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Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Zeta Zero-Counting Function
Prof. Fayez A. Alhargan, PhD. BEng.
21 July 2021
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Background
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Introduction
The estimation of the number of zeta zeros was introduced by
Riemann in his landmark paper in 1859, as an approximate
expression. Then in 1905 H. von Mangoldt proved the
approximation. Also, Aleksandar Ivic restated the proof using
contour integration.
In this presentation, a more accurate expression of the zeta
zero-counting function is developed exhibiting the expected step
function behavior and its relation to the primes is demonstrated.
This presentation is based on the paper:
Alhargan, Fayez (2021), A Concise Proof of the Riemann Hypothesis via Hadamard
Product, https://hal.archives-ouvertes.fr/hal-03294415/document.
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Riemann Expression
In the range {0, T}, the number of roots of ξ(s); was conjectured by
Riemann [1], as approximately
= T
2π
ln T
2π
− T
2π
, (1)
and some 46 years later was proved by H. von Mangoldt [2], the prove was
outlined by Ivic ([3], p. 17), where he showed using contour integration, that
the number of zeros is given approximately by
N(T) = T
2π
ln T
2π
− T
2π
+ 7
8
+ 1
π
=
Z
L
ζ0(s)
ζ(s)
ds, (2)
and demonstrated that
=
Z
L
h
ζ0(s)
ζ(s)
i
ds = O(ln T). (3)
Although the integral in Equation (3) is small compared to the major elements
in Equation (2), it still contains the sawtooth-like waveform component, that I
will demonstrate later.
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Now, recalling Riemann [1] main justification of Equation (1), quoted as
follows:
"because the integral
R
d log ξ(t), taken in a positive sense around the
region consisting of the values of t whose imaginary parts lie between 1
2
i
and −1
2
i and whose real parts lie between 0 and T, is (up to a fraction
of the order of magnitude of the quantity 1
T
) equal to (T log T
2π
−
T)i; this integral however is equal to the number of roots of ξ(t) =
0 lying within this region, multiplied by 2πi. One now finds indeed
approximately this number of real roots within these limits, and it is
very probable that all roots are real."
In essence, Riemann instinctively was invoking Cauchy’s argument principle,
for ξ(s) is a meromorphic function inside and on some closed contour D, and
ξ(s) has no zeros or poles on D, thus
1
2πi
I
D
ξ0(s)
ξ(s)
ds = Z − P, (4)
where Z and P denote the number of zeros and poles of ξ(s); inside the
contour D.
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
New Formulation
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Formal Definition
Figure (1) shows that the zero-counting function is a staircase step function.
Thus, we can utilize the Heaviside function, to formally define the
zero-counting function ν(t), as
ν(t) :=
X
m
H(t − tm), (5)
where the sum is over tm, the imaginary values of the ζ(s) zeros.
ν(t)
t
14.13 21.02 25.01 30.42
1
2
3
4
Figure 1: Zeros-Counting Heaviside Step Function.
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Cauchy’s Argument Principle
Now, from the proof of the Riemann Hypothesis [4], which implies that ξ(s)
has simple zeros only on the critical line <(s) = 1
2
, at s = sm and s = s̄m.
Then, we can invoke Cauchy’s argument principle, to define the
zero-counting function ν(t), in the range {s, s̄} enclosed by the contour D, see
Figure (2), for the number of zeros of ξ(s), as
4πiν(t) =
I
D
h
ξ0(s)
ξ(s)
i
ds. (6)
Noting that ξ(s) = 1
2
ζ(s)(s − 1)sΓ( s
2
)π−
s
2 , taking the log and differentiating,
Equation (6) can be expressed in terms of zeta function as
4πiν(t) =
I
D

ζ0(s)
ζ(s)
+
1
(s − 1)
+
1
s
+
Γ0( s
2
)
Γ( s
2
)
−
1
2
ln π

ds, (7)
where the closed contour D encompasses the critical strip [0 ≤ (s) ≤ 1].
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
D L1
L2
σ
t
1
2
sm
s
s̄m
s̄
Figure 2: ζ(s) Critical Strip, Contours D, L1 and L2.
From Figure (2), we see that
• all the poles of [ζ0(s)/ζ(s) + Γ0( s
2
)/Γ( s
2
)] are on the critical line (s) = 1
2
,
• the contour L1 encloses all the sm poles in the range from s̄ to s,
• the contour L2 encloses only the two poles s = 0 and s = 1.
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Thus, we can rearrange Equation (7), as
4πiν(t) =
I
L1

ζ0(s)
ζ(s)
+
Γ0( s
2
)
Γ( s
2
)
−
1
2
ln π

ds +
I
L2
h
1
(s − 1)
+
1
s
i
ds. (8)
Now, the contour integration around L1, can be transformed to a line
integral, as
I
L1
= lim
→0
Z s+
s̄+
+
Z s−
s+
−
Z s̄−
s−
−
Z s̄+
s̄−

= 2
Z s
s̄
(9)
and using the residue theorem for the contour integral around L2, we obtain
I
L2
h
1
(s − 1)
+
1
s
i
ds = 4πi, (10)
thus, Equation (8) becomes
2πiν(t) =
Z s
s̄

ζ0(s)
ζ(s)
+
Γ0( s
2
)
Γ( s
2
)
−
1
2
ln π

ds + 2πi. (11)
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Integrating Equation (11), we have
2πiν(t) =

ln ζ(s) + ln Γ( s
2
) − s
2
ln π
s
s̄
+ 2πi. (12)
Thus, finally we have
2πiν(t) = ln ζ(s) − ln ζ(s̄) + ln Γ( s
2
) − ln Γ( s̄
2
) + ln π− s
2 − ln π− s̄
2 + 2πi,
(13)
with s = 1
2
+ it, we have
2πiν(t) = ln ζ(1
2
+ it) − ln ζ( 1
2
− it)
+ ln Γ( 1
4
+ i t
2
) − ln Γ( 1
4
− i t
2
) − it ln π + 2πi.
(14)
Differentiating Equation (14), we have
2πiν0
(t) =
ζ0( 1
2
+ it)
ζ( 1
2
+ it)
−
ζ0( 1
2
− it)
ζ( 1
2
− it)
+
Γ0( 1
4
+ i t
2
)
Γ( 1
4
+ i t
2
)
−
Γ0( 1
4
− i t
2
)
Γ( 1
4
− i t
2
)
− i ln π.
(15)
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Approximation
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Now, utilizing the first few terms in the Stirling approximation; i.e.
Γ(z) ∼ (z)z
e−z
z− 1
2
√
2π, (16)
and the first few terms in the asymptotic expansion of the digamma function;
i.e.
Γ0(z)
Γ(z)
∼ ln z −
1
2z
. (17)
Therefore, we have
ln Γ( s
2
) − ln Γ( s̄
2
) ∼ s
2
ln s
2
− s̄
2
ln s̄
2
+ 1
2
ln s̄ − 1
2
ln s − it, (18)
and
Γ0( 1
4
+ i t
2
)
Γ( 1
4
+ i t
2
)
−
Γ0( 1
4
− i t
2
)
Γ( 1
4
− i t
2
)
= ln( 1
2
+it)−
1
( 1
2
+ it)
−ln(1
2
−it)+
1
(1
2
− it)
. (19)
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Thus, finally we have
2πiν(t) =( 1
4
+ i t
2
) ln( 1
4
+ i t
2
) − ( 1
4
− i t
2
) ln( 1
4
− i t
2
)
+ 1
2
ln( 1
4
− i t