887 907 911 919 929 937 941 947 953 967 971 977 983 991 997
Here is a list of all the prime numbers up to 1,000:
13
SOLO Primes
Run This
Return to TOC
14
SOLO Primes Euclid's Lemma
In number theory, Euclid's lemma (also called Euclid's first theorem) is a lemma that captures one of the fundamental properties of prime numbers. It states that if a prime divides the product of two numbers, it must divide at least one of the factors. For example since 133 × 143 = 19019 is divisible by 19, one or both of 133 or 143 must be as well. In fact, 19 × 7 = 133. It is used in the proof of the fundamental theorem of arithmetic.
Let p be a prime number, and assume p divides the product of two integers a and b. Then p divides a or p divides b (or perhaps both).
Divisibility Definition: Assume a ≠ 0 and let b be any integer. If there is an integer q such that b = a.q, a is said to divide b; a is a divisor of b and b is a multiple of a. Notation of a divide b is a|b.
The lemma first appears as proposition 30 in Book VII of Euclid's Elements. It is included in practically every book that covers elementary number theory
Proof:
211221212211
222
111
rrrmrmpmmprpmrpmba
prrpmb
prrpma
Using Euclidean Division Theorem
Since p|a.b we must have r1.r2=0 meaning r1=0, or r2=0, or r1=0 and r2=0.
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15
SOLO Primes
Fundamental Theorem of ArithmeticIn number theory, the fundamental theorem of arithmetic (also called the unique factorization theorem or the unique-prime-factorization theorem) states (existence) that every integer greater than 1 is either prime itself or is the product of prime numbers, and (uniqueness) that, although the order of the primes in the second case is arbitrary, the primes themselves are not.
Book VII, propositions 30 and 32 of Euclid's Elements is essentially the statement and proof of the fundamental theorem. Article 16 of Gauss' Disquisitiones Arithmeticae is an early modern statement and proof employing modular arithmetic.
Canonical representation of a positive integerEvery positive integer n > 1 can be represented in exactly one way as a product of prime powers:
k
iik
ik ppppn1
2121
Proof of Fundamental Theorem of Arithmetic
Existence
By inspection, each of the small natural numbers 1, 2, 3, 4, ... is the product of primes. This is the basis for a proof by induction. Assume it is true for all numbers less than n. If n is prime, there is nothing more to prove. Otherwise, there are integers a and b, where n = ab and 1 < a ≤ b < n. By the induction hypothesis, a = p1p2...pn and b = q1q2...qm are products of primes. But then n = ab = p1p2...pnq1q2...qm is the product of primes
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SOLO Primes
Fundamental Theorem of Arithmetic
Canonical representation of a positive integerEvery positive integer n > 1 can be represented in exactly one way as a product of prime powers:
k
iik
ik ppppn1
2121
Proof of Fundamental Theorem of Arithmetic (continue)
Uniqueness
Assume that s > 1 is the product of prime numbers in two different ways:
nm qqqppps 2121 We must show m = n and that the qj are a rearrangement of the pi.
By Euclid's lemma p1 must divide one of the qj; relabeling the qj if necessary, say that p1 divides q1. But q1 is prime, so its only divisors are itself and 1. Therefore, p1 = q1, so that
nm qqppp
s 22
1
This can be done for all m of the pi, showing that m ≤ n. If there were any qj left over we would have
which is impossible, since the product of numbers greater than 1 cannot equal 1. Therefore m = n and every qj is a pi.
nmm
qqppp
s
121
1
q.e.d.
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17
SOLO Primes
Marin Mersenne, Marin Mersennus or
le Père Mersenne (1588 –1648)
Mersenne Prime
In mathematics, a Mersenne number, named after Marin Mersenne (a French monk who began the study of these numbers in the early 17th century), is a positive integer that is one less than a power of two: 12 p
pM
Named after Marin Mersenne
Publication year 1636[1]
Author of publication Regius, H.
Number of known terms 47
Conjectured number of terms
Infinite
Subsequence of Mersenne numbers
First terms 3, 7, 31, 127
Largest known term 243112609 − 1
OEIS index A000668
As of October 2009[ref], 47 Mersenne primes are known. The largest known prime number (243,112,609 – 1) is a Mersenne prime.[3] Since 1997, all newly-found Mersenne primes have been discovered by the "Great Internet Mersenne Prime Search" (GIMPS), a distributed computing project on the Internet.
A basic theorem about Mersenne numbers states that in order for Mp to be a Mersenne prime, the exponent p itself must be a prime number. This rules out primality for numbers such as M4 = 24 − 1 = 15: since the exponent 4 = 2×2 is composite, the theorem predicts that 15 is also composite; indeed, 15 = 3×5
While it is true that only Mersenne numbers Mp, where p = 2, 3, 5, … could be prime - and it was believed by early mathematicians that all such numbers were prime[2] - Mp is very rarely prime even for a prime exponent p. The smallest counterexample is the Mersenne number
89x232047121111 M
Prime Numbers Formulas
18
SOLO Primes
Goldbach’s Conjecture
Christian Goldbach (1690 –1764)
Goldbach's conjecture is one of the oldest and best-known unsolved problems in number theory and in all of mathematics. It states:
Every even integer greater than 2 can be expressed as the sum of two primes.
The conjecture has been shown to be correct[2] up through 4 × 1018 and is generally assumed to be true, but no mathematical proof exists despite considerable effort
History:On 7 June 1742, the German mathematician Christian Goldbach (originally of Brandenburg-Prussia) wrote a letter to Leonhard Euler (letter XLIII)[4] in which he proposed the following conjecture:
Every integer which can be written as the sum of two primes, can also be written as the sum of as many primes as one wishes, until all terms are units
He then proposed a second conjecture in the margin of his letter
Every integer greater than 2 can be written as the sum of three primes
The two conjectures are now known to be equivalent, but this did not seem to be an issue at the time
Prime Numbers Formulas
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SOLO Primes
Euler Zeta Function and the Prime History
232 4
1
3
1
2
11
In 1650 Mengoli asked if a solution exists for
P. Mengoli1626 - 1686
The problem was tackled by Wallis, Leibniz, Bernoulli family, without success. The solution was given by the young Euler in 1735. The problem was named “Basel Problem” for Basel the town of Bernoulli and Euler.
Euler started from Taylor series expansion of the sine function
!7!5!3
sin753 xxx
xx
Dividing by x, he obtained
!7!5!3
1sin 642 xxx
x
x
The roots of the left side are x =±π, ±2π, ±3π,…. However sinx/x is not a polynomial, but Euler assumed (and check it by numerical computation) that it can be factorized using its roots as
2
2
2
2
2
2
91
411
21
2111
sin
xxxxxxx
x
x
Leonhard Euler(1707 – 1783)
SOLO Primes
!7!5!3
1sin 642 xxx
x
x
2
2
2
2
2
2
91
411
sin
xxx
x
x
Leonhard Euler(1707 – 1783) If we formally multiply out this product and collect all the x2 terms, we
see that the x2 coefficient of sin(x)/x is
122222
11
9
1
4
11
n n
But from the original infinite series expansion of sin(x)/x, the coefficient of x2 is −1/(3!) = −1/6. These two coefficients must be equal; thus,
1
22
11
6
1
n n 6
1 2
12
n n
Euler extend this to a general function, Euler Zeta Function
,4,3,24
1
3
1
2
11: nn
nnn The sum diverges for n ≤ 1 and
converges for n > 1.
Euler computed the sum for n up to n = 26. Some of the values are given here
,9450
8,945
6,90
4,6
28642
Euler checked the sum for a finite number of terms.
Euler Zeta Function and the Prime History (continue – 1)
SOLO Primes
Euler Product Formula for the Zeta Function
Leonhard Euler proved the Euler product formula for the Riemann zeta function in his thesis Variae observationes circa series infinitas (Various Observations about Infinite Series), published by St Petersburg Academy in 1737
primepx
nx pn 1
11
1
where the left hand side equals the Euler Zeta Function
Euler Proof of the Product Formula
xxxxx
s8
1
6
1
4
1
2
1
2
1
xxxxxxxx
13
1
11
1
9
1
7
1
5
1
3
11
2
11
xxxxxxxxx
33
1
27
1
21
1
15
1
9
1
3
1
2
11
3
1
xxxxxxxx
17
1
13
1
11
1
7
1
5
11
2
11
3
11
all elements having a factor of 3 or 2 (or both) are removed
xxxx
nxn
x5
1
4
1
3
1
2
11
1
1
converges for integer x > 1
all elements having a factor of 2 are removed
Leonhard Euler(1707 – 1`783)
EulerZeta Function and the Prime History (continue – 2)
SOLO Primes
Leonhard Euler(1707 – 1`783)
Euler Product Formula for the Zeta Function
primepx
nx pn
x1
11
1
Euler Proof of the Product Formula (continue)
xxxxxxxx
17
1
13
1
11
1
7
1
5
11
2
11
3
11
Repeating infinitely, all the non-prime elements are removed, and we get:
12
11
3
11
5
11
7
11
11
11
13
11
17
11
x
xxxxxxx
Dividing both sides by everything but the ζ(s) we obtain
xxxxxx
x
131
1111
171
151
131
121
1
1
Therefore
primepx
nx pn
x1
11
1
EulerZeta Function and the Prime History (continue – 3)
SOLO Primes
Leonhard Euler(1707 – 1`783)
Euler Product Formula for the Riemann Zeta Function
primeps
ns pn
s1
11
1
Another Proof:
According to Fundamental Theorem of Arithmetic: Every positive integer n > 1 can be represented by exactly one way as a product of prime powers
integer,21
21 iik primeppppn k
1
211
211
n
s
kn
skppp
ns
primeps
primep k
sk
n
s
kn
s ppppp
ns k
1
11
1121
1
21
Since in the sum n covers all the integers, for each prime there are the powers of al integers k ϵ [1,∞)
EulerZeta Function and the Prime History (continue – 4)
24
SOLO Primes
The Euler zeta function, ζ(s), is a function is the sum of the infinite series
1
1
nxn
x
Let compute
1,ln
1,1
1
1
1
1px
ps
x
dxx
s
s
According to Maclaurin – Euler Integral Convergence Test for Infinite Seriesthe integral and therefore the series are divergent for p ≤ 1, convergent for p > 1.
Leonhard Euler(1707 – 1`783)
Euler Zeta Function and the Prime History (continue – 5)
Euler Zeta Function for x > 1
0823.190
1
2
114
202.11
2
113
645.16
1
2
112
612.22/3
1
2
111
2
10
4
44
33
2
22
n
n
n
n
SOLO Primes
Euler Product Formula
primeps
ns pn
s1
11
1
Another Proof of the Product Formula
Start with the following geometric series expansion
skssss ppppp
11111
1
132
When , we have |p−s| < 1 and this series converges absolutely
Hence we may take a finite number of factors, multiply them together, and rearrange terms. Taking all the primes p up to some prime number limit q, we have
1
1
1
1
qsqps np
s
where σ is the real part of s. By the fundamental theorem of arithmetic, the partial product when expanded out gives a sum consisting of those terms n−s where n is a product of primes less than or equal to q. The inequality results from the fact that therefore only integers larger than q can fail to appear in this expanded out partial product. Since the difference between the partial product and ζ(s) goes to zero when σ > 1, we have convergence in this region.
Leonhard Euler(1707 – 1`783)
EulerZeta Function and the Prime History (continue – 6)
Return to TOC
26
In number theory, the Prime Number Theorem (PNT) describes the asymptotic distribution of the prime numbers. The prime number theorem gives a general description of how the primes are distributed amongst the positive integers.
Prime Number Distribution
SOLO Primes
Since a general formula for the Prime determination couldn’t be found, the attention was driven to the following question: How to find a function that defines the number of primes less or equal to a given number x? This function was named π (x)
primepxp
xprimesofnumberx 1:
The first question that was unsuccessful tackled was: Given a integer number N, how to find the Prime Number P, less then N, and as closed as possible to N.
Return to TOC
27
In number theory, the Prime Number Theorem (PNT) describes the asymptotic distribution of the prime numbers. The prime number theorem gives a general description of how the primes are distributed amongst the positive integers.
Prime Number Theorem (PNT) Let π(x) be the prime-counting function that gives the number of primes less than or equal to x, for any real number x. For example, π(10) = 4 because there are four prime numbers (2, 3, 5 and 7) less than or equal to 10. The Prime Number Theorem then states that the limit of the quotient of the two functions π(x) and x / ln(x) as x approaches infinity is 1, which is expressed by the formula
Prime Number Theorem (PNT)
1
ln/lim
xx
xx
π(x)
x / ln(x)
SOLO Primes
Return to TOC
28
SOLO Primes
History of the Asymptotic Law of Distribution of Prime Numbers
Based on the tables by Anton Felkel and Jurij Vega, Adrien-Marie Legendre conjectured in 1797 or 1798 that π(a) is approximated by the function a/(A ln(a) + B), where A and B are unspecified constants. In the second edition of his book on number theory (1808) he then made a more precise conjecture, with A = 1 and B = −1.08366.
Adrien-Marie Legendre )1752 – 1833 (
Carl Friedrich Gauss considered the same question: "Ins Jahr 1792 oder 1793", according to his own recollection nearly sixty years later in a letter to Encke (1849), he wrote in his logarithm table (he was then 15 or 16) the short note "Primzahlen unter
But Gauss never published this conjecture.
BaA
aa
ln
a
aa
ln
29
SOLO Primes
History of the Asymptotic Law of Distribution of Prime Numbers
Later Gauss came up with a new approximating function, the logarithmic integral Li (x)
x
u
duxLi
2 ln:
Calculating 1000
1000
xxx
Computing by hand, it seams that Δ(x) tends to zero ,but very slowly. To see how slow computing the inverse of Δ(x) it was found that
xx ln/1
Meaning that x
xln
1
Define
Carl Friedrich Gauss(1777 – 1855)
xLi
x
x
x
ln
30
x π(x) π(x) − x / ln x π(x) / (x / ln x) li(x) − π(x) x / π(x)10 4 −0.3 0.921 2.2 2.500
102 25 3.3 1.151 5.1 4.000103 168 23 1.161 10 5.952104 1,229 143 1.132 17 8.137105 9,592 906 1.104 38 10.425106 78,498 6,116 1.084 130 12.740107 664,579 44,158 1.071 339 15.047108 5,761,455 332,774 1.061 754 17.357109 50,847,534 2,592,592 1.054 1,701 19.667
1010 455,052,511 20,758,029 1.048 3,104 21.9751011 4,118,054,813 169,923,159 1.043 11,588 24.2831012 37,607,912,018 1,416,705,193 1.039 38,263 26.5901013 346,065,536,839 11,992,858,452 1.034 108,971 28.896
1014 3,204,941,750,802 102,838,308,636 1.033 314,890 31.202
1015 29,844,570,422,669 891,604,962,452 1.031 1,052,619 33.507
1016 279,238,341,033,925 7,804,289,844,393 1.029 3,214,632 35.812
1017 2,623,557,157,654,233 68,883,734,693,281 1.027 7,956,589 38.116
1018 24,739,954,287,740,860 612,483,070,893,536 1.025 21,949,555 40.420
1019 234,057,667,276,344,607 5,481,624,169,369,960 1.024 99,877,775 42.725
1020 2,220,819,602,560,918,840 49,347,193,044,659,701 1.023 222,744,644 45.028
1021 21,127,269,486,018,731,928 446,579,871,578,168,707 1.022 597,394,254 47.332
1022 201,467,286,689,315,906,290 4,060,704,006,019,620,994 1.021 1,932,355,208 49.636
1023 1,925,320,391,606,803,968,923 37,083,513,766,578,631,309 1.020 7,250,186,216 51.939
SOLO Primes
History of the Asymptotic Law of Distribution of Prime Numbers
31
SOLO Primes
History of the Asymptotic Law of Distribution of Prime Numbers
Both Gauss's formulas imply the same conjectured asymptotic equivalence of π(x) , x / lnx and Li (x) stated above, although it turned out that Gauss's Li (x) approximation is considerably better if one considers the differences instead of quotients. By using L’Hopital theorem we can see that
11ln
lnlim
ln
1lnln1
lim
ln
limln/
lim
2
x
x
x
xx
xx
xdd
xLixd
d
xx
xLixxxx
Example:
6115ln/,128,78498,106 nnnnnLinn
Carl Friedrich Gauss(1777 – 1855)
32
SOLO Primes
Gauss's function compared to the true number of primes
Gauss's guess was based on throwing a dice with one side marked "prime" and the others all blank. The number of sides on the dice increases as we test larger numbers and Gauss discovered that the logarithm function could tell him the number of sides needed. For example, to test primes around 1,000 requires a six-sided dice. To make his guess at the number of primes, Gauss assumed that a six-sided dice would land exactly one in six times on the prime side. But of course it is very unlikely that a dice thrown 6,000 times will land exactly 1,000 times on the prime side. A fair dice is allowed to over- or under-estimate this score. But was there any way to understand how to get from Gauss's theoretical guess to the way the prime number dice had really landed? Aged 33, Riemann, now working in Göttingen, discovered that music could explain how to change Gauss's graph into the staircase graph that really counted the primes.
Carl Friedrich Gauss(1777 – 1855)
University of Göttingen
History of the Asymptotic Law of Distribution of Prime Numbers
33
SOLO Primes
John Edensor Littlewood1885 - 1977
xx
xxLix
lnlnln
ln2/1
.10341010x
.1031010x
Gauss asserted that π (x) < Li (x). Toward the end of his 1859 paper Riemann makes the same assertion. Using computation this was proved to be true for all x < 108.In 1914 Litlewood showed that π (x) – Li (x) changes sign infinitely often. He showed that there is a constant K > 0 such that
is greater than K for arbitrarily large x and less than –K for arbitrarily large x.Litlewood’s method helped Skewes, who in 1933, showed that there is at least one sign change at x for some
Skewes proof required the Riemann Hypothesis. In 1955 he obtained a bound without using the Riemann Hypothesis. This new bound was
Skewes large bound can be reduced substantially. In 1966 Sherman Leham showed that between 1.53x101165 and 1.65x101165 there are more than 10500 successive integers x for which π (x) > Li (x). Lehman work suggest there is no sign change before 1020.In 1987 Riele showed that between 6.62x10370 and 6.69x10370 there are more than 10180
successive integers for which π (x) > Li (x).
History of the Asymptotic Law of Distribution of Prime Numbers
34
SOLO Primes
History of the Asymptotic Law of Distribution of Prime Numbers
In 1837 Johann Peter Gustav Lejeune Dirichlet introduced Dirichlet Series
Johann Peter Gustav Lejeune Dirichlet
)1805– 1859 (
1
:ˆn
sn
nfsf
is convergent for Re (s) > c if f (n) = O (n c-1 ) as n → ∞.
Given the Perron’s Formula
Oskar Perron ( 1880 – 1975)
011
10
2
1
xif
xifds
s
x
i
i
i
n
then
xnn
i
i ns
si
i
s nfnxif
nxifnf
s
ds
n
nfx
is
dssfx
i 111 1
0
2
1ˆ2
1
For f (n) = 1 we obtain the Zeta Function
1
1:
nsn
s
therefore
xn
i
i
s
s
dssx
i 1
12
1
SOLO Primes
History of the Asymptotic Law of Distribution of Prime Numbers
In two papers from 1848 and 1850, the Russian mathematician Pafnuty L'vovich Chebyshev attempted to prove the asymptotic law of distribution of prime numbers. His work is notable for the use of the zeta function ζ(s) (for real values of the argument "s", as are works of Leonhard Euler, as early as 1737) predating Riemann's celebrated memoir of 1859, and he succeeded in proving a slightly weaker form of the asymptotic law, namely, that if the limit of π(x)/(x/ln(x)) as x goes to infinity exists at all, then it is necessarily equal to one.[2] He was able to prove unconditionally that this ratio is bounded above and below by two explicitly given constants near to 1 for all x.[3]
Leonhard Euler(1707 – 1`783)
Joseph Louis François Bertrand
(1822 –1900)
Although Chebyshev's paper did not prove the Prime Number Theorem, his estimates for π(x) were strong enough for him to prove Bertrand's postulate that there exists a prime number between n and 2n for any integer n ≥ 2.
5/6,30/532log 1230/15/13/12/1
1 ccc where , and N is sufficiently large.
N
NcN
N
Nc
lnln 11
Pafnuty Lvovich Chebyshev
) ) 1821 – 1894
SOLO Primes
History of the Asymptotic Law of Distribution of Prime Numbers
Without doubt, the single most significant paper concerning the distribution of prime numbers was Riemann's 1859 memoir On the Number of Primes Less Than a Given Magnitude, the only paper he ever wrote on the subject. Riemann introduced revolutionary ideas into the subject, the chief of them being that the distribution of prime numbers is intimately connected with the zeros of the analytically extended Riemann zeta function of a complex variable. In particular, it is in this paper of Riemann that the idea to apply methods of complex analysis to the study of the real function π(x) originates. Extending these deep ideas of Riemann, two proofs of the asymptotic law of the distribution of prime numbers were obtained independently by Jacques Hadamard and Charles Jean de la Vallée-Poussin and appeared in the same year (1896). Both proofs used methods from complex analysis, establishing as a main step of the proof that the Riemann zeta function ζ(s) is non-zero for all complex values of the variable s that have the form s = 1 + i t with t > 0
Georg Friedrich Bernhard Riemann
)1826– 1866(
Jacques Salomon Hadamard
(1865 –1963)
Charles-Jean Étienne Gustave Nicolas de la Vallée Poussin
(1866 1962)
SOLO Primes
History of the Asymptotic Law of Distribution of Prime Numbers
During the 20th century, the theorem of Hadamard and de la Vallée-Poussin also became known as the Prime Number Theorem. Several different proofs of it were found, including the "elementary" proofs of Atle Selberg and Paul Erdős (1949). While the original proofs of Hadamard and de la Vallée-Poussin are long and elaborate, and later proofs have introduced various simplifications through the use of Tauberian theorems but remained difficult to digest, a surprisingly short proof was discovered in 1980 by American mathematician Donald J. Newman. Newman's proof is arguably the simplest known proof of the theorem, although it is non-elementary in the sense that it uses Cauchy's integral theorem from complex analysis
Atle Selberg (1917 –2007)
Paul Erdős (1913 –1996)
Donald J. Newman ( 1930 –2007)
Return to TOC
38
SOLO Primes The Chebychef Contribution
integeres,1
2121
ii
m
i
ki
km
kk kprimespppppn im
The starting point is that any positive number can be factored into a unit product of powers of distinct primes
integeres,lnlnlnlnln1
2211
ii
m
iiimm kprimesppkpkpkpkn
The utility of this formula is enhanced by the use of von Mangold symbol Λ (n)
otherwise
kandpprimesomeforpnifpn
k
0
1integerln
Hans Carl Friederich von Mangold (1854 – 1925)
The symbol Σj|n will be used to denote a sum on j where j runs through all of the positive divisors of the positive integer n. With this notation we have:
m
iii
nj
pkjn1|
lnln
To prove this note that from and the definition of Λ (j) the only nonzero terms that can appear on the right side are ln p1,ln p2,…,ln pk. Moreover p1 appears for j=p1, j=p1
2,…,j=p1k1. Thus ln p1 appears exactly
k1 times. Similarly p2 appears exactly k2 times, etc. q.e.d.
mkm
kk pppn 2121
Since we have products a most useful formula is obtained by using natural logarithm
Pafnuty Lvovich Chebyshev
) ) 1821 – 1894
Return to TOC
39
SOLO Primes
otherwise
kandpprimesomeforpnifpn
k
0
1integerln Von Mangoldt Function1895
Pafnuty Lvovich Chebyshev
) ) 1821 – 1894
The Chebyschev Functions (1851)
primepxp
px ln:Chebyschev Theta Function
primepxpxn k
pnx ln:Chebyschev Psi Function
From the definition of Chebyschev Psi Function and of Λ (j)
3/12/1
lnlnlnln:32
xxx
ppppnx
primepxp
primepxp
primepxp
primepxpxn k
40
SOLO Primes
3ln2ln7ln5ln2ln3ln2lnln primep
xpk
px
otherwise
kandpprimesomeforpnifpn
k
0
1integerln
The Chebyschev Functions (continue - 1)
7ln5ln3ln2lnln:1010
primep
p
px
Example: x = 10
Prime Numbers p < x = 10 :p: 2, 3, 5, 7
Prime Numbers p2 < x = 10 :p2: 22=4, 32=9
Prime Numbers p3 < x = 10 :p3: 23=8,
,010,3ln9,2ln8,7ln7,06
,5ln5,2ln4,3ln3,2ln2,01
7ln5ln3ln22ln3:1010
xn
nx
1621028 43 x
2ln
10ln32ln410ln2ln3
10..integral: xxtsx
primepxp
primepxp
pp
xpx
k
lnln
lnln
41
SOLO Primes
3/2/ln: xxxpnx
primepxpxn k
otherwise
kandpprimesomeforpnifpn
k
0
1integerln Von Mangoldt Function1895
The Chebyschev Functions (continue - 2)
primepxp
px ln:
Theorem x
x
x
x
xx
xxxx
limlimln/
lim
Proof:
primepxp
xprimesofnumberx 1:
primepxp
xp
primepxp
xpxxxxxk
1lnln3/2/lnln
Define:
11ln
ln/::,: 321
xx
x
xx
xL
x
xL
x
xL
primepxp
Therefore: 321 LLL
One the other hand, if 0 < α <1, x > 1, then: x > α → ln x > ln α
xxxxxxxxppx
xx
xpxxpx
xp
xpxpx
primepxp
lnlnln1lnlnln:10lnln
Return to Newman Proof of PNT
Chebyshev didn’t prove that the limit is 1.
42
SOLO Primes
3/2/ln: xxxpnx
primepxpxn k
The Chebyschev Functions (continue - 3)
primepxp
px ln:
Theorem x
x
x
x
xx
xxxx
limlimln/
lim
Proof (continue):
primepxp
xprimesofnumberx 1:
Define:
11ln
ln/::,: 321
xx
x
xx
xL
x
xL
x
xL
primepxp
321 LLL
xxxx ln
Dividing the inequality by x > 1 we obtain:
1
lnln
x
x
x
xx
x
x
Keep α fixed and x → ∞ we obtain: 0ln
lim10
1
x
xx
Hence:
31 limln
limlimlim Lx
xxL
x
xxxxx
gives: 321 limlimlim LLLxxx
q.e.d.
Tacking α→1: 31 limlim LLxx
together with 321 LLL
Return to TOC
xx OReturn to
43
SOLO Primes
xx O
The Chebyschev’s First Estimate
primepxp
px ln:
Theorem
Proof: Start with the Binomial formula
121
1212222112
integer
2
0
22
nn
nnnn
n
n
k
nn
k
nn
nnpppp
npn
eeeepn
nnpnpnpnnpn
2lnlnlnln
2
2222
Taking natural algorithm from both sides, we obtain nnn 22ln2
Definition of O:We say that f (x) = O (g (x)) if exists a constant k > 0 such that |f (x)| < k |g (x)|
nk
primepnpnnpnnkn
kbbydividednotispcpknnnna1222
:&:12122
cb
apkcbka
npnnknkn
212
:
44
SOLO Primes
xx O
The Chebyschev’s First Estimate
primepxp
px ln:
Theorem
Proof (continue):
q.e.d.
Definition of O:We say that f (x) = O (g (x)) if exists a constant k > 0 such that |f (x)| < k |g (x)|
Let be r the minimal integer such that 2r > x. Then
xxx 2ln12/
rrrr
xxxxxxxx
xxx
22222222 1122
Therefore xx O
xxxxx rr
jj
r
jjj
2ln12
21
1
21
12ln1
22ln1
22
1
0
1
01
Taking natural algorithm from both sides, we obtain nnn 22ln2Define [x] the biggest integer less than x; i.e. 0 < x – [x] < 1 Then
xxx
xxxx
xxxx 2ln12ln
22ln
222
22
22/
Return to TOC
45
SOLO Primes
xx O
The Chebyschev’s Second Estimate
primepxp
px ln:
Theorem
Proof:
Definition of O:We say that f (x) = O (g (x)) if exists a constant k > 0 such that |f (x)| < k |g (x)|
3/2/ln: xxxpnx
primepxpxn k
For 0 < δ < 1 and y = x1-δ, we have
x
xx
y
xyyx
y
xp
yp
yyy
primepxpy
primepxp
primepxpy
primepxpy
primepyp
ln1
1
ln1
lnln
ln
1ln
ln
11&1
1
Therefore
x
x
x
x
x
x
x
x
xx
x
x
x
x
x
1
1ln
1
1ln
ln/
We also proved that xx
x
x
x
x
x
ln/
46
SOLO Primes
xx O
The Chebyschev’s Second Estimate
primepxp
px ln:
Theorem
Proof (continue):
Definition of O:We say that f (x) = O (g (x)) if exists a constant k > 0 such that |f (x)| < k |g (x)|
3/2/ln: xxxpnx
primepxpxn k
For x → ∞ and δ→0 we have
For 0 < δ < 1 and y = x1-δ, we have
2ln12
1
1ln
1
1ln 2ln12
x
x
x
x
x
x
x
x xx
0ln
x
x
xxx
2ln12
Therefore xx Oq.e.d.
Return to TOC
47
SOLO Primes
Riemann's Zeta Function (1859)The Riemann Zeta Function or Euler–Riemann Zeta Function, ζ(s), is a function of a complex variable s that analytically continues the sum of the infinite series
tisn
sn
s
1
1
“On the Number of Primes Less Than a Given Magnitude”, 7 page paper offered to the Monatsberichte der Berliner Akademie on October 19, 1859. The exact publication date is unknown.
ssss ss
1
2sin12 1
where Γ(s) is the Gamma Function, which is an equality of Meromorphic Functions valid on the whole complex plane. This equation relates values of the Riemann Zeta Function at the points s and 1 − s. The functional equation (owing to the properties of sin ) implies that ζ(s) has a simple zero at each even negative integer s = −2n — these are known as the trivial zeros of ζ(s). For s an even positive integer, the product sin(πs/2)Γ(1−s) is Regular and the functional equation relates the values of the Riemann Zeta Function at odd negative integers and even positive integers.
Georg Friedrich Bernhard Riemann )1826– 1866(
Return to TOC
To construct the analytic Continuation of the Zeta Function, Riemann established the relation (see proof ).
Graph showing the Trivial Zeros, the Critical Strip and the Critical Line of ζ (s) zeros.
SOLO Primes
,2,11
1 1
nn
Bn nn
Those roots are called the Trivial Zeros of the Zeta Function. The remaining zeros of ζ (s) are called Nontrivial Zeros or Critical Roots of the Zeta Function.The Nontrivial Zeros are located on a Critical Strip defined by 0 < σ < 1.
Since Bn+1 = 0 for n + 1 odd (n even) we also have ,2,102 mm
We found
tispn
sprimep
zn
sRe
1
11
1
Riemann Zeta Function Zeros
Since the product contains no zero factors we see that ζ (z) ≠ 0 for Re {z} >1.
Riemann Conjecture in his paper was that all Zeta Function Nontrivial Zeros are located at σ = ½. This Conjecture was not proved and is named One of the Greatest Mysteries in Mathematics.
Bn are the Bernoulli numbers
49
SOLO Primes
Riemann's Zeta Function
Specific Values
,3,2,1,0
!22
212
221 n
n
Bn
nnn
For any positive even number 2n
where B2n are the Bernoulli numbers.
,3,2,11
1 1
nn
Bn nnFor negative integers one has
Therefore ζ vanishes at the negative even integers ζ (-2m) = 0 since B2m+1 = 0 for all m , m=1,2,…
,3,2,12
121 2 mB
mm m
It is easy to show that the last equation is equivalent with
2
1
210
101 0
BB
50
SOLO Primes
Riemann's Zeta Function
The Riemann zeta function or Euler–Riemann zeta function, ζ(s), is a function of a complex variable s that analytically continues the sum of the infinite series
tisn
sn
s
1
1
which converges when the real part of s is greater than 1. More general representations of ζ(s) for all s are given below. The Riemann zeta function plays a pivotal role in analytic number theory and has applications in physics, probability theory, and applied statistics.
Georg Friedrich BernhardRiemann
1826 - 1866
51
SOLO Primes
Riemann's Zeta Function tisn
sn
s
1
1
Georg Friedrich Bernhard Riemann )1826– 1866(
Riemann zeta function ζ(s) in the complex plane. The color of a point s encodes the value of ζ(s): colors close to black denote values close to zero, while hue encodes the value's argument. The white spot at s = 1 is the pole of the zeta function; the black spots on the negative real axis and on the critical line Re(s) = 1/2 are its zeros. Values with arguments close to zero including positive reals on the real half-line are presented in red
52
SOLO Primes
Riemann imaginary landscape
Graph showing the Trivial Zeros, the Critical Strip and the Gritical Line of ζ (s) zeros.
Modulus |ζ s)| ploted over the complex plane
Riemann's Zeta Function
53
SOLO Primes
The plots above show the real and imaginary parts of plotted in the complex plane together with the complex modulus of ζ (s) . As can be seen, in right half-plane, the function is fairly flat, but with a large number of horizontal ridges. It is precisely along these ridges that the nontrivial zeros of ζ (s) lie.
Riemann's Zeta Function
54
Riemann's Zeta FunctionPrimes
55
Re ζ (s) in the original domain, Re s > 1.
Re ζ (s) after Riemann’s extension.
Riemann's Zeta Function
Primes
56
SOLO Primes
The position of the complex zeros can be seen slightly more easily by plotting the contours of zero real (red) and imaginary (blue) parts, as illustrated above. The zeros (indicated as black dots) occur where the curves intersect
The figures bellow highlight the zeros in the complex plane by plotting |ζ(s)|) where the zeros are dips) and 1/|ζ(s)) where the zeros are peaks).
Riemann's Zeta Function
57
The Riemann Hypothesis
The Non-Trivial Zeros ρ of ζ (s) has Re ρ = 1/2
Riemann's Zeta Function
Primes
58
SOLO Primes
Year Number of zeros Computed by1859 (approx.) 1 B. Riemann1903 15 J. P. Gram1914 79 R. J. Backlund1925 138 J. I. Hutchinson1935 1,041 E. C. Titchmarsh1953 1,104 A. M. Turing1956 15,000 D. H. Lehmer1956 25,000 D. H. Lehmer1958 35,337 N. A. Meller1966 250,000 R. S. Lehman1968 3,500,000 J. B. Rosser, et al.1977 40,000,000 R. P. Brent1979 81,000,001 R. P. Brent1982 200,000,001 R. P. Brent, et al.1983 300,000,001 J. van de Lune, H. J. J. te Riele1986 1,500,000,001 J. van de Lune, et al.2001 10,000,000,000 J. van de Lune (unpublished)2004 900,000,000,000 S. Wedeniwski2004 10,000,000,000,000 X. Gourdon
Computation of the Non-trivial Zeros of the Riemann Zeta Function.All were on the Critical Line σ = ½.
Riemann's Zeta FunctionRiemann Conjecture in his paper was that all Zeta Function Nontrivial Zeros are located at σ = ½. This Conjecture was not proved and is named One of the Greatest Mysteries in Mathematics.
Return to TOC
59
SOLO Primes Riemann's Zeta Function Properties
1
1'uduu
ss
s s
We found
ic
ic
s
sds
x
s
s
ix
'
2
1Mellin Transform
1,
1ln
2
tisxdxx
xss
s
primepxp
xprimesofnumberx 1:
100
2/12ln
12/112
Re
s
es
ss
es
Hadamard
γ is the Euler-Mascheroni constant
γ=0.57721566490153286060651
2210 11
1
1ss
ss
1
lnlnlim
!
1 1
k
N
m
m
k
k
Nm
k
N
k
k
3/2/ln: xxxpnx
primepxpxn k
otherwise
kandpprimesomeforpnifpn
k
0
1integerln Von Mangoldt Function1895
primepxp
px ln:
60
SOLO Primes Riemann's Zeta Function Properties
We found
11
11
1
xdxxxss
s s
11
1lim1 1
11
s
ss
s
ss
sss ResRes
primesdistinctkofproducttheisnif
factorprimemultiplesomecontainsnif
nif
n
FunctionbiusoM
k1
0
11
10
11
| nif
nifd
nd
1
1
nsn
n
s
11
1 xdxxss s
Mellin Transform
ic
ic
s sds
sx
ix
2
1
61
SOLO Primes Riemann's Zeta Function Properties
We found
1
1
4
1
3
1
2
1
1
/1
1
4
1
3
1
2
1:
1
0
11
n
n
k
n
n
xn
xxxxxJ
FunctionbiusoM
primesdistinctkofproducttheisnif
factorprimemultiplesomecontainsnif
nif
n
xJn
nx
1,
1
ln
2
tisxd
xx
x
s
ss
primepxp
xprimesofnumberx 1:
1
11
n
nxn
xJ
ic
ic
s
s
ss
n
n
sds
sx
ixJ
xdxxJs
s
xdxxJxdxxJs
s
Jxxxn
xxxxxJ
ln
2
1
ln
ln
000101
4
1
3
1
2
1:
0
1
0
1
1
1
1
1
4
1
3
1
2
1
p
sssxdxdv
xu
s pxdxxxxdxxss
10
11
11
62
SOLO Primes Riemann's Zeta Function
We found
x
n
n
x
dxxLi
xLin
nxR
0
1
/1
ln:
:
1 !
lnlnln
n
n
nn
xxxLi
1
1
11 1
1 1!1
!1
1
m
mmn
n
nnm n
m
m
mmm
t
n
n
mm
txR
nm
63
SOLO Primes
xxLix ln O
x
t
tdxLi
2 ln:
primepxp
xprimesofnumberx 1:
xxx 2ln O
nnLipn2/51 lnO
Constantln
11 2/1 Eulerx
x
e
pxp
O
0Im0
2/12ln
12/112
s
es
ss
es Hadamard
Definition of O:We say that f (x) = O (g (x)) if exists a constant k > 0 such that
|f (x)| < k |g (x)| Return to TOC
64
SOLO Primes
Riemann Zeta Function
11
10
2
1
2:Re aif
aifds
s
a
i ss
s
Special case of Perron’s Formula
Chebychev Psi Function
2:Re
11
2:Re/
1
ln
2
1/ln
2
1ln:
ss
s
mprimep
xpms
mprimep
xp ss
smPerron
xa
mprimep
xp
dss
x
p
p
ids
s
pxp
ipx
mmm
m
We were able to swap the infinite sum and the infinite integral since the terms are convergent as Re (s) = 2
11
1lnln1
tispm
psprimep m
ms
SeriesTaylor
primep
s
1
ln
1
ln1'ln
11
1
tis
p
p
p
pp
s
ss
sd
d
primep primep mms
Taylor
p
s
s
s
tispn
sprimep
sn
s
1
1
11
1
2:Re2:Re
1
'
2
1ln
2
1
ss
s
ss
s
mprimep
xpms
dss
x
s
s
ids
s
x
p
p
ix
m
Von Mangoldt Psi FormulaHans Carl Friederich von Mangoldt 1895
2/12
0Re0
1
1ln0
0'ln:
xx
xpx
mprimep
xpm
65
SOLO Primes
2:Re2:Re
1
'
2
1ln
2
1
ss
s
ss
s
mprimep
xpms
dss
x
s
s
ids
s
x
p
p
ix
m
Von Mangoldt Psi Formula(continue – 1)
1 42
t
10'
xdss
x
s
s
LC
s
LC
R
eRsCj
L
0cos2
2:
R
Critical Region(non-trivial zeros)
ζ (s) = 0trivial zerosζ (s) = 0
26 4
Therefore
Define a semi-circular path CL (left side), with s=2 as the origin., and R → ∞.
0''
sincos
''
0cos0
coscos
sincos
,,
R
xC
R
C
R
C
iiRR
C
s
LL
RLRL
dxs
sdR
R
x
s
s
deRiiRR
x
s
sds
s
x
s
s
LL Cs
s
C
s
ss
s
ss
s
dss
x
s
s
ids
s
x
s
s
ids
s
x
s
s
ids
s
x
s
s
ix
2Re
0
2:Re2:Re
'
2
1'
2
1'
2
1'
2
1
s
x
s
s
s
x
s
s
s
x
s
s
s
x
s
s s
sofzeros
s
s
s
s
s
Cs L
'Residues
'Residue
'Residue
'Residues
102)Re(
2/12
0Re0
1
1ln0
0'ln:
xx
xpx
mprimep
xpm
66
SOLO Primes
Von Mangoldt Psi Formula(continue – 2)
LCs
s
dss
x
s
s
ix
2Re
'
2
1
1Re0
00
,...4,2
00
1
1
0
0
10
'lim
'lim
1
'1lim
'lim
'Residues
'Residue
'Residue
ZerosTrivialNon
s
ZerosTrivial
sss
s
sofzeros
s
s
s
s
x
s
ss
x
s
ss
x
s
ss
s
x
s
ss
s
x
s
s
s
x
s
s
s
x
s
s
2
10&2ln
2
10'2ln
0
0''lim
0
0
s
x
s
ss
s
1 42
t
10'
xdss
x
s
s
LC
s
LC
R
eRsCj
L
0cos2
2:
R
Critical Region(non-trivial zeros)
ζ (s) = 0trivial zerosζ (s) = 0
26 4
2/12
0Re0
1
1ln0
0'ln:
xx
xpx
mprimep
xpm
xx
s
sx
s
ss
ss
1
1
1
1
11'
1lim
1
'1lim
Now we have:
67
SOLO Primes
Von Mangoldt Psi Formula(continue – 3)
LCs
s
dss
x
s
s
ix
2Re
'
2
1
1Re0
00
,...4,2
00
1
1
0
0
'lim
'lim
1
'1lim
'lim
ZerosTrivialNon
s
ZerosTrivial
sss
x
s
ss
x
s
ss
x
s
ss
s
x
s
ss
2/12
1
2
1
2
1
00
2
,4,2
00
1ln22
2'2
lim'
lim
x
n
x
n
xn
s
nsx
s
ss
Taylor
n
n
n
n
ns
ZerosTrivial
s
00
00
10
0
'lim
'lim
xx
s
ss
x
s
ss
s
ZerosTrivialNon
s
1 42
t
10'
xdss
x
s
s
LC
s
LC
R
eRsCj
L
0cos2
2:
R
Critical Region(non-trivial zeros)
ζ (s) = 0trivial zerosζ (s) = 0
26 4
2/12
0Re0
1
1ln0
0'ln:
xx
xpx
mprimep
xpm
q.e.d.
1'
'
1'lim
'
0
HopitalL
s s
s
We also have:
68
SOLO Primes
Von Mangoldt showed that ψ can also be determined from the non-trivial zeros ρ of the Zeta Function ζ (ρ) = 0
2
2/1lnln
2
010
1
xxxpx
mxp
primepm
Because the zeros ρ are complex, the values xρ/ρ are also complex.But since the nontrivial zeros come in complex-conjugate pairs ρ and ρ*. The values xρ/ρ and xρ*/ρ* are also complex conjugate so all imaginary parts cancel in the infinite sum.
The function xρ/ρ maps the positive reals onto a logarithmic spiral in the complex plane. xρ/ρ and xρ*/ρ* produce complex conjugate spirals (mutual reflections across the real axis. xρ/ρ + xρ*/ρ* =2 Re [xρ/ρ] is a real valued function, a sort of logarithmically – rescaled sinusoid with increased amplitude as pictured bellow:
...)13.14(2/1 i ...)58.37(2/1 i
Von Mangoldt Psi Formula (continue – 4)
69
SOLO Primes
Von Mangoldt showed that ψ can also be determined from the non-trivial zeros ρ of the Zeta Function ζ (ρ) = 0
2
2/1lnln
2
010
1
xxxpx
mxp
primepm
Comparing ψ (x) with its approximation via summing the first 50 zeros of the Zeta function.
The Chebyshev Psi Function can be reconstructed by starting with the function x – ln (2π)-1/2 ln (1-1/x2), and then successively adding “spiral wave” functions.
Von Mangoldt Psi Formula (continue – 5)
70
SOLO Primes
Von Mangoldt showed that ψ can also be determined from the non-trivial zeros ρ of the Zeta Function ζ (ρ) = 0
2
2/1lnln
2
010
1
xxxpx
mxp
primepm
Comparing ψ (x) in the interval x ϵ (2.5, 5.5) with its approximation via summing the first 100 zeros of the Zeta function.
Comparing ψ (x) in the interval x ϵ (2.5, 5.5) with its approximation via summing the first 500 zeros of the Zeta function.
The Chebyshev Psi Function can be reconstructed by starting with the function x – ln (2π)-1/2 ln (1-1/x2), and then successively adding “spiral wave” functions.
2
2/1lnln
2
010
1
xxxpx
mxp
primepm
Von Mangoldt Psi Formula (continue – 6)
71
SOLO Primes
Von Mangoldt showed that ψ can also be determined from the non-trivial zeros ρ of the Zeta Function ζ (ρ) = 0
2
2/1lnln
2
010
1
xxxpx
mxp
primepm
Let take the derivative of the staircase function ψ (x)
2/12
11'
2
010
1
x
xxxx
xd
d
Since ψ (x) is a staircase function that jumps at each prime power pk, ψ’(x) should be zero except for spikes at
2, 3, 4, 5, 7, 8, 9, 11, 13, 16, 17, 19,…In the sum
each conjugate pair contributes a waveform (harmonic mode)
21'
2
010
1
x
xxx
, xxeexxx xixi ln1cos2 1ln1ln1111 ImReImImRe
Since 0 < Re ρ < 1, we have -1 < Re (ρ-1) < 0, therefore the amplitude of the waveform is a monotonic decreasing function of x. The frequency of the waveform is related to Im (ρ – 1) ln x is a monotonic increasing function of x.
12 Rex
Von Mangoldt Psi Formula (continue – 7)
72
SOLO Primes
The effect of Riemann's harmonics
Riemann's harmonics
Von Mangoldt Psi Formula (continue – 8)
73
SOLO Primes
Von Mangoldt Psi Formula (continue – 9)
For example here are plots of ψ’(x) using Nρ=10, 50 and 200 pairs of zeros
ψ’(x) is zero except for spikes at2, 3, 4, 5, 7, 8, 9, 11, 13, 16, 17, 19,…
Nρ = 10
Nρ = 50
Nρ = 200
2/12
11'
2
010
1
x
xxxx
xd
d
74
SOLO Primes
Each conjugate pair contributes a waveform (harmonic mode) , xxxx ln1cos2 111 ImRe
If the Riemann Hypothesis (R.H. = Re ρ = ½) is true all the harmonics will have the same amplitude xx /22 2/1
If the Riemann Hypothesis is not , that at least one harmonics has a different amplitude then others.
Von Mangoldt Psi Formula (continue – 10)
75
SOLO Primes
01
lim
010
x
xx
But independent if the assumption that Riemann Hypothesis is true or false, since we have 0 < Re ρ < 1 for all ρ, we have
From the Explicit Formula for ψ (x)
2
2/1ln
111
2
010
x
x
x
xx
x
Also 02
2/1ln
1lim
2
x
xx
Therefore that proves the Prime Number Theorem.
1lim x
xx
Von Mangoldt Psi Formula (continue – 11)
Return to TOC
SOLO Primes
1
1
4
1
3
1
2
1
1
1
1
4
1
3
1
2
1:
ln
n
n
s
xn
xxxxxJ
xdxxJs
s
This sum is only formally infinite, since , as soon as decreases bellow 2, which will happen as soon as n > lnx/ln2. f (x) has jumps of 1/r when x passes a prime power pr. (when x passes a prime p, this is regarded as the prime power p1.)
0/1 nx nx /1
Proof:
primepxp
s
primepxp
s
primepxp
sa
SeriesTaylor
primepxp
s
primepxp
s
ppp
pps
321ln
1
3
1
2
1
1ln1lnln
Riemann's Zeta Function Relations
SOLO Primes
1
1
4
1
3
1
2
1
1
1
1
4
1
3
1
2
1:
ln
n
n
s
xn
xxxxxJ
xdxxJs
s
Proof (continue – 1):
primepxp
s
primepxp
s
primepxp
s ppps 32
3
1
2
1ln
Using Stieltjes’ Integrals and performing Integration by Parts, we obtain
p
sssxdxdv
xu
s pxdxxxxdxxss
10
11
11
This follows since and d π (x) will increase by 1 when x is a prime number p, and will be zero between primes.
0lim000
0
xxx s
x
In the same way
p
snnsnsxdxdv
xu
sn pxdxxxxdxxss
n
1
1
0
1
1
1
11 1
1
Riemann's Zeta Function Relations
SOLO Primes
Riemann's Zeta Function Relations
1
1
4
1
3
1
2
1
1
1
1
4
1
3
1
2
1:
ln
n
n
s
xn
xxxxxJ
xdxxJs
s
Proof (continue – 2):
1
1
1
12
1
1
1
32
2
1
3
1
2
1ln
xdxxJs
xdxxsxdxxs
ppps
s
ss
primepxp
s
primepxp
s
primepxp
s
1
11:
n
nxn
xJ
SOLO Primes
ic
ic
s
s
ss
n
n
sds
sx
ixJ
xdxxJs
s
xdxxJxdxxJs
s
Jxxxn
xxxxxJ
ln
2
1
ln
ln
000101
4
1
3
1
2
1:
0
1
0
1
1
1
1
1
4
1
3
1
2
1
1,
1
ln
2
tisxd
xx
x
s
ss
We found the following expressions for ln ζ(s)/s:
0
1 xdxfxsFxf sMM
ic
ic
s sdsFxi
x M1- fsfM
2
1
Riemann's Zeta Function Relations
Return to TOC
SOLO Primes
Abel’s Method of Partial Summation:
1
2 11
1
11 11
N
n
N
nnN
n
iin
N
n
n
iin
N
nnn babababa
N
n
N
nnN
n
iin
N
n
n
iin bababa
1 11
11
1 1
N
n
n
iinn
N
nnN baaba
1 11
11
n
iin
N
nnnnNN
N
nnn bBBaaBaba
1111
1
:
1
n
n
Niels Henrik Abel ( 1802 – 1829)
SOLO Primes
Use Abel’s Method of Partial Summation:
n
iin
N
nnnnNN
N
nnn bBBaaBaba
1111
1
:
1lim1
N
n
s
Nnsfor:
by choosing an = n-s, bn = 1, therefore Bn = n
110
1
11lim1limlimn
ssN
n
ss
N
s
N
N
n
s
NnnnnnnNNns
xdxxsxdxns s
nx
n
n
n
s
1
1
1
1 1
Where [x] is the integer, less then x and closer to x
10s.t.integer xxx
11
1 xdxxss s
1
1 1 1
1
1
1 11 11
1
xdx
xxs
s
xsxd
x
xxsxd
x
xsxdxxss
s
s
sss
11 1
1
xdxxxs
s
ss s
Riemann's Zeta Function Relations
Return to TOC
SOLO Primes
1
1 1 1
xdx
xxs
s
ss
s
11
100lim
11 xd
xdxd
x
xdns
s
N
n
s
N
Proof:
Integrating by parts:
11
11
1
1
11
11
11
0
1
,
,1
11
1
ss
s
ssss
xddvxu
xvdxxsdus
x
xdxxs
s
s
x
xdxxs
s
xs
x
dxxxs
x
dxxs
x
dxxs
x
x
x
xds
s
s
10s.t.integer xxx
11
11 1
forconvergesn
xdx
xx
nss
We can see that
We have an Analytic Continuation for by removing the singularity at s = 1of ζ (s). We can see that ζ (s) can a simple pole at s=1, and
1
s
ss
11
1lim1 1
11
s
ss
s
ss
sss ResRes
Riemann's Zeta Function Relations
SOLO Primes
0
1 xdxfxsFxf sMM
ic
ic
s sdsFxi
x M1- fsfM
2
1
Mellin Transform
Inverse Mellin Transform
0
1 xdxxs
ssF s
M
ic
ic
s sds
sx
ix
2
1
11
1 xdxxss s
10s.t.integer xxx
Riemann's Zeta Function Relations
Return to TOC
SOLO Primes
primesdistinctkofproducttheisnif
factorprimemultiplesomecontainsnif
nif
nk1
0
11
Möbius Function
The most important property of Möbius function is
10
11
| nif
nifd
nd
The symbol d|n means that the integer d divides the integer n, therefore the sum is on all integers d that divide n. (note that the improper divisor d=1 and d=n have to be included in this formula)
To prove this property, suppose that with all pi being different primes.Then d|n, and μ (d) = (-1)k if d is a product of precisely k different members of the set of s primes pi. This case will occur for different divisors d of n. All divisors d of n containing one or several of the primes pi twice or more have μ (d) = 0, according to the definition of μ (d). Thus
is
i ipn
1
k
s
1,01110|
sifk
sd s
s
k
k
nd
August Ferdinand Möbius1790 - 1868
111|
nd
d
SOLO Primes
primesdistinctkofproducttheisnif
factorprimemultiplesomecontainsnif
nif
nk1
0
11
Möbius Function
The most important property of Möbius function is
10
11
| nif
nifd
nd
Theorem: This relation has as one of its consequence that:
1
1
nsn
n
s
since:
111
1
1
||
1 11
s
ns
nd
s
mdd
m dss
ns n
d
dm
d
d
d
mn
ns
q.e.d.Return to TOC
SOLO Primes
1
1
4
1
3
1
2
1
1
/1
1
4
1
3
1
2
1:
1
0
11
n
n
k
n
n
xn
xxxxxJ
primesdistinctkofproducttheisnif
factorprimemultiplesomecontainsnif
nif
n
xJn
nx
Proof
xdu
xx
umu
xnmm
nm
m
x
n
nxJ
n
n
n ud
u
n um
u
n m
mn
n m
mn
n
n
1 |
/1
1 |
/1
1 1
/1
1 1
/1
1
/1
10
11
| nif
nifd
nd
Conversion from J (x) back to π (x)
q.e.d.
Return to TOC
SOLO Primes
1
1
4
1
3
1
2
1
1
/1
1
4
1
3
1
2
1:
1
0
11
n
n
k
n
n
xn
xxxxxJ
primesdistinctkofproducttheisnif
factorprimemultiplesomecontainsnif
nif
n
xJn
nx
Riemann defined the following formula to approximate the π (x):
The Riemann Prime Number Formula
x
n
n
x
dxxLi
xLixLixLixLixLi
xLin
nxR
0
6/15/13/12/1
1
/1
ln:
6
1
5
1
3
1
2
1
:
SOLO Primes
Riemann defined the following formula to approximate the π (x):
The Riemann Prime Number Formula (continue – 1)
x
n
n
x
dxxLi
xLin
nxR
0
1
/1
ln:
:
We can see from the Table that R (x) gives a better approximation of the π (x) then Li (x)
SOLO Primes
Riemann defined the following formula to approximate the π (x):
x
n
n
x
dxxLi
xLin
nxR
0
1
/1
ln:
:
11
ln
1
ln
0
1ln
0
!lnlim
!
lnlnln
!ln
!ln:
n
n
tn
nx
n
n
x
n
neofSeriesTaylor
x tex
dtedx
x
nn
tt
nn
xx
nn
tt
n
dtttd
t
e
x
dxxLi
tt
t
1 !
lnlnln
n
n
nn
xxxLi
The Riemann Prime Number Formula (continue – 2)
SOLO Primes
Riemann defined the following formula to approximate the π (x):
The Riemann Prime Number Formula (continue – 3)
x
n
n
x
dxxLi
xLin
nxR
0
1
/1
ln:
:
1 !
lnlnln
n
n
nn
xxxLi
1 11
11
1 11
/
1
/1
!
lnln
!
/ln:
n mm
m
nn
n m
m
n
ntex
n
n
mmn
tn
n
nn
n
nt
mm
nt
n
t
n
neLi
n
nxLi
n
nxR
t
0
1limlim
1
11
11
sn
n
n
ns
nss
n
But
1
1
11
1
lim'
lim1
limlim
1lim
lnlim
ln
2
2
12111
1
11
11
1
sos
sos
s
s
ssd
d
n
n
sd
d
nsd
d
n
n
n
nn
n
nn
sssn
ss
nsss
nss
n
SOLO Primes
Riemann defined the following formula to approximate the π (x):
The Riemann Prime Number Formula (continue – 4)
x
n
n
x
dxxLi
xLin
nxR
0
1
/1
ln:
:
1 !
lnlnln
n
n
nn
xxxLi
1
1
11 1
1 1!1
!1
1
m
mmn
n
nnm n
m
m
mmm
t
n
n
mm
txR
nm
Return to TOC
92
SOLO Primes
Theorem
xn
primepxp
npxk
ln:
For x ≥ 2 we have
otherwise
andpprimesomeforpnifpn
0
1integerln
2/1
22lnln
xOtdtt
t
x
xx
x
Proof
primep
xp
px ln:Define
then
x
xx
x
p
t
ptd
tt
ptd
tt
ptd
tt
t
x
xp
xx
xpxp
x
ptp
xx
tp
x
ln1
ln
ln
ln
ln
ln
ln
ln
ln
lnln/
22
22
22
Von Mangoldt Function
x
tdtt
t
xx
x
xx
x
22ln
1
ln/
Return to TOC
93
SOLO Primes
Hadamard Proof of the Prime Number Theorem (1896)
Hadamard paper on PNT used the Riemann Zeta Function ζ (s) for which he proed some new properties.
His paper published in 1896 consists of two parts:
In the First Part he proved that the Zeta Function has no Zeros on the line Re (s) = σ = 1. His proof is complicated, hence here we give the F. Mertens method to prove this.
Jacques Salomon Hadamard
(1865 –1963)
94
SOLO Primes
Hadamard Proof of the Prime Number Theorem (continue - 1
Start with the Riemann Zeta Function
11
1lnln1
tispm
psprimep m
ms
SeriesTaylor
primep
s
1
1ln
1
ln1'ln
11
1
tis
pp
p
pp
s
ss
sd
d
primep primep mms
Taylor
p
s
s
s
tispn
sprimep
sn
s
1
1
11
1
132
1ln1
32
xm
x
m
xxxxx
m
m
mmSeriesTaylor
Where the last series counts the prime powers pm, with the weight ln p, therefore
otherwise
kandpprimesomeforpnifpn
k
0
1integerln Von Mangoldt Function1895
1
1ln
'ln
11
tis
n
n
pp
s
ss
sd
d
ns
primep mms
Jacques Salomon Hadamard
(1865 –1963)
95
SOLO Primes
Hadamard Proof of the Prime Number Theorem (continue - 2)
otherwise
kandpprimesomeforpnifpn
k
0
1integerln Von Mangoldt Function1895
1
'
1
tisn
n
s
s
ns Jacques Salomon
Hadamard (1865 –1963)
100
2/12ln
12/112
Re
s
es
ss
es
Hadamard Product Representation of Riemann Zeta Function
Hadamard established the following form of the Mellin Inversion Formula
i
in
sn
s
xnn sd
n
a
s
x
in
xa
2
21
22
1ln
Substitute an = Λ (n)
i
i
si
in
s
s
xn
sds
s
s
x
isd
n
n
s
x
in
xn
2
2 2
2
21
2
'
2
1
2
1ln
96
SOLO Primes
Hadamard Proof of the Prime Number Theorem (continue - 3)
Jacques Salomon Hadamard
(1865 –1963)
i
i
si
in
s
s
xn
sds
s
s
x
isd
n
n
s
x
in
xn
2
2 2
2
21
2
'
2
1
2
1ln
11
1
tisuduus
s
szd
d
s ReRe
ic
ic
s
sds
x
s
s
ix
'
2
1
primepxpxn k
pnx ln:
1 42
t
10'
xdss
x
s
s
LC
s
LC
R
eRsCj
L
0cos2
2:
R
Critical Region(non-trivial zeros)
ζ (s) = 0trivial zerosζ (s) = 0
26 4
Return to TOC
97
SOLO Primes
Newman’s Proof of the Prime Number Theorem (1980)
Proofs have introduced various simplifications to Hadamard and de la Vallée-Poussin through the use of Tauberian theorems but remained difficult to digest, a surprisingly short proof was discovered in 1980 by American mathematician Donald J. Newman. Newman's proof is arguably the simplest known proof of the theorem, although it is non-elementary in the sense that it uses Cauchy's integral theorem from complex analysis
Donald J. Newman ( 1930 –2007)
Prime Number Theorem 1
ln/lim
xx
xx
Newman’s Proof:
x
x
x
x
xx
xxxx
limlimln/
limSince we proved that it is enough to prove that
1lim x
xx
Newman started by proving that
01
2
xdx
xx
First suppose that exists λ > 1 such that θ (x) ≥ λ x for all x sufficiently large (say x ≥ x0)
0
1
0
21
2222
ud
u
uudx
xu
xuxtd
t
txtd
t
tt x
tu
x
tdud
x
x
x
x
Now suppose that exists λ < 1 such that θ (x) ≤ λ x for all x sufficiently large (say x ≥ x0)
This is a contradiction to
01
2
xdx
xx
0
10
2
1
2222
ud
u
uudx
xu
xuxtd
t
txtd
t
tt x
tu
x
tdud
x
x
x
x
This is a contradiction to
01
2
xdx
xx
Therefore the only possibility is:
1lim
x
xx
98
SOLO Primes
Newman’s Proof of the Prime Number Theorem
Donald J. Newman ( 1930 –2007)
Newman started by proving that
01
2
xdx
xx
This is done in the following steps:
011
0
111
ln: dteezdx
x
xz
x
x
x
xd
p
pz tzt
ex
dtexdzz
ddvxu
vdxzxduz
primepp
z
t
t
z
z
Newman’s Proof (continue – 1):
Define:
Prove that:
002
12
1 tdeetdee
eexd
x
xx tttt
ttex
tdexd
t
t
1: tt eetf
zz
ztdetdeetdetfzF tztzttz 1
1
1:
00
1
0
???0
1
1
1limlim
00
zz
zzF
zz
Apply Analytical Theorem – A Tauberian Theorem
00
1
1
1limlim
1200
xd
x
xx
zz
zzF
zz
q.e.d.
99
SOLO Primes
Newman’s Proof of the Prime Number Theorem
Donald J. Newman ( 1930 –2007)
011
0
111
ln: dteezdx
x
xz
x
x
x
xd
p
pz tzt
ex
dtexdzz
ddvxu
vdxzxduz
primepp
z
t
t
z
z
Newman’s Proof (continue – 1):
Use the Identity:
11
ln
1
ln1ln
tiz
p
p
p
pp
z
zzd
d
zzd
d
primep primepzz
z
111
1
1
zzzz pppp
We found:
11
ln
1
lnln
1
ln
tiz
pp
pz
pp
p
p
p
p
p
z
zzd
d
primepzz
primepzz
primepz
primepz
The sum is:
2/112ln
1
ln2
zzforconvergent
p
p
pp
p
primepz
primepzz
ReRe
100
SOLO Primes
Newman’s Proof of the Prime Number Theorem
Donald J. Newman ( 1930 –2007)
Newman’s Proof (continue – 2):
We found:
1
1
ln
1
lnln
1
ln'
tizpp
pz
pp
p
p
p
p
p
z
z
primepzz
primepzz
primepz
primepz
2/112ln
1
ln2
zzforconvergent
p
p
pp
p
primepz
primepzz
ReRe
Change z to z+1:
We found:
We proved also that:
1
1
ln1
1
1
1
1'
foranalyticpp
p
zzz
z
zzz
z
primepzz
0
1
ln
1
11
1
11
11
1'
foranalyticpp
p
zzz
z
zzz
z
primepzz
0
1
1
1lim
0
zz
zz
Stil need to prove
101
SOLO Primes
Newman’s Proof of the Prime Number Theorem
Donald J. Newman ( 1930 –2007)
Analytical Theorem – A Tauberian Theorem
Newman’s Proof (continue – 3):
Proof of the Analytic Theorem
t
LC
R
R
R
0
T ts
T dtetfsF0Consider the sequence of functions
Those functions are entire (analytic), and we are trying to show that limT→∞ FT (0) exists and is equal to F (0).
Let chose a closed counterclockwise path of integration γR composed from a semicircle γR
+(z) {z ϵ C| |z|≤ R, Re(z)>-δ}, where we choose δ > 0 small enough (depending on R) so that F (z) is analytic inside γR. (Such a δ exists by compactness and the fact that F (z) is analytic for Re (z) ≥ 0)
Let f (t) be a bounded and locally integrable function for t ≥ 0, and suppose that when Re (z) ≥ 0 extends holomorphically to Re (z) ≥ 0. then exists and equals F (0).
0dttf
0dtetfsF ts
102
SOLO Primes
Newman’s Proof of the Prime Number Theorem
Donald J. Newman ( 1930 –2007)
Analytical Theorem – A Tauberian Theorem
Newman’s Proof (continue – 4):
Proof of the Analytic Theorem (continue – 1)
t
LC
R
R
R
0
Let use the Cauchy Theorem to compute
Let f (t) be a bounded and locally integrable function for t ≥ 0, and suppose that when Re (z) ≥ 0 extends holomorphically to Re (z) ≥ 0. then exists and equals F (0).
0dttf
0dtetfsF ts
The additional term z2/R2 was introduced by Newman in order to help the proof.
001
1lim12
12
2
02
2
TzT
Tz
CauchyzT
T FFzR
zezFzFz
z
zd
R
zezFzF
iR
Rz
zd
R
zezFzF
izT
T
2
2
12
1Start with the integral on γR+
zeB
tdetftdetfzFzFTz
T
st
B
tT
stT Re
maxRe
0
2
Re2
*Re
2
22Re
2
2 Re211
R
ze
zR
zzze
zR
zRe
zR
ze TzTzTzzT
R
B
R
ze
z
eBR
z
zd
R
zezFzF
iTz
TzzT
T
R
2Re
Re
2
2 Re2
Re21
2
1
103
SOLO Primes
Newman’s Proof of the Prime Number Theorem
Donald J. Newman ( 1930 –2007)
Analytical Theorem – A Tauberian Theorem
Newman’s Proof (continue – 5):
Proof of the Analytic Theorem (continue – 2)
t
LC
R
R
R
0
Let f (t) be a bounded and locally integrable function for t ≥ 0, and suppose that when Re (z) ≥ 0 extends holomorphically to Re (z) ≥ 0. then exists and equals F (0).
0dttf
0dtetfsF ts
RRRz
zd
R
zezF
iz
zd
R
zezF
iz
zd
R
zezFzF
izT
TzTzT
T
2
2
2
2
2
2
12
11
2
11
2
1
Continue with the integral on γR-
Since FT (z) is entire (analytic in all complex plane we can replace γR- with the left
semicircle CL and obtain
R
B
R
ze
z
eBR
z
zd
R
zezF
iz
zd
R
zezF
iTz
Tz
C
zTT
zTT
LR
2Re
Re
2
2
2
2 Re2
Re21
2
11
2
1
104
SOLO Primes
Newman’s Proof of the Prime Number Theorem
Donald J. Newman ( 1930 –2007)
Analytical Theorem – A Tauberian Theorem
Newman’s Proof (continue – 6):
Proof of the Analytic Theorem (continue – 3)
t
LC
R
R
R
0
Let f (t) be a bounded and locally integrable function for t ≥ 0, and suppose that when Re (z) ≥ 0 extends holomorphically to Re (z) ≥ 0. then exists and equals F (0).
0dttf
0dtetfsF ts
RRRz
zd
R
zezF
iz
zd
R
zezF
iz
zd
R
zezFzF
izT
TzTzT
T
2
2
2
2
2
2
12
11
2
11
2
1
Continue with the integral on γR-
Finally we observed that the integral converges to zero uniformly on compact sets for Re (z) <0 and T→∞, since the integral is the product of independent of T, and ezT, which goes to zero uniformly on compact subsets of γR.
2
2
1R
ze
z
zF zT
2
2
1R
z
z
zF
012
1lim
2
2
Rz
zd
R
zezF
izT
T
105
SOLO Primes
Newman’s Proof of the Prime Number Theorem
Donald J. Newman ( 1930 –2007)
Analytical Theorem – A Tauberian Theorem
Newman’s Proof (continue – 7):
Proof of the Analytic Theorem (continue – 4)
t
LC
R
R
R
0
Let f (t) be a bounded and locally integrable function for t ≥ 0, and suppose that when Re (z) ≥ 0 extends holomorphically to Re (z) ≥ 0. then exists and equals F (0).
0dttf
0dtetfsF ts
tfBR
B
z
zd
R
zezFzF
iz
zd
R
zezFzF
i
z
zd
R
zezFzF
iFF
t
TR
zTT
zTT
zTTT
RR
R
0
2
2
2
2
2
2
max:02
12
11
2
1
12
100
Therefore
0
00lim tdtfFFTT q.e.d.
Return to TOC
106
SOLO
References
Primes
1. Marcus de Sautoy, “The Music of the Primes – Searching to Solve the Greatest Mystery in Mathematics”, Harper-Collins Publishers, 2003
Internet
http://en.wikipedia.org/wiki/
http://www.mathsisfun.com/prime_numbers.html
http://empslocal.ex.ac.uk/people/staff/mrwatkin/zeta/giants.pdf
http://plus.maths.org/content/music-primes
N. Levinson, “A Motivated Account of an Elementary Proof of the Prime Number Theory”, MITK. Chandrasekharan, “Lectures on The Riemann Zeta-Function”, Tata Institute of Fundamental Research, Bombay, 1953
Matt Rosenzweig, “Other Proofs of the Prime Number Theorem”
Jerome Baltzersen, “Hardy’s Theorem and The Prime Number Theorem”, University of Copenhagen, June 2007
G.B. Arfken, H.J. Weber, “Mathematical Methods for Physicists”, Academic Press, Fifth Ed., 2001
107
SOLO
References (continue – 1)
Primes
Internet
B.E. Peterson, “Riemann Zeta Funcyion”, http://people.oregonstate,edu/~peterseb/misc/docs/zeta.pdf
http://mathworld.wolfram.com/RiemannZetaFunctionZeros.html
David Borthwick, “Riemann’s Zeros and the Rhythm of the Primes”, Emory University, November 18, 2009
Ryan Dingman, “The Riemann Hypothesis”, March 12 2010
Laurenzo Menici, “Zeros of the Riemann Zeta-function on the critical lane”, Feb. 4 2012, Universita degli Studi, Roma
P.T. Bateman, H.G. Diamond, “A Hundred Years of Prime Numbers”, http://www.jstor.org
D.J. Newman, “Simple Analytic Proof of the Prime Number Theorem”, The American Mathematical Monthly, Vol. 87, No. 9 (Nov. 1980), pp. 693- 696
M. Baker, D. Clark, “The Prime Number Theorem”, December 24, 2001
http://www.frm.utn.edu.ar/analisisdsys/material/function_gamma.pdf
K.S. Kedlaya, “Analytic Number Theory”, MIT, Spring 2007, “The Prime Number Theorem”
108
SOLO
References (continue – 2)
Primes
Internet
D. Miličić, “Notes on Riemann Zeta Function”, http://www.math.utah.edu/~milicic/zeta.pdf
P. Garrett, “Riemann’ Explicit/Exact formula”, (October 2, 2010), http://www.math.umn.edu/~garrett/m/mfms/notes_c/mfms_notes_02.pdf
http://homepage.tudelft.nl/11r49/documents/wi4006/gammabeta.pdf
http://empslocal.ex.ac.uk/people/staff/mrwatkin/zeta/encoding2.htm
Robert B. Ash, “Complex Variables”, Chapter 7: The Prime Number Theorem, University of Illinois, http://www.math.uluc.edu/~r-ash/CV/CV7.pdf
Physics 116A, “The Riemann Zeta Function”
M. Rosenzweig, “D.J. Newman’s Method of Proof for the Prime Number Theorem”, M. Rosenzweig, “Other Proofs of the Prime Number Theorem”, http://people.fas.harvard.edu/~rosenzw/
“Notes on the Riemann Zeta Function”, January 25, 2007
109
SOLO
References (continue –3)
Primes
Internet
A. Granville, K. Soundarajan, “The Distribution of Prime Number”
E.C. Titchmarsh, “The Zeta-Function og Riemann”, Cambridge at the University Press, 1980
http://www.dartmouth.edu/~chance/chance_news/recent_news/chance_news_10.10.html
http://empslocal.ex.ac.uk/people/staff/mrwatkin/zeta/encoding2.htm
Hans Riesel, “Prime Numbers and Computer Methods for Factorization”, Chapter 2:“The Primes viewed at Large”,
Prime Numbers and the Riemann Zeta Function « Edwin Chen's Blog
D.R. Heath-Brown, “Prime Number Theory and the Riemann Zeta Function”, http://eprints.maths.ox.ac.uk/182/1/newton.pdf
http://cage.ugent.be/~jvindas/Talks_files/Introduction_Tauberians_Distributional_Approach.pdf
110
Marcus Peter Francis du SautoyProf. Of Mathematics Oxford
University
Return to TOC
April 9, 2023 111
SOLO
TechnionIsraeli Institute of Technology
1964 – 1968 BSc EE1968 – 1971 MSc EE
Israeli Air Force1970 – 1974
RAFAELIsraeli Armament Development Authority
1974 – 2013
Stanford University1983 – 1986 PhD AA
112
SOLO Primes
Definition of O: (E. Landau Definition)
We say that f (x) = O (g (x)) if exists a constant k > 0 such that |f (x)| < k |g (x)|
Definition of o
We say that f (x) = o (g (x)) when x → a if 0/lim
xgxfax
Asymptotics
Definition axxgxf ,~means
axxgxgxfisthatxgxfax
,,1/lim o
Definitions
113
SOLO Primes
Definition. Let a Function f: Ω → C,
(a)We say that f ϵ C1 (Ω) iff there exists df ϵ C (Ω, M2 (R), a 2x2 matrix-valued function such that
where d f (s) (h) means that the matrix d f (s) acting on the vector h.(b) We say that f is Holomorphic on Ω if
exists for all s ϵ Ω and is continuous in Ω. We denote this by f ϵ H (Ω). A function f ϵ H (C) is called Entire.
0,2 hRhhohsfdsfhsf
Holomorphic, Entire Functions
sw
sfwfsf
sw
lim:'
Note that (b) is equivalent to the existence of a function f’ ϵ C(Ω) so that
where f’(s) h is the product between the complex numbers f’(s) and h. 0,2 hRhhohsfdsfhsf
114
SOLO Primes
Definition.
A Meromorphic Function is a function whose only singularities, except infinity,are poles.
Meromorphic Functions
E.C. Titchmarch, “Theory of Functions” pg. 284b, 110
A Meromorphic Function in a region if is analytic in the region except at a finite number of poles. The expression is used in contrast to Holomorphic, which is some time used instead of Analytic.
Return to TOC
115
SOLO Primes
Mellin Transform
0
1 xdxfxsFxf sMM
We can get the Mellin Transform from the two side Laplace Transform
Robert Hjalmar Mellin ( 1854 – 1933)
xdxfesFxf sx
2LL2
10
11
0
1
sFxdxfxxdxfxxxfx ssMM
ic
ic
s sdsFxi
x M1- fsfM
2
1
Example:
sxdexe xsx
0
1M
xexf
116
SOLO Primes
Mellin Transform (continue – 1)
0
1 xdxfxsFxf sMM
Relation to Two-Sided Laplace Transformation
Robert Hjalmar Mellin ( 1854 – 1933)
tdexdex tt ,
Let perform the coordinate transformation
tdeeftdeeftdeefesF tsttstttst
0
1M
After the change of functions teftg :
tdetgsGtdeefsF tstst
2LM
Inversion Formula
xfefsdxsFi
sdesGi
tgxe
tic
ic
sexic
ic
tstt
ML
L
2
12
2
1
2
1
c
t
cxdssFxRC
s 0M
RC
R
117
SOLO Primes
Properties of Mellin Transform (continue – 2)
fkk
k
k
fkk
k
k
fz
fk
kk
fa
f
f
s
SszsFstftd
dt
sksksks
SkszsFkstftd
d
SzszsFCztft
SssFsd
dtft
SsasFaRatf
SsFaataf
SsFtf
HolomorphyofStriptdtftsFtftf
M
M
M
M
M
M
M
MM0t,
1
11:
1
,
ln
0,,
0,11
1
0
1
Original Function Mellin Transform Strip of Convergence
118
SOLO Primes
Properties of Mellin Transform (continue – 3)
21
0
21
1
0
1
0
1
//
1
1
11:
1
11:
1
ff
t
t
k
fkk
k
kk
k
fkkk
k
k
f
s
SSssFsFxxdxtfxf
sFsxdxf
sFsxdxf
kssss
SssFstftd
dt
sksksks
SssFkstfttd
d
SsFtf
HolomorphyofStriptdtftsFtftf
M2M1
M
M
M
M
M
MM0t,
Original Function Mellin Transform Strip of Convergence
Return to TOC
119
SOLO Primes
1Re10
1
zxfordte
tzz
t
tt
z
u
uu
z
due
uz
0
1
Proof:
Gamma Function
Change of variables u=nt
t
tnt
zz
t
tnt
z
tde
tntdn
e
ntz
0
1
0
1
Thus for n=1,2,3,…,N
t
tNt
z
z
t
tt
z
z
t
tt
z
z
tde
t
Nz
tde
tz
tde
tz
0
1
02
1
0
1
1
2
1
1
1
0& xyixz
Summing those equationsfor x > 0
t
t
zNtttzzz
tdteeeN
z0
12
1111
2
1
1
1
_________________________________________________
Proof of Riemann's Zeta Function Relations
120
SOLO Primes
Proof (continue – 1): 0& xyixz
Since converges only for Re (z)= x > 1, then letting N → ∞, we obtain for x > 1
1n
zn
Uniform convergence of
t
t
zNtttNzz
tdteee
z0
12
111lim
2
1
1
1
01
1
1
111
1
2
2
tqeeee t
q
q
t
q
t
q
t
allows to interchange between limit and the integral:
RatioGoldentde
ttd
e
ttd
e
tz
t
tt
zt
tt
zt
tt
z
zz
2
51
1112
1
1
1
ln2
1ln2
0
1
0
1
ln2
02
1ln2
0
1ln2
0
1 11
11
t
ttt
xt
tt
xyixzt
tt
z
tdee
ttde
ttd
e
t
The first integral gives
The integral diverges for 0 < x ≤ 1, and converges only for x > 1
1Re10
1
zxfordte
tzz
t
tt
z
Proof of Riemann's Zeta Function Relations
121
SOLO Primes
Proof (continue – 2): 0& xyixz
t
tt
zt
tt
zt
tt
z
zztd
e
ttd
e
ttd
e
tz
ln2
1ln2
0
1
0
1
1112
1
1
1
In the second integral we have
This integral converges only for x > 1, therefore we proved that
ln21 2/ tforee tt
since RatioGoldeneforee ttt
2
5101 2/2/
t
tt
x
termfinite
t
txtu
dtedv
t
tt
xt
tt
xiyxzt
tt
z
tde
txettd
e
ttd
e
ttd
e
t x
t
ln22/
2
ln2
2/1
ln22/
1
ln2
1
ln2
1
12211
1
2/
finite
t
ttxx
xxt
tt
x
tdet
xxxxtermsfinitetde
t
ln22/1
ln22/
1 1212
1Re12
1
1
1
0
1
zxfortde
tzzz
t
tt
z
zz
1Re10
1
zxfordte
tzz
t
tt
z
After [x] (the integer defined such that x-[x] < 1) such integration the power of t in the integrand becomes x-[x]-1 < 0. and we have:
q.e.d.
Proof of Riemann's Zeta Function Relations
Return to TOC
122
SOLO Primes
Proof
The integral can be rewritten as
00
1sin2
1 0
0
1
itoreturnsandzeroencirclesiatstartspaththe
de
izz
zi
i
z
i
iy
x
i
i
2
IntegralIII
i
i
z
originaroundCircleIntegralII
i
i
z
IntegralI
i
i
z
i
i
z
de
de
de
de
1lim
1lim
1lim
11
0
1
0
1
0
0
0
1
Proof of Riemann's Zeta Function Relations
123
SOLO Primes
Proof (continue – 1)
The first integral can be written as
i
iy
x
i
i
2
t
tt
zzi
et
tt
zzi
t
tit
ziiti
i
z
tde
tetd
e
tetd
e
eitd
e
i
0
110 11
1
0
0 1
0 111lim
1lim
The second integral can be written as
0
1
2lim2
1
2lim
21
2lim
1lim
2
020
2
02
1
0
2
02
1
0
21
0
de
deie
e
deie
ed
e
ii
i
i
e
x
i
e
iyxi
i
e
iyxie
originaroundCircle
i
i
z
00
1sin2
1 0
0
1
itoreturnsandzeroencirclesiatstartspaththe
de
izz
zi
i
z
Proof of Riemann's Zeta Function Relations
124
SOLO Primes
Proof (continue – 2)
The third integral can be written as
i
iy
x
i
i
2
t
tt
zzi
et
tt
zzi
t
tit
ziiti
i
z
tde
tetd
e
tetd
e
eitd
e
i
0
11
0
11
1
0
1
0 111lim
1lim
Therefore
t
tt
zt
tt
zzizit
tt
zzizi
i
i
z
tde
tzitd
e
t
i
eeitd
e
teed
e 0
1
0
1
0
10
0
1
1sin2
122
11
But we found that 1Re10
1
zxfordte
tzz
t
tt
z
00
1sin2
1 0
0
1
itoreturnsandzeroencirclesiatstartspaththe
de
izz
zi
i
z
Therefore
0
0
1
1sin2
1 i
i
z
de
izz
z
The right hand is analytic for any z ≠ 1. Since it equals Zeta Function in the half plane x > 1, it is the Analytic Continuation of Zeta to the complax plane for any z ≠ 1.
0
0
1
1sin2
1 i
i
z
de
izz
z
q.e.d.
Proof of Riemann's Zeta Function Relations
Return to TOC
125
SOLO Primes
Proof
0
0
1
12
sin221
i
i
zz
zz
ide
R
RC
C
plane
Re
Im
Let add a circular path of radius R → ∞. On this path
0
1lim
1
2
0
1
d
e
eRd
ei
i
i
R
eR
zi
R
eR
deRdC
z
Therefore we have
d
ed
ed
ed
e
z
C
zi
i
zi
i
z
R1111
110
0
10
0
1
Since the integral is over a closed path in the complex λ plane, we can use the Residue Theorem to calculate it. The residues are given by
,2,121 nnie
1
1
1
110
0
1
222211 n
z
n
zzi
i
z
niiniide
de
Proof of Riemann's Zeta Function Relations
126
SOLO Primes
Proof (continue)
0
0
1
12
sin221
i
i
zz
zz
ide
R
RC
C
plane
Re
Im
11
11
1
1
1
10
0
1 122222
1 nz
zzz
n
z
n
zi
i
z
niiiniiniid
e
2sin22/2/lnln11 z
eeieeiiiiiii izizizizzzzz
znn
z
1
1
11
zzid
ez
i
i
z
12
sin221
0
0
1
q.e.d.
Proof of Riemann's Zeta Function Relations
Return to TOC
127
SOLO Primes
i
iy
x
i
i
2
00
12
1 0
0
1
itoreturnsandzeroencirclesiatstartspaththe
dei
zz
i
i
z
We also found
zzid
ez
i
i
z
12
sin221
0
0
1
Has zeros for
,...4,2,002
sin
zforz
,7,5,301 zforz
z 1 Has no zeros, but has simple poles for z = 1,2,3,4,….
If we return to ζ (z) equation we can see that the zeros of are cancelled by the poles of Γ (1-z). Only the simple pole at z = 1 remain and is the single pole of ζ (s).
0
0
1
1
i
i
z
de
Let find the Residue of this pole:
0
0
1
111 12
1lim11lim1lim
i
i
z
zzzd
eizzzz
1cos
limsin
1lim11lim
1
'
1
1
sin1
1
zzz
zzz
z
HopitalL
z
zzz
z
0
0
1
1 12
1lim
i
i
z
zd
ei
Proof of Riemann's Zeta Function Relations
Return to TOC
128
SOLO Primes
Proof
zzzzz z
1
2sin22sin2
zzid
ez
i
i
z
12
sin221
0
0
1
We found
0
0
1
1sin2
1 i
i
z
de
izz
z
Combining those two relations, we get
zzzzz z
1
2sin22sin2
q.e.d.
Proof of Riemann's Zeta Function Relations
Return to TOC
129
SOLO Primes
Proof
zzzz zz 112/sin2 1
Start from
use
zzzzz z
1
2sin22sin2
zzz
sin1 zzz
1sin
or
zzz
zz
1
2sin2
1
zzzz zz
1
2sin12 1
q.e.d.
Proof of Riemann's Zeta Function Relations Return to TOC
Return to Riemann Zeta Function
130
SOLO Primes
Proof
Start from
use
zzzzz z
1
2sin22sin2
zzz
sin1
zzz
1
sin
21
22
sinzz
z z
z
2
zz
zzz
zz
1
2sin
2/12/
12
1
1
or
zz
zzz zzz
12/1
1122/ 2/12/12/
z
z
z
z zzzz
1
2/12/ 12/12/
Proof of Riemann's Zeta Function Relations
131
SOLO Primes
Proof (continue)
z
z
z
z zzzz
1
2/12/ 12/12/
or
zz
zzz zzz
12/1
1122/ 2/12/12/
2
1
22 12/1 zz
z z
2/12
121 2/1 z
zz z
z
z
1
2
1
2/1
1122/1 z
zzz
therefore
q.e.d. zz
zz zz
1
2
12/ 2/12/
Use LegendreDuplication Formula: 0Re2
22
112
zzzz
z
2/z
z
Proof of Riemann's Zeta Function Relations Return to TOC
132
Jacob Bernoulli1654-1705
The Bernoulli numbers are among the most interesting and important number sequences in mathematics. They first appeared in the posthumous work "Ars Conjectandi" (1713) by Jakob Bernoulli (1654-1705) in connection with sums of powers of consecutive integers. Bernoulli numbers are particularly important in number theory, especially in connection with Fermat's last theorem (see, e.g., Ribenboim (1979)). They also appear in the calculus of finite differences (Nörlund (1924)), in combinatorics (Comtet (1970, 1974)), and in other fields.
Bernoulli Numbers The Bernoulli numbers Bn play an important role in several topics of mathematics. These numbers can be defined by the power series
SOLO
0 !1 n
n
nz n
zB
e
z
133
SOLO Primes
Bernoulli Numbers
0 !1 n
n
n
seriesTaylor
z n
zB
e
z
Let compute the Bernoulli number using
1Residue2
2
!
12
!
11
z
n
eCnzn e
zi
i
n
z
zd
e
z
i
nB
z
R
RC
C
planez
zRe
zIm
The zeros of e z = 1 are at z = ± 2 π i k
1 1
1 12
1'
22
1'
2
1
2
1
2
1!
1lim
1
2lim
1lim
1
2lim2
2
!
1Residue2
2
!
k knn
k knkiz
Hopitall
zkiznkiz
Hopitall
zkiz
z
n
en
kikin
ze
kiz
ze
kizi
i
n
e
zi
i
nB
z
01
x
xn
n
n e
x
xd
dB
134
SOLO Primes
Bernoulli Numbers
0 !1 n
n
nz n
zB
e
z
Let compute the Bernoulli number using
1Residue2
2
!
12
!
11
z
n
eCnzn e
zi
i
n
z
zd
e
z
i
nB
z
R
RC
C
planez
zRe
zIm
The zeros of e z -1 = 1 are at z = ± 2 π i k
1 11 2
1
2
1!
1Residue2
2
!
k knnz
n
en
kikin
e
zi
i
nB
z
oddn
evennk
oddn
evennki
kikik
nn
k
n
kn
kn
0
12
0
2111
2/
111
oddn
evennnn
k
nB n
n
knn
n
n
0
2
!12
1
2
!12
2/
1
2/
,2,1,0
120
222
!212 2
m
mn
mnmm
B m
m
n
Return to Riemann Zeta Function Return to Riemann Zeta Function
135
SOLO Primes Bernoulli Numbers
0 !1 k
k
nz k
zB
e
zLet multiply with
1 !
1m
mz
m
ze
2
1
00
2
1
00
variablesofChange
10
2
01
!
1
!
!
1
!
!!
1
!!
1
11
n
nn
k
k
n
n
k
knkk
knm
k
k
nm
m
k
k
nm
mz
z
zknk
BzB
zknk
BzB
k
zBBz
mz
k
zBz
me
zez m
k
knm
0, knm
0
1,1 nkm
Therefore, equalizing the coefficients of z, from the two side we obtain
10 B 20
!!
11
0
nBknk
n
kk
Algorithm for Bernoulli Numbers Computation
136
SOLO Primes Bernoulli Numbers
0 !1 k
k
nz k
zB
e
zLet multiply with
1 !
1m
mz
m
ze
We obtained 10 B
20!!
!
!!
1!
1
0
1
0
1
0
nBk
nB
knk
nB
knkn
n
kk
n
kk
n
kk
This demonstrates that the Bernoulli numbers are rational, and we have an algorithm to calculate the nth Bernoulli number.
2
1
2
10
!1!1
!2
!2!0
!22 011
1
0
1
BBBBn
6
1
2
31
3
10
!1!2
!3
!2!1
!3
!3!0
!33 22
3
2/1
1
3
1
0
1
BBBBn
Algorithm for Bernoulli Numbers Computation (continue)
Return to TOC
137
SOLO Primes
Proof
i
iy
x
i
i
2
00
1sin2
1 0
0
1
itoreturnsandzeroencirclesiatstartspaththe
de
izz
zi
i
z
We found
and zzz
sin1 zzz
sin1
0
0
12
1 0
0
1
itoreturnsand
zeroencirclesiatstartspaththe
dei
zz
i
i
z
0 1
21 12
!1
12
!1 i
i
n
Cnzn d
ei
n
z
zd
e
z
i
nB
i
iy
x
i
i
2
therefore 1!1
11
n
n Bn
zz
0
0
12
1 0
0
1
itoreturnsand
zeroencirclesiatstartspaththe
dei
zz
i
i
z
zz
nz 11 1
n
Bn nn
,2,11
1 1
nn
Bn nn Bn are the Bernoulli numbers
q.e.d.
We found
Zeta-Function Values and the Bernoulli Numbers
Return to Riemann Zeta Function
138
SOLO Primes
Zeta Function Values and the Bernoulli Numbers
,2,1,0
!22
212 2
2
mBm
m m
mm
zzzz zz
1
2
12/ 2/12/ Let use
with z = 2 m mm
mm mm 212
212 2/21
m
mm
m
mmm
m
m
Bmm
mB
mm
m
mm
mm
2
2/112
2
22/12
2/1
2/1!2
!121
!22
21
2/1
!1
22/1
!121
We found
,3,2,1
2/1!2
!12121 2
2/112
mBmm
mm m
mm
139
SOLO Primes
Zeta Function Values and the Bernoulli Numbers
We found
2/112
2/11
2/1
!12
!121
224212531
121221
12531
212/1
m
m
mm
m
mm
mm
mmmmm
,3,2,1
2/1!2
!12121 2
2/112
mBmm
mm m
mm Therefore
Finally
,2,11
1 1
nn
Bn nn
,3,2,12
121 2 mB
mm m
We also found The two expressionsAgree.
Return to TOC
Return to Riemann Zeta Function
140
SOLO Primes
zzz z 2/: 2/ zz 1We found that
The function η (z) has simple poles at z = 0 of Γ (z/2) and one at z = 1 of ζ (z).
A new function, where those poles are removed ( entire = analytic in all complex plane) and retains the symmetry relation is
zzzzz z 2/12
1: 2/ zz 1
We saw that ζ (z) has trivial zeros at z = -2 n , n=1,2,3,…. Also Γ (z/2) has simple poles at z/2= -1,-2,-3….. Thus for z/2=-1,-2,-3,… the simple poles of Γ (z/2) cancel the trivial zeros of ζ (z).
Therefore the zeros of ξ (z) = 0 are equal to the non-trivial zeros of ζ (z) = 0.
2
1101lim
22lim2/1
2
1limlim0
12/
0
11
21
0
2/
00
zzz
z
z
z
z
zzzz
zzzzzzz
2
12/1
2
12/
2
1lim1lim2/1
2
1limlim1
2/1
2/12/
1
1
1
2/
11
zzzzzzzzz z
zz
z
zz
Zeros of Zeta-Function: ζ (z) = 0
141
SOLO Primes
zzzz z 2/11: 2/ zz 1The zeros of ξ (z) = 0 are equal to the non-trivial zeros of ζ (z) = 0.
For Re {z}=σ > 1, we have
1Re01
1
tizfor
pz
primepz
102/112/
Therefore if ρ is a zero of ζ (z) , so is 1 - ρ i.e. ζ (1-ρ) = 0, and
1Re111Re
The zeros of ξ (z) that are equal to the non-trivial zeros of ζ (ρ) = 0 can exist only on the Critical Strip: 0 < Re (ρ) < 1.
Zeros of Zeta-Function: ζ (z) = 0
01012/2/310
2/1
Suppose ρ is a zero of ζ (z) , i.e. ζ (ρ) = 0 and, therefore, Re {ρ} < 1. Re {ρ} < 1
Since the product contains no zero factors we see that ζ (z) ≠ 0 for σ = Re {z} >1.σ = Re {z} >1
Re0
142
SOLO Primes
zzzz z 2/11: 2/ zz 1The zeros of ξ (z) = 0 are equal to the non-trivial zeros of ζ (z) = 0.
The zeros of ξ (z) that are equal to the non-trivial zeros of ζ (ρ) = 0 can exist only on the Critical Strip: 0 < Re (ρ) < 1.
Zeros of Zeta-Function: ζ (z) = 0
SOLO Primes
zzzz z 2/11: 2/ zz 1Zeros of Zeta-Function: ζ (z) = 0
• ξ (z) is an entire function (analytic in all the complex plane except at ∞)
ξ (z) is regular for Re {z}=σ > 0
ξ (1-z) is regular for Re {1-z}=1-σ > 0, i.e. σ < 1. Since ξ (z)= ξ (1-z) it is regular for both σ > 0 and for σ < 1, meaning for all σ, i.e. ξ (z) is entire.
SOLO Primes
Zeros of Zeta-Function: ζ (z) = 0
• ξ (z) has no zero at the Re{z} = σ = 1
tizpn
zprimep
zn
sRe
1
11
1
Start with
0cos12coscos2121cos2cos432coscos43 222 Suppose that ζ (1+i t) = 0, and consider (Mertens 1898)
tititD 2:, 43 At z=1 the pole of ζ (z) at z = 1 will cancel some of the alleged ζ (1+i t), and 1 + 2 i t may be a zero of ζ (z) but is certainly not a pole. Therefore, if we prove that D (z) does not have a zero at z = 1, than we prove that ζ (z) has no zero on the line Re{z} = σ = 1 line.
Proof:
11
1lnln1
tizpm
pzprimep m
mz
SeriesTaylor
primep
z
tizpm
ppzprimep m
mz
SeriesTaylor
primep
z
primep
z
1
1Re1lnRe1lnln
where we used 1/1ln1
wnwwn
n
SOLO Primes
Zeros of Zeta-Function: ζ (z) = 0
• ξ (z) has no zero at the Re{z} = σ = 1
tizpn
zprimep
zn
sRe
1
11
1
tititD 2:, 43
Proof (continue – 1):
tizpm
ppzprimep m
mz
SeriesTaylor
primep
z
primep
z
1
1Re1lnRe1lnln
Hence
primep m
mtiimtm
primep m
imtm
primep m
imtm
primep m
m
pppm
pm
pm
pm
tititD
1
2
1
2
11
43Re1
1Re
1Re4
1Re3
2lnln4ln3,ln
pmtipmteppmtipmtep pmtiimtpimtimt ln2sinln2cos&lnsinlncos ln2ln
pmtpm
tD mprimep m
mmm
m
ln:02coscos431
,ln1
cos12 2
SOLO Primes
Zeros of Zeta-Function: ζ (z) = 0
• ξ (z) has no zero at the Re{z} = σ = 1
tizpn
zprimep
zn
sRe
1
11
1
tititD 2:, 43 Proof (continue – 2):
pmtpm
tD mprimep m
mmm
m
ln:02coscos431
,ln1
cos12 2
Therefore: 12,43 tititD
1
1lim2lim
1lim1lim
1
,lim
0101
4
01
3
0101
ti
titD
Let find:
Since ζ (z) has a simple pole at z=1
11lim01
If ζ (1+it) has a zero for a t then
1lim
01
it
We see that the left side of the inequality above is finite when σ→1, but the right side is infinite, a contradiction. We conclude that ζ (1+it) ≠ 0. Since t is arbitrary, ζ has no zeros on Re {z} = σ = 1. q.e.d.
Return to TOC
SOLO Primes
The Behavior of ζ (x) as x → 1
1,1ln1
2ln
12ln
2
1
1
1
2
xasxnnx
xn
n
O
xxxx
nx
xxxxx
xxxxxxxxxn
x
n
11
1
2123
1
2
11
2
2
6
1
4
1
2
12
4
1
3
1
2
11
4
1
3
1
2
11
1:
Proof:We have: 1
1
1
xn
xn
x
Define the Dirichlet Eta Function:
Therefore:
1
11
1
21
1
21
1
nx
n
xx nxx
2ln2
11
2ln
1
2ln21
1
1
2ln
1
2ln21
2ln11
1
1
1
21
1
21
1
222ln
1
1
2ln
eTaylorx
x e
Proof of Riemann's Zeta Function Relations
SOLO Primes
The Behavior of ζ (x) as x → 1
1,1ln1
2ln
12ln
2
1
1
1
2
xasxnnx
xn
n
O
Proof (continue – 1):
1
1
1
21
1
nx
n
x nx
2ln2
11
2ln
1
21
1 1
1
x
x
nnnnennnnn n
x
xln1
1
ln1
11111ln1
1
2
1111
1
1
ln1
2lnln1111
O
n
n
n
n
n
nx
nx
n
nn
nnnn
Therefore using we obtain:
1
1 /12lnn
n n
1ln1
2ln
12ln
2
11
ln1
2ln2ln2
11
2ln
11
2
2
2
xnn
nn
n
n
n
n
O
O
q.e.d.
Proof of Riemann's Zeta Function Relations Return to TOC
149
SOLO Primes
Proof
11
11
1
1
tispn
sprimep
sn
s
11
1
1
11
1
1
111
n
n
n
sn
n
s
n
n
n
s
n
ss
n
s dxxdxndxxndsxns
s
1
1
ss extends to an analytic function in the right half plane (σ > 0)
For σ > 1,
Fix n ≥ 1. Observe that for x ϵ [n,n+1],
11
11
nduuduusxnn
n
x
n
sss
Since converges for all σ > 0, we see that
1
1
nn
11
1
1
1
n
n
n
ss xdxns
s
converges uniformly in any closed half plane { σ ≥ ε}, for ε > 0. Thus, the series defines an analytic function in the right half plane { σ ≥ ε}. q.e.d.
Proof of Riemann's Zeta Function Relations
Theorem
150
SOLO Primes
Proof
11
11
1
1
tispn
sprimep
sn
s
01
1:ˆ
foranalytic
sss
1
1'
ss
s
extends to an analytic function in the right half plane (σ ≥ 1)
Define:
q.e.d.
ss
sss
ss
sssss
ss
sss
ss
s
1
ˆ'ˆ1
1
1ˆ11'ˆ
1
1'
1
1' 12
01
1':'ˆ 2
foranalytic
sss
01
11lim1lim:ˆResidue 1s
1
1s1s
sssss
01
1ˆ
1
ˆ'ˆ11lim
1
1'Residue
11s
ss
ssss
ss
ss
Return toIkehara-Wiener Theorem
Proof of Riemann's Zeta Function Relations
Theorem
Return to TOC
151
SOLO Primes
Theorem
Proof
11
11
1
1
tispn
sprimep
sn
s
01
1:ˆ
foranalytic
sss
1
1'
sss
s
extends to an analytic function in the right half plane (σ ≥ 1)
Define:
q.e.d.
sss
ssss
sss
ssssss
sss
ssss
sss
s
1
1ˆ'ˆ1
1
1ˆ11'ˆ
1
1'
1
1' 12
01
1':'ˆ 2
foranalytic
sss
01
11lim1lim:ˆResidue 1s
1
1s1s
sssss
01
11ˆ
1
1ˆ'ˆ11lim
1
1'Residue
11s
sss
sssss
sss
ss
Return to Newman’a Proof
Proof of Riemann's Zeta Function Relations Return to TOC
SOLO Primes
Zeta Function ζ (s) and its Derivative ζ‘ (s)
11
lim
1:
1
1
forconvergestisn
ss
ns
nsN
N
N
nsN
1ln
'lim'
ln:'
1
1
tisn
nss
n
ns
sd
ds
nsN
N
N
nsNN
sp
p
n
ns
primeps
ns
:lnln
'1
1
1
ln1lim
ln1:
ns
kkk
NN
k
N
ns
kk
Nk
kk
N
n
nss
n
ns
sd
ds
Riemann's Zeta Function Relations
Return to TOC
153
SOLO Primes
11
1
tizduuuz
z
zzd
d
z ReRe
Theorem
Define:
Proof
11
ln1
ln1ln
11
1
tiz
pp
p
pp
z
zzd
d
zzd
d
primep primep mmz
Taylor
p
z
z
z
otherwise
kandpprimesomeforpnifpn
k
0
1integerln Von Mangoldt Function1895
The infinite sums are convergent for σ > 1 so we can write
primep k
zpk
primep m
zm
primep mmz
pkppp
pm
lnln1
ln11
11ln111
tizkkkkkpk
z
zzd
d
k
z
k
z
primep k
z
xn
nx :
Proof of Riemann's Zeta Function Relations
154
SOLO Primes
11
1
tizuduuz
z
zzd
d
z ReRe
Theorem
Proof (continue – 1)
11ln111
tizkkkkkpk
z
zzd
d
k
z
k
z
primep k
z
Let compute
zzM
k
zM
k
zM
k
zz
M
k
zzM
k
zzM
k
zM
k
zM
k
z
kkkMMkkkkMM
kkkkMMkkkkkkk
11
111111
1
1
1
1
1
1
20
1
1111
We have 0lnlimlimlim
Mn
primepMp
z
MMn
z
M
z
M k
pMnMMM
1
1
11
1
11
1
1
1
11
1
1
1M
zM
k
k
k
zku
kuk
M
k
k
k
zzzM
k
uduuzuduuzudukzkkk
Proof of Riemann's Zeta Function Relations
155
SOLO Primes
11
1
tizuduuz
z
zzd
d
z ReRe
Theorem
Proof (continue – 2)
1lim1limlim1
11
1
11
10
uduuzuduuzkkkMM
z
zzd
d
zM
z
M
zzM
kM
z
M
q.e.d.
Proof of Riemann's Zeta Function Relations
Return to TOC
156
SOLO Primes
1'
1
1
tizuduuz
z
z
z
zzd
d
z ReRe
We found
0
1 udufuvFvf vMM
ic
ic
s sdsFvi
vvf M1- fM
2
1
ic
ic
z
zdz
x
z
z
ix
'
2
1
The Mellin and the Inverse Mellin Transform of a function f (z) are defined by
From the relation above we can see that is the Mellin Transformation of ψ (x).Therefore we can use the Inverse Mellin Transform to obtain:
zz
z
'
Robert Hjalmar Mellin ( 1854 – 1933)
Proof of Riemann's Zeta Function Relations
Return to TOC
157
SOLO Primes
Proof
tispn
sprimep
sn
s
1
1
11
1
2
11ln1
11lnln
nss
primep nnn
ps
1,
1ln
2
tisxdxx
xss
s
primepxp
xprimesofnumberx 1:
The last equality is true since
otherwise
primenifnn
0
11
21
00
2 1
11ln
11ln1
11ln1
ns
ns
ns n
nn
nn
n
using
we obtain
2 1
11ln
11lnln
nss nn
ns
Proof of Riemann's Zeta Function Relations
158
SOLO Primes
Proof (continue)
1,
1ln
2
tisxdxx
xss
s
primepxp
xprimesofnumberx 1:
2 1
11ln
11lnln
nss nn
ns
Let compute
sss
s
s
s
s
ss
n
n
sn
n
n
ns
sn
ns
nnn
n
n
n
n
n
n
n
xxsxdx
xs
x
sxd
xx
s
1
11ln
11ln
11
11ln
1
11ln
1ln
1lnln11
111 11
therefore 11
ln2
1
n
n
ns
xdxx
sns
hence 1
1ln
2
xdxx
xss
s
q.e.d.
Proof of Riemann's Zeta Function Relations
Return to TOC
159
SOLO Primes
The Riemann Zeta Function can be factored over its nontrivial zeros ρ as the Hadamard Product:
/
2/12ln
1
21
112: ze
z
zz
ez
Hadamard (1893) used the Weierstrass product theorem to derive this result. The plot above shows the convergence of the formula along the real axis using the first 100 (red), 500 (yellow), 1000 (green), and 2000 (blue) Riemann zeta function zeros.
γ is the Euler-Mascheroni constant
γ=0.57721566490153286060651
Hadamard Product of ζ (s)
Jacques Salomon Hadamard
(1865 –1963)
1
22
1
2/
010
21
22/
1
211
1:
n
n
zz
n
n
s
sofzerostrivial
xsba
en
ze
z
z
en
se
s
s
es
zzz
2
1
2
12
2
112
Riemann's Zeta Function Relations
Return to TOC
160
SOLO Primes
Perron’s Formula
11
10
2
1
2:Re aif
aifds
s
a
i ss
s
Oskar Perron
( 1880 – 1975)
1 32
t
10 adss
a
LC
s
10 adss
a
RC
s
LC
RC
R
eRsCj
L
0cos2
2:
R
eRsCj
R
0cos
2:
R
Proof
Define the two semi-circular paths CL (left side), CR (right side) with s=2 as the common origin., and R → ∞.
RLRL
RLRL
C
R
C
R
C
iiRR
C
s
dadRR
a
deRiiRR
ads
s
a
,,
,,
coscos
sincos
sincos
LR
LR
RLRL
CC
CC
C
R
RC
s
R aora
aora
dadss
a
)0cos&1()0cos&1(
)0cos&1()0cos&1(0
limlim,,
cos
161
SOLO Primes
Perron’s Formula
11
10
2
1
2:Re aif
aifds
s
a
i ss
s
1 32
t
10 adss
a
LC
s
10 adss
a
RC
s
LC
RC
R
eRsCj
L
0cos2
2:
R
eRsCj
R
0cos
2:
R
Proof (continue)
We can see tat
10Residue
11lim
1Residue
1Residue
2Re
0
2Re
2Re
as
a
as
as
as
a
as
a
s
Cs
s
s
s
Cs
s
Cs
RR
L
q.e.d.
1Residue
1Residue
1
1
1
1
2
1
2Re
2Re
2Re
2Re
0
2
22:Re as
a
as
a
adss
a
adss
a
adss
a
adss
a
dss
ads
s
a
i s
Cs
s
Cs
Cs
s
Cs
s
C
s
C
s
i
i
s
ss
s
R
L
R
L
R
L
Return to TOC
SOLO Primes
Alfred Tauber ( 1866 – 1942)
Auxiliary Tauberian Theorem
Abel Theorem on Power Series (1826).If the Series is convergent to the number β then
0n nc
01
limn
nn
rrc
Niels Henrik Abel ( 1802 – 1829)
One other statement of Abel Theorem: A possible divergent series is said to be Abel summable to β if the power series has radius of convergence at least 1 and .
0n ncn
n nrc
0
01lim
n
nn
rrc
The genesis of Tauberian Theory is do to Alfred Tauber, that proved in 1897 the following Theorem that gives a sufficient condition for the converse of Abel’s Theorem
Tauber Theorem on Power Series (1897).If and
0n
nnrc
then the Series converges to the number β
0n nc
n
ncn ,
1o
Definition of oWe say that f (x) = o (g (x)) when x → a if 0/lim
xgxf
ax
SOLO Primes
Auxiliary Tauberian Theorem (continue – 1)
John Edensor Littlewood1885 - 1977
Godfrey Harold "G. H." Hardy
] ( 1877 – 1947)
The phrase “Tauberian Theorem” was coined by G.H. Hardy,who along with J.E. Littlewood made a number of contributions in this area.
Generally “Tauberian Theorems” are those in which some type of “ordinary” convergence (e.g. convergence ofeach ), is deduced from some “weaker” type of convergence (e.g. convergence of for each z with Re z>0) provided additional conditions are satisfied (e.g. has an analytic extension to a neighborhood of the each point on the imaginary axis.
0dtetF tyi
Ry
0dtetF tz
0dtetFzG tz
Return to Analytic Theorem
SOLO Primes
Auxiliary Tauberian Theorem (continue – 2)
In 1910 Littlewood gave a weaker condition for convergence then Tauber where he replaced o (1/n) with O (1/n).
then the Series converges to the number β
0n nc
Littlewood Theorem on Power Series (1910).If and
0n
nnrc
n
ncn ,
1O
John Edensor Littlewood1885 - 1977
Godfrey Harold "G. H." Hardy
] ( 1877 – 1947)
Two years after Hardy and Littlewood conjectured and later proved the following:
Hardy and Littlewood TheoremLet be convergent for |r| < 1. Suppose that for some number α ≥ 0
0n
nnrc
Crcrn
nn
r
0
1lim
If 1 nallfornMcn n
then
1
','0
CCwherenCc
nn
kk
Definition of O:We say that f (x) = O (g (x)) if exists a constant k > 0 such that |f (x)| < k |g (x)|
The phrase “Tauberian Theorem” was coined by G.H. Hardy.
SOLO Primes
Auxiliary Tauberian Theorem (continue – 3)
In 1931 Ikehara, a student of Norbert Wiener, showed the following Tauberian Theorem for Dirichlet Series. His aim was to give a proof of the Prime Number Theorem (PNT) in the form
1lim x
xx
Ikehara-Wiener Theorem (1931)
Let F be given by the Dirichlet Series
1,1
sforconvergentn
csF
nsn Re
where the coefficients satisfy the Tauberian condition cn ≥ 0. If there exists a constant β such that
1
z
zF
admits a continuous extension to the line Re z = 1, then
N
nn
Nc
N 1
1lim
Shikao Ikehara (1904 –1984)
Norbert Wiener ( 1894 – 1964 )
SOLO Primes
Auxiliary Tauberian Theorem (continue – 4)Ikehara-Wiener Theorem (1931)
Let F be given by the Dirichlet Series 1,1
sforconvergentn
csF
nsn Re
where the coefficients satisfy the Tauberian condition cn ≥ 0. If there exists a constant β such that
1
zzF
admits a continuous extension to the line Re z = 1, then
N
nn
Nc
N 1
1lim
Proof of PNT
1
1ln
'ln:
11
tis
n
n
pp
s
ss
sd
dsF
ns
primep mmsChoose
1
1'
ss
s
extends to an analytic function in the right half plane (σ ≥ 1)
Therefore ncn :We proved
According to Ikehara-Wiener Theorem with β = -1
1lim
1lim
1lim
1
x
xn
xc
N xxn
x
N
nn
N
1/lim
xxx
q.e.d.
SOLO Primes
Auxiliary Tauberian Theorem (continue – 5)
Tauberian LemmaLet f (x) be a function on [2,∞) and suppose x f (x) monotone non-decreasing on [2,∞). Let m and n be real numbers, n ≠-1. If
then
xx
xtdtf m
nx
ln~
1
2
xx
xnxf m
n
ln
1~
Proof:
Let x ≥ 2, ε > 0 and x (1-ε) ≥ 2
111
1lnx
x
x
x
x
x
xfxt
tdxfx
t
tdtfttdtf
and
x
x
x
x
x
x
xfxt
tdxfx
t
tdtfttdtf
111
1ln
SOLO Primes
Auxiliary Tauberian Theorem (continue – 6)
Proof (continue – 1):
Let ε > 0. By hypothesis there exists Aε ≥ 2 such that x ≥ Aε
m
n
m
nnxxx
x x
x
x
xtdtftdtftdtfxfx
ln
1
1ln
111ln
21211
2
1
2
1
xx
xtdtf
x
xm
nx
m
n
ln
1
ln
1 21
2
21
thus if 0 < ε < 1 and then
Ax ,
1
2max
mnn
m
nxxx
x x
x
x
xtdtftdtftdtfxfx
1ln
11
ln
11ln
211211
221
Tauberian LemmaLet f (x) be a function on [2,∞) and suppose x f (x) monotone non-decreasing on [2,∞). Let m and n be real numbers, n ≠-1. If
then
xx
xnxf m
n
ln
1~
xx
xtdtf m
nx
ln~
1
2
SOLO Primes
Auxiliary Tauberian Theorem (continue – 7)
Proof (continue – 2):
Tauberian LemmaLet f (x) be a function on [2,∞) and suppose x f (x) monotone non-decreasing on [2,∞). Let m and n be real numbers, n ≠-1. If
then
xx
xnxf m
n
ln
1~
xx
xtdtf m
nx
ln~
1
2
If follows that if 0 < ε < 1 then
1ln
111lnsuplim
221n
n
m
x x
xfx
1ln
111lninflim
212 n
n
m
x x
xfx
11/1lim
221111lim
1ln
111lim
0
12
0'221
0
n
n nnHopitalLn
11/1lim
211112lim
1ln
111lim
0
12
0'212
0
n
n nnHopitalLn
SOLO Primes
Auxiliary Tauberian Theorem (continue – 8)
Proof (continue – 3):
Tauberian LemmaLet f (x) be a function on [2,∞) and suppose x f (x) monotone non-decreasing on [2,∞). Let m and n be real numbers, n ≠-1. If
then
xx
xnxf m
n
ln
1~
xx
xtdtf m
nx
ln~
1
2
If follows that as x → ∞ then
1
lnlim
n
x
xfxn
m
x
therefore
q.e.d.
m
n
mnx x
xnxf
xxn
xf
ln
1~1
ln/1lim
SOLO Primes
Auxiliary Tauberian Theorem (continue – 9)
Chebyshev Function Method
Since
0
1'xdxx
ss
s s
Using Mellin’s Inverse Transform we have
ic
ic
s sdxss
s
ix
'
2
1
By the contour integral we obtain the Psi von Mangoldt formula of 1895
1 42
t
10'
xdss
x
s
s
LC
s
LC
R
eRsCj
L
0cos2
2:
R
Critical Region(non-trivial zeros)
ζ (s) = 0trivial zerosζ (s) = 0
26 4
2/12
0Re0
1
1ln0
0'ln:
xx
xpx
mprimep
xpm
We then use this formula to deduce 2
~2
1
xtdt
x
This part uses the fact that are no roots on Re s = 1. Then the Tauberian Lemma, yields xx ~There are some variants of this method:1.Hadamard estimated
2.La Valée Poussin estimated
xtd
t
t1 2
xtd
t
t1
SOLO Primes
Auxiliary Tauberian Theorem (continue – 10)
La Valée Poussin Function Method
Define
0
1'xdxx
ss
s s
Using Mellin’s Inverse Transform we have
ic
ic
s sdxss
s
ix
21
'
2
1
1 42
t
10'
xdss
x
s
s
LC
s
LC
R
eRsCj
L
0cos2
2:
R
Critical Region(non-trivial zeros)
ζ (s) = 0trivial zerosζ (s) = 0
26 4If we estimate the contour integral we obtain ψ1 (x) ~ x. Then the Tauberian Lemma, yields.
10:1
xtd
t
tx
1~
x
x
ic
ic
s sdxss
s
ix
'
2
1
ic
ic
sic
ic
xs
xic
ic
sx
sdss
x
ss
s
itdtsd
ss
s
it
tdsdt
ss
s
idt
t
t
'
2
1'
2
1'
2
1 1
Given Mellin Transform of Chebyshev ψ (x) and its Inverse:
Charles-Jean Étienne Gustave Nicolas de la Vallée Poussin
(1866 1962)
SOLO Primes
Auxiliary Tauberian Theorem (continue – 11)
Riemann’s Function MethodRiemann didn’t prove the Prime Number Theorem but he did have the ingredients described here
0 1
lnxd
xx
x
s
ss
Since
1
1lnxdxxJ
s
s s
1
1
4
1
3
1
2
1 1
4
1
3
1
2
1:
n
nxn
xxxxxJ
Then using Mellin’s Inverse Transform
ic
ic
s sdxs
s
ixJ
ln
2
1
This integral is only conditionally convergent.We estimate and deduce
Then
xxxJ ln/~
xxxxxxxJx ln/ln/ln/2/1 oO
and
Return to TOC
174
SOLOInfinite Series
Given a series:
Theorems of Convergence of Sequences and Series
n
iin uS
1Convergence Definition:
The series Sn converges to S as n →∞ if for all ε > 0 there exists an positive integer N such that
If no such N exists then we say that the series diverges.
NnallforSuSSn
iin
1
Convergence Theorem:The series Sn converges as n →∞ if if and only if there exists an positive integer M such that
If no such M exists then we say that the series diverges.
11
NallforMuSN
iiN
If S is unknown we can use the Cauchy Criterion for convergence: for all ε > 0 there exists an positive integer N such that
NmnallforuuSSm
jj
n
iimn
,11
Augustin Louis Cauchy ) 1789-1857(
A necessary (but not sufficient) condition for convergence is that lim i→∞ ui = 0
175
SOLO Complex Variables
Let {un} :=u1 (z), u2 (z),…,un (z),…, be a sequence of single-valued functions of z insome region of z plane.
We call U (z) the limit of {un} ,if given any positive number ε we can find a number N (ε,z) such that and we write this: zNnzUzu n ,
zUzuorzUzun
nnn
lim
x
y C
R
If a sequence converges for all values z in a region R, we call Rthe region of convergence of the sequence. A sequence that is notconvergent at some point z is called divergent at z.
Infinite Series
Return to TOC
176
SOLO Complex VariablesInfinite Series
Series of Functions From the sequence of functions {un} let form a new sequence {Sn} defined by:
n
i
inn zuzuzuzuzS
zuzuzS
zuzS
1
21
212
11
If , the series is called convergent and S (z) is its sum. zSzS nn
lim
A necessary (but not sufficient) condition for convergence is that lim n→∞ un(z) = 0
Example: The Harmonic Series
nnn
1
4
1
3
1
2
11
1
1
01
limlim n
un
nn
By grouping the terms in the sum as
2
1
22
1
2
1
1
2
1
1
1
8
1
7
1
6
1
5
1
4
1
3
1
2
11
p
p
pppp
Return to TOC
177
SOLO Complex Variables
Absolute Convergence of Series of Functions
Given a series of functions:
n
i
in zuzS1
If is convergent the series is called absolutely convergent.
n
i
i zu1
If is convergent but is not, the series is called conditionally convergent.
n
i
i zu1
n
i
i zu1
Uniformly Convergence of Sequences and Series
If for the sequence of functions {un(z)} we can find for each ε>0 a number N (ε)
such that for all zR we say that {un} uniformlyconverges to U (z). ( N is a function only of ε and not of z)
NnzUzu n
If the series of functions {Sn(z)} converges to S (z) for all zR we define the remainder
1
:nz
inn zuzSzSzR
The series of functions {Sn(z)} is uniformly convergent to S (z)
if for all for all ε>0 and for all zR we can find a number N (ε)
such that NnzSzS n
x
y C
R
Return to TOC
178
SOLO
z
zofzerosn
n
z
z
z
n
sin
,2,11sin
12
2
zofzerosn
enz
ez
zte
n
n
zz
zt
1
,2,1
1
1
1
0
1
Euler’s Product
2/12/2/
1
2
010
12ln
0
1
2/2/
211
12
11
z
e
zz
e
n
n
z
zeroszTrivialzerosztrivialNon
z
zofpole
z
primep
z
zz
en
ze
z
z
epz
Weierstrass Product
Hadamard Product
1
22 sin1
1
n
zz
n
zz
zz
010
2/12ln
12/112
Re
ss
es
ss
es
Infinite Products
179
SOLO Infinite Products
In 1735 Euler solved the problem, named “Basel Problem” , posed by Mengoli in 1650, by showing that
6
1
4
1
3
1
2
11
2
12232
n n
122
2
2
2
2
2
2
2
19
14
11sin
k k
xxxx
x
x
He did this by developing an Infinite Product for sin x /x:
The roots of sin x are x =0, ±π, ±2π, ±3π,…. However sin x/x is not a polynomial, but Euler assumed (and check it by numerical computation) that it can be factorized using its roots as
We now that if p (x) and q (x) are two polynomials, then using the roots of the two polynomials we have:
m
n
qqqq
pppp
xxxxxxa
xxxxxxa
xq
xp
21
21
We want to show how to express a general solution for complex function f (x) using the zeros and the poles (finite or infinite) of f (x).
Return to TOC
180
SOLO Infinite Products
The Mittag-Leffler and Weierstrass Theorems
Magnus Gösta Mittag-Leffler1846 - 1927
Karl Theodor Wilhelm Weierstrass
(1815 – 11897)
We want to answer the following questions:
• Can we find f ϵ M (C) so that f has poles exactly a prescribed sequence {zn} that does not cluster in C, and such that f has prescribed principal parts (residiu) at these poles (this refers to fixing the entire portion of the Laurent Series with negative powers at each pole)?
A positive answer to this question was given by Mittag-Leffler
• Can we find f ϵ H (C) so that f has zeros exactly at a given sequence {zn} ?
A positive answer to this question was given by Weierstrass
Return to TOC
181
SOLO Infinite Products
Definition 1:We say that the Infinite Product converges, if for any N0 > iN the limit
exists and is nonzero.
If this is satisfied then we can compute
N
Nj iN
N
Nj iN
N
Ni iN
N0000lnlimlnlimlimlnln
We transformed the Infinite Product in an Infinite Series, and we know that a necessary (but not sufficient) condition for an Infinite Series to converge is
1lim0lnlim j
jj
j
For simplicity we will define
0lim1 j
jjj aa
1j j
00lim N
N
Nj jN
182
SOLO Infinite Products
Lemma 2:Let aj ϵ C be such that |aj| < 1. Let . Then
N
j jN aQ1
1:
Nj j
Nj j a
N
aeQe 112
1
Proof:
Since 1 + |aj| ≤ e |aj|
N
j j
N
a
Q
N eaa 111 1
On the other hand, since ex ≤ 1 + 2 x for 0 ≤ x ≤ 1,
NN
aaa
QaaeeeNj
jNj
jNNj j
2/212/21 122
22
111
11 q.e.d.
Proof: Suppose . Then, by the previous Lemma, QN ≤ eM, for all N. Since Q1 ≤Q2 ≤ …., the sequence of “partial products” {QN} converges.Conversely, if the Infinit Product converges to Q, then Q ≥ 1 andfor all N. Then converges.
Maj j
11
1j ja
QaN
j j ln21
Lemma 3:Let aj ϵ C be such that |aj| < 1. Then converges if and only if converges.
11
j ja
1j ja
q.e.d.
183
SOLO Infinite Products
Proof: Since the product converges, then |aj| → 1, so that aj ≠ 0 for j ≥ j0. Let assume j0 = 1, and define
11
j ja
N
j jN
N
j jN aQandaP11
1:,1:
Note that for a suitable choice of indexes ajk
N
n
n
k j
N
j jN kaaP
1 1111:
Then 111 11 1
N
N
n
n
k j
N
n
n
k jN QaaPkk
and for N, M > 1, N > M
MN
n
Mj jM
n
Mj j
M
j j
NMN
j
M
j jjMN
QQaQ
aaaaPP
11
11111
1
111 1
Hence, {PN} is a Cauchy Sequence, since {QN} is, and it converges.
Lemma 4:If the infinite product converges, then also
converges. Hence if the series converges, also converges.
11
j ja
11
j ja
11
j ja
1j ja
184
SOLO Infinite Products
Proof (continue – 1):
We need to prove that {PN} does not converge to zero. By Lemma 2
2
31
NMj jaN
Mj j ea
for M ≥ j0, and N > M. Then using
2
11
2
31111
N
Mj j
N
Mj j aa
for M ≥ j0, and N > M. Hence 2
11
N
Mj ja
so that
012
111limlim 0
11
j
j j
N
Mj j
M
j jj
Nj
aaaP
q.e.d.
11 NN QP
Lemma 4:If the infinite product converges, then also
converges. Hence if the series converges, also converges.
11
j ja
11
j ja
11
j ja
1j ja
Return to TOC
185
SOLO Infinite Products
Start with some introductory results:
sf
sfsf
sd
d 'ln
TheoremLet f (s) be entire holomorphic (analytic for all s ϵ C) and f (s) ≠ 0 everywhere. There is an entire function g (s) for which f = eg.
Proof:
Since f (s) ≠ 0 and entire, f’ (s) is also entire, and so is f’(s)/ f (s), therefore
entireissf
sd
d
sf
sfsg
sd
dln
':
and taking g (0)= 1 we obtain sgesf q.e.d.
CorollaryIf f (s) is entire holomorphic (analytic) with finitely many zeros {ai≠0}(with multiplicity) and m zeros at s=0, then there exists an entire g (s) such that
nsgm asessf /1
Proof:
Since is entire with no zeros we can apply the Theorem nm asssf /1/
q.e.d.
The Weierstrass Factorization Theorem
Karl Theodor Wilhelm Weierstrass
(1815 – 11897)
186
SOLO Infinite Products
The Weierstrass Factorization Theorem
DefinitionWe define the Weierstrass Elementary Factors as
,2,11
01,
2
2
nes
nsnsE
n
sss
n
LemmaFor |s| ≤ 1, |1 – E (s,n)| ≤ |s|n+1.
Proof: The case n = 0 is trivial. Let n ≥ 1. Let differentiate E (s,n)
n
sss
nn
sss
nn
sss
n
sss
nn
sss
nnnnn
eseseesssensEsd
d
222212
22222
111,
By developing in a Taylor series
0, 2
2
knk
kk
n
sss
n bsbesnsEsd
dn
0
10
1,,k
kk
k
kk saknsE
sd
dsansE
,2,10
0
1,0
21
0
jjn
ba
aaa
nEa
jnjn
n
Karl Theodor Wilhelm Weierstrass
(1815 – 11897)
Inspired by the fact that
321
1ln&11
321
1ln ss
ss
es s w have the following
187
SOLO Infinite Products
The Weierstrass Factorization Theorem
DefinitionWe define the Weierstrass Elementary Factors as
,2,11
01,
2
2
nes
nsnsE
n
sss
n
LemmaFor |s| ≤ 1, |1 – E (s,n)| ≤ |s|n+1.
Proof (continue – 1):
01,1
k
nk
kk asansE
So for |s| ≤ 1
1
0
1
1
1
1
11
1
11
1
11
1
,11
,1
nn
nkk
n
nkk
ns
nk
nk
k
n
nk
nkk
n
nk
kk
snEsasas
sassassansE
q.e.d.
188
SOLO Infinite Products
The Weierstrass Product
Let {sj} be a sequence of complex numbers such that limj→∞ |sj|=+∞. We may assume that 0 < |s1| ≤ |s2| ≤… Let {pj} be integers. Then the Weierstrass Product defined as
converges uniformly on every set {|s|≤r}, to a Holomorphic Entire function F. The zeros of F are precisely the points {sj} counted with the corresponding multiplicity.
1
1
2
1
1
2
1,j
s
s
ps
s
s
s
jj j
j
jp
jjjjes
sp
s
sE
Proof:Let r > 0 be fixed. Let j0 be such that |sj| > r for j ≥ j0. Thus,
11
1,
jj
p
j
p
jj
j s
r
s
sp
s
sE
By the hypothesis on the pj’s,
00
1
1,jj
p
jjj j
j
j
s
rp
s
sE
By Weierstrass M (Majorant Test) it follows that converges uniformly on {|s| ≤ r}, for any r > 0. Then exist C > 0 such that
01,/
jj jj pssE
C
jj
ps
sEp
s
sE
jj jj
eeeCps
sE
jj
jj jj
0
0
0
1,1,
1,
C
jj
pz
zE
jj jj
jj jj
jj
pz
zE
eepz
zEp
z
zEe
jj
Taylorj
j
0000
1,,
1,1,
189
SOLO Infinite Products
The Weierstrass Product
Let {sj} be a sequence of complex numbers such that limj→∞ |sj|=+∞. We may assume that 0 < |s1| ≤ |s2| ≤… Let {pj} be integers. Then the Weierstrass Product defined as
converges uniformly on every set {|s|≤r}, to a Holomorphic Entire function F. The zeros of F are precisely the points {sj} counted with the corresponding multiplicity.
1
1
2
1
1
2
1,j
s
s
ps
s
s
s
jj j
j
jp
jjjjes
sp
s
sE
Proof:Let r > 0 be fixed. Let j0 be such that |sj| > r for j ≥ j0. Thus,
11
1,
jj
p
j
p
jj
j s
r
s
sp
s
sE
By the hypothesis on the pj’s,
00
1
1,jj
p
jjj j
j
j
s
rp
s
sE
By Weierstrass M (Majorant Test) it follows that converges uniformly on {|s| ≤ r}, for any r > 0. Then exist C > 0 such that
01,/
jj jj pssE
C
jj
ps
sEp
s
sE
jj jj
eeeCps
sE
jj
jj jj
0
0
0
1,1,
1,
C
jj
pz
zE
jj jj
jj jj
jj
pz
zE
eepz
zEp
z
zEe
jj
Taylorj
j
0000
1,,
1,1,
190
SOLO Infinite Products
The Weierstrass Factorization Theorem
LemmaLet {zj} be a sequence of complex numbers such that limj→∞ |zj|=+∞. Then there exists an entire function F whose zeros are precisely the {z j}, counting multiplicity.This function is
11,:
kjj
k jz
zEssF
Return to TOC
191
SOLO Infinite Products
The Hadamard Factorization Theorem
Definition: Order of an Entire FunctionAn Entire (analytic for all z ϵ C) Function f is said to be of Order ρ, 0 ≤ ρ ≤ +∞, if
meaning that
rasezf r
rz
Osupinf:
0
CzallforeAzfBAexists zB
:0,inf:
0
Examples:
(1) Polynomials have Order 0. Let N be the degree of p (z)
for all ε > 0 and a suitable constant Cε .
raseCrCazazazp rNnn
01
(2) The exponential ex has order 1, and more generally, have order n
and no smaller power of r would suffice.(3) sin z, cos z, sinh z, cosh z have order 1.(4) exp {exp z} has infinite order.
nnnn rzzr eeee Re
nxe
Return to TOC
192
SOLO Complex Variables
Mittag-Leffler’s Expansion Theorem
Magnus Gösta Mittag-Leffler1846 - 1927
1
110
n nn
n aazafResfzf
Suppose that the only singularities of f (z) in the z-plane are thesimple poles a1, a2,…, arranged in order of increasing absolutevalues. The respective residues of f are Res { f (a1)}, Res { f (a2)}, …
C
x
y
RN
1ana
CN
Proof:
Assume ξ is not a pole of f (z), then has simple polesat a1, a2,…, and ξ.
z
zf
Residue of at an, n = 1,2,… is z
zf
n
nnaz a
afRes
z
zfaz
n
lim
Residue of at ξ is z
zf
fz
zfz
naz
lim
Let take a circle CN at the origin with a radius RN → ∞
By the Residue Theorem
NNCinn n
n
Ca
afResfdz
z
zf
Assume f (z) is analytic at z = 0, then NN
Cinn n
n
Ca
afResfdz
z
zf0
193
SOLO Complex Variables
Mittag-Leffler’s Expansion Theorem (continue – 1)
C
x
y
RN
1ana
CN
Proof (continue – 1):
Let take a circle CN at the origin with a radius RN → ∞
NN
Cinn n
n
Ca
afResfdz
z
zf
i
2
1
NN
Cinn n
n
Ca
afResfdz
z
zf
i0
2
1
NN
N
CC
Cinn nn
n
dzzz
zf
idz
zzzf
i
aaafResff
2
11
2
1
110
Since | z-ξ | ≥ | z | - | ξ |=RN - | ξ | for z on CN, we have if | f(z) | ≤ M
0
2limlim
NN
N
RC
R RR
RMdz
zz
zfN
N
N
0lim
N
N
CR
dzzz
zf
1
110
n nn
n aazafResfzf
Therefore using this result and ξ → z, we obtain
q.e.d.
Return to TOC
194
SOLO Complex Variables
Generalization of Mittag-Leffler’s Expansion Theorem
q.e.d.
Suppose that the only singularities of f (z) in the z-plane are the poles a1, a2,…, arranged in order of increasing absolute values, and having Higher Order then One. The respective residues of f are Res { f (a1)}, Res { f (a2)}, … Suppose that exists a Positive Integer p such that for |z| = RN
|f (z)| < RNp+1
and the poles a1, a2,…, an are all inside the Circle of Radius RN around the origin (|a1|≤ |a2|≤…≤ |an | < RN). Then
p
i jp
j
p
jjjj
ii
j jp
j
p
ip
p
a
z
a
z
aazaf
i
zf
aza
zaff
p
zf
zfzf
1 112
11
11
11Res
!
0
Res0!
0!1
0
Proof: Start with the Integral
Nj
N
Cina jp
j
j
pwpzw
Cp
zaa
af
zww
wf
zww
wf
dwzww
wf
iI
1101
1
ResResRes
2
1
C
x
y
RN
1ana
CN
Return to Infinite Product
195
SOLO Complex Variables
Generalization of Mittag-Leffler’s Expansion Theorem
Proof (continue – 1):
but
111limRes
ppzwpzw z
zf
zww
wfzw
zww
wf
C
x
y
RN
1ana
CN
i
i
ip
pp
iw
pp
p
p
wpw
wd
wfd
zwwd
d
ipi
p
p
zww
wfw
wd
d
pzww
wf
1
!!
!
!
1lim
!
1limRes
1
00
11
010
1
1 !11
ip
ip
ip
p
zw
ip
zwwd
d
p
iip
i
p
ii
i
ip
ip
wpw
zi
f
wd
wfd
zw
ip
ipi
p
pzww
wf
01
01010
!
0
!1
!!
!
!
1limRes
Therefore
Leibnitz Formula for RepeatedDifferentiation of a Product
196
SOLO Complex Variables
Generalization of Mittag-Leffler’s Expansion Theorem
Proof (continue – 2):
but
Nj Cina j
pj
jp
iip
i
p zaa
af
zi
f
z
zf1
011
Res
!
0
C
x
y
RN
1ana
CN
Therefore
Nj
N
Cina jp
j
j
pwpzw
Cp
zaa
af
zww
wf
zww
wf
dwzww
wf
iI
1101
1
ResResRes
2
1
0max2
2
1
2
11max
11
N
pN
NCN
N
Rn
RwfCN
pN
N
Cp
wfzRR
Rdw
zww
wf
iI
0
Res
!
0
11
011
j jp
j
jp
iip
i
p zaa
af
zi
f
z
zf
11
1
0
Res
!
0
j jp
j
pj
p
i
ii
aza
zaf
i
zfzf
197
SOLO Complex Variables
Generalization of Mittag-Leffler’s Expansion Theorem
We can see that for p = 0 we get
C
x
y
RN
1ana
CN
11
11Res0
Res0
n nnn
n nn
n
aazaff
aza
zaffzf
We recovered the Mittag-Leffler’s Expansion Theorem
11
1
0
Res
!
0
j jp
j
pj
p
i
ii
aza
zaf
i
zfzf
112
11
111
ResRes
jp
j
p
jjjj
j jp
j
pj
a
z
a
z
aazaf
aza
zaf
q.e.d.
Proof (continue – 3):
Return to TOC
198
SOLO Complex Variables
Expansion of an Integral Function as an Infinite Product
An Integral Function is a function which is Analytic for all finite values of z.For example ez, sin z, cos z are Integral Functions. An Integral Function may be regarded as a generalization of a Polynomial.
Let f (z) be an Integral Function (no Poles) with Simple/Non-simple Zeros at a1, a2,…,an,.., arranged in increasing order (|a1|≤ |a2|≤…≤|an|≤…. ). Suppose that exists a Positive Integer p such that for |z| = RN
|f (z)| < RNp+1
and the Zeros a1, a2,…, an are all inside the Circle of Radius RN around the origin (|a1|≤ |a2|≤…≤ |an | < RN).Then f (z) can be expanded as an Infinite Product (Hadamard):
1
1
1
2
11
1
2
2
111 10
j
a
z
pa
z
a
z
j
zczc pj
p
jjp
p ea
zefzf
C
x
y
RN
1ana
CN
Note:1.The minimum p for which |f(z)|<RN
p+1 is called the Order of f(z)2.If f(z) has no poles or zeros then the previous relation reduces to
1110
pp zczcefzf
The Hadamard Factorization Theorem
Return to TOC
199
SOLO Complex Variables
Expansion of an Integral Function as an Infinite Product
Proof:
C
x
y
RN
1ana
CN
Let compute: zf
zfzf
zd
d 1
ln
1limlimRes1
21'11
f
fazf
f
faz
f
f j
az
HopitalLj
azaz
jjj
Define
pii
ff
zdd
c z
i
i
i ,,1,0!1
: 0
1
1
112
01
1 111
jp
j
p
jjj
p
i
ii
a
z
a
z
aazzic
zf
zf
All Zeros of f (z) (a1, a2,…,an,..) are Simple Poles of f(1)(z)/f(z), therefore we can apply the previous result and write:
1
12
1
0
0
1
1 11Res
! jp
j
p
jjjaz
p
i
i
z
i
i
a
z
a
z
aazf
f
i
zf
fzd
d
zf
zf
j
The Hadamard Factorization Theorem
200
SOLO Complex Variables
Expansion of an Integral Function as an Infinite Product
Proof (continue – 1):
C
x
y
RN
1ana
CN
Integrating from 0 to z along a path not passing through any of aj, we obtain
1
1
1
2
2
0
11 1
1
2
1ln
0ln
jp
j
p
jjj
jp
i
ii
a
z
pa
z
a
z
a
azzc
f
zf
The values of the logarithms will depend on the path chosen, but when we take exponentials all the ambiguities disappear,
112
01
1 111
jp
j
p
jjj
p
i
ii
a
z
a
z
aazzic
zf
zf
1
1
1
2
11
1
2
2
0
11
10 j
a
z
pa
z
a
z
j
zc pj
p
jj
p
i
ii
ea
ze
f
zf
q.e.d.
If |f(z)| < RNp+1 it will be true for all q > p. If we choose the ρ = min p for which
the inequality holds, then we obtain the Hadamard’s Factorization .
The Hadamard Factorization Theorem
Return to TOC
201
SOLO Primes
Hadamard Infinite Product Expansion of Zeta Function
Graph showing the Trivial Zeros, the Critical Strip and the Critical Line of ζ (z) zeros.
1
1
1
2
11
1
2
2
111 10
j
a
z
pa
z
a
z
j
zczc pj
p
jjp
p ea
zefzf
Since (z-1) ζ (z) is Analytic and has only Zeros we can use the Hadamard Infinite Product Expansion
Zeta Function ζ (z) has Order p=0
2
1
2
10 1 B
The Zero of the Zeta Function ζ (z) are-Trivial Zeros at z=-2n, n=1,2,…- Nontrivial Zeros ρ on the Critical Zone 0 < Re ρ < 1
1
2
0102/10
21101 1
n
n
z
zofzerostrivial
z
zofzerosnontrivial
zc
fzf
en
ze
zezz
Hadamard Infinite Product Expansion of (z-1) ζ (z) is:
pii
ff
zdd
c z
i
i
i ,,1,0!1
: 0
1
1
12ln2/1
2/2ln2/1
0
0'0:
1
0
1
1
zzzf
zf
fc
2
10&
2
2ln0'
1
1
z
forconverges
nzn
z
202
SOLO Primes
Hadamard Infinite Product Expansion of Zeta Function (continue)
Graph showing the Trivial Zeros, the Critical Strip and the Critical Line of ζ (z) zeros.
1
2
010
12ln
211
21
n
n
z
zofzerostrivial
z
zofzerosnontrivial
z
en
ze
zezz
1
22
21
22/
1
n
n
zz
en
ze
z
z
Hadamard Infinite Product Expansion of (z-1) ζ (z) is:
We found the Weierstrass Expansion for the Gamma Function:
100
2/12ln
12/112
Re
zz
ez
zz
ez
2
122
21
22
1
2
ze
zze
en
zzz
n
n
z
Hadamard (1893) used the Weierstrass product theorem to derive this result. The plot above shows the convergence of the formula along the real axis using the first 100 (red), 500 (yellow), 1000 (green), and 2000 (blue) Riemann zeta function zeros.Return to TOC
bxtxxtxtxaxxtfdttf nnn
n
iiiin
b
a
1121100
01lim
SOLO
Riemann Integral
http://en.wikipedia.org/wiki/Riemann_integral
ix 1ix
it
itf
ax 0 bxn
ii xx 1
b
a
dttf
In Riemann Integral we divide the interval [a,b]in n non-overlapping intervals, that decrease asn increases. The value f (ti) is computed inside theintervals.
bxtxxtxtxa nnn 1121100
The Riemann Integral is not always defined, for example:
irationalex
rationalexxf
3
2
The Riemann Integral of this function is not defined.
Georg Friedrich BernhardRiemann
1826 - 1866
Integration
Integration
SOLO
Thomas Joannes Stieltjes
1856 - 1894
Riemann–Stieltjes integral
Bernhard Riemann1826 - 1866
The Stieltjes integral is a generalization of Riemann integral. Let f (x) and α (x) be] real-valued functions defined in the closed interval [a,b]. Take a partition of the interval
and consider a Riemann sum
bxxxa n 10
iii
n
iiii xxxxf ,1
11
If the sum tends to a fixed number I when max(xi-xi-1)→0 then I is called aStieltjes integral or a Riemann-Stieltjes integral. The Stieltjes integral of fwith respect to α is denoted:
xdxf
df
If f and α have a common point of discontinuity, then the integral doesn’t exist.However, if f is continuous and α’ is Riemann integrable over the specific interval
or sometimes simply
xd
xddxfxdxf
:''
my
ky
kyE
myE
1M
2M 01 ME
02 ME xfy
SOLO
Lebesgue Integral
Measure
The mean idea of the Lebesgue integral is the notion of Measure.
Definition 1: E (M) є [a,b] is the regionin x є [a,b], of the function f (x) for which Mxf
Definition 2: µ [E (M)] the measure of E (M) is
0 ME
dxME
We can see that µ [E (M)] is the sum of lengths on x axis for which Mxf
From the Figure above we can see that for jumps M1 and M2 021 MEME
Example: Let find the measure of the rationale numbers, ratio of integers, that are countable
n
mrrrrrr k ,,
4
3,
4
1,
3
2,
3
1,
2
15321 3
Since the rationale numbers are discrete we can choose ε > 0 as small as we want and construct an open interval of length ε/2 centered around r1, an interval of ε/22 centered around r2,.., an interval of ε/2k centered around rk
k
rationalsE222 2
00
rationalsE
Integration
xfyyyyxfyyEyydttfbxa
nnibxa
n
i
iiin
b
a
supinflim 110
0
1
a b
0y1y
1ky
1kyky
1ny
ny 1kyE
1kyE kyE
xfy
irationalex
rationalexxf
3
2
SOLO
Lebesgue Integral
Henri Léon Lebesgue1875 - 1941
A function y = f (x) is said to be measurable if the set of points x at which f (x) < c is measurable for any and all choises of the constant c.
The Lebesgue Integral for a measurable function f (x) is defined as:
Example
30131
0
1110/
irationalsErationalsEirationalsExfE
dxxfdxxfdxxfdxxf
3
2
0 1 x
xf
Irationals
Rationals
For a continuous function the Riemann and Lebesgue integrals give the same results.
Integration
IntegrationSOLO
Lebesgue-Stieltjes integration
Thomas Joannes Stieltjes
1856 - 1894
Henri Léon Lebesgue
1875 - 1941
In measure-theoretic analysis and related branches of mathematics, Lebesgue-Stieltjes integration generalizes Riemann-Stieltjes and Lebesgue integration, preserving the many advantages of the latter in a more general measure-theoretic framework.
Let α (x) a monotonic increasing function of x, and define an interval I =(x1,x2).
Define the nonnegative function
12 xxIU The Lebesgue integral with respect to a measure constructed using U (I) is caled Lebesgue-Stieltjes integral, or sometimes Lebesgue-Radon integral.
Johann Karl August Radon
1887 –1956
IntegrationSOLO
Darboux Integral Lower (green) and upper (green plus lavender) Darboux sums for four subintervals
Jean-Gaston Darboux
1842 - 1917 In real analysis, a branch of mathematics, the Darboux integral or Darboux sum is one possible definition of the integral of a function. Darboux integrals are equivalent to Riemann integrals, meaning that a function is Darboux-integrable if and only if it is Riemann-integrable, and the values of the two integrals, if they exist, are equal. Darboux integrals have the advantage of being simpler to define than Riemann integrals. Darboux integrals are named after their discoverer, Gaston Darboux.
A partition of an interval [a,b] is a finite sequence of values xi such that bxxxa n 10
Definition
Each interval [xi−1,xi] is called a subinterval of the partition. Let ƒ:[a,b]→R be a bounded function, and let nxxxP ,,, 10 be a partition of [a,b]. Let
xfmxfM
iiiixxx
ixxx
i,, 11
inf:;sup:
The upper Darboux sum of ƒ with respect to P is
n
iiiiPf MxxU
11, :
The lower Darboux sum of ƒ with respect to P is
n
iiiiPf mxxL
11, :
IntegrationSOLO
Darboux Integral(continue – 1)
Lower (green) and upper (green plus lavender) Darboux sums for four subintervals
Jean-Gaston Darboux
1842 - 1917The upper Darboux sum of ƒ with respect to P is
n
iiiiPf MxxU
11, :
The lower Darboux sum of ƒ with respect to P is
n
iiiiPf mxxL
11, :
The upper Darboux integral of ƒ is baofpartitionaisPUU Pff ,:inf ,
The lower Darboux integral of ƒ is baofpartitionaisPLL Pff ,:inf ,
If Uƒ = Lƒ, then we say that ƒ is Darboux-integrable and set
ff
b
a
LUdttf the common value of the upper and lower Darboux integrals.
IntegrationSOLO
Lebesgue Integration
Henri Léon Lebesgue
1875 - 1941
Illustration of a Riemann integral (blue) and a Lebesgue integral (red)
Riemann Integral A sequence of Riemann sums. The numbers in the upper right are the areas of the grey rectangles. They converge to the integral of the function.
Darboux Integral Lower (green) and upper (green plus lavender) Darboux sums for four subintervals
Jean-Gaston Darboux
1842 - 1917
Bernhard Riemann1826 - 1866
Return to TOC
211
Prime Number Applications
Primes
RSA is an algorithm for public-key cryptography that is based on the presumed difficulty of factoring large integers, the factoring problem. RSA stands for Ron Rivest, Adi Shamir and Leonard Adleman, who first publicly described the algorithm in 1977. Clifford Cocks, an English mathematician, had developed an equivalent system in 1973, but it wasn't declassified until 1997
A user of RSA creates and then publishes the product of two large prime numbers, along with an auxiliary value, as their public key. The prime factors must be kept secret. Anyone can use the public key to encrypt a message, but with currently published methods, if the public key is large enough, only someone with knowledge of the prime factors can feasibly decode the message.[2] Whether breaking RSA encryption is as hard as factoring is an open question known as the RSA problem
Adi Shamir, Ron Rivest andLeonard Adleman
212
Prime Number Applications
Primes
Here is an example of RSA encryption and decryption. The parameters used here are artificially small, but one can also use OpenSSL to generate and examine a real keypair.1.Choose two distinct big (order of 10 308) prime numbers, p and q2. Compute n = p q n is used as the modulus for both the public and private keys. Its length, usually expressed in bits, is the key length 3.Compute φ (n) = (p-1)x(q-1) giving
4. Choose any number 1 < e < φ (n) that is coprime to (not divide) φ (n) e is released as the public key exponent5.Determine d as d-1= e (mod (φ (n)), i.e., d is the multiplicative inverse of e (modulo φ (n)) This is more clearly stated as solve for d given d.e=1 (modulo φ (n)). d is kept as the private key exponent.
The public key consists of the modulus n and the public (or encryption) exponent e. The private key consists of the modulus n and the private (or decryption) exponent d, which must be kept secret. p, q, and φ(n) must also be kept secret because they can be used to calculate d.
213
Prime Number ApplicationsPrimes
Here is an example of RSA encryption and decryption. The parameters used here are artificially small, but one can also use OpenSSL to generate and examine a real keypair.1.Choose two distinct prime numbers, such as
p = 61 and q = 53 (the small prime numbers is for the example only)2.Compute n = p q giving n = 61x53 = 32333.Compute φ (n) = (p-1)x(q-1) giving φ (3233) = (61-1)x(53-1) = 31204.Choose any number 1 < e < 3120 that is coprime to (not divide) 3120 Let e = 175. Compute d, the modular multiplicative inverse of e (mod φ (n)) 17 x d = 1 (mod (3120) d = 2753 ← 17x2753 = 46801 = 3120 x 15 + 1
The public key is n = 3233, e = 17.
For a padded plaintext message m, the encryption function is c (m) = m17 (mod (3233)
The private key is n = 3233, d = 2753. For an encrypted ciphertext c, the decryption function is c2753 (mod (3233)) m (c) = c2753 (mod (3233))Example: m=65, → c (65)=6517 (mod (3233)=2790, m (2790)=27902753 (mod (3233))=65
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214
Riemann's Zeta Function
Primes
215
SOLO Primes
Mathematics Carl Friedrich Gauss taught here in the 19th century. Bernhard Riemann, Johann Peter Gustav Lejeune Dirichlet and a number of significant mathematicians made their contributions to mathematics here. By 1900, David Hilbert and Felix Klein had attracted mathematicians from around the world to Göttingen, which made Göttingen a world mecca of mathematics at the beginning of the 20th century.
University of Göttingen
Carl Friedrich Gauss(1777 – 1855)
Georg Friedrich Bernhard Riemann
)1826– 1866 (
Johann Peter Gustav Lejeune Dirichlet
)1805– 1859 (
David Hilbert)1862 – 1943 (
Christian Felix Klein (1849 – 1925)
216
SOLO
University of Göttingen
In the 1930s, the university became a focal point for the Nazi crackdown on "Jewish physics", as represented by the work of Albert Einstein. In what was later called the "great purge" of 1933, academics including Max Born, Victor Goldschmidt, James Franck, Eugene Wigner, Leó Szilárd, Edward Teller, Emmy Noether, and Richard Courant were expelled or fled. Most of them fled Nazi Germany for places like the United States, Canada, the United Kingdom, and Ireland.
Max Born (1882–1970)Nobel Physics
Victor Moritz Goldschmidt(1888 –1947)Mineralogist
James Franck (1882 –1964)
Nobel Physicist
Eugene Paul "E. P." Wigner
(1902 – 1995)Nobel Physicist
Leó Szilárd (1898 –1964)
Physicist
Edward Teller (1908 –2003)
PhysicistHydrogen Bomb
Amalie Emmy Noether
)1882 – 1935,(Mathematician
Richard Courant (1888 –1972) Mathematician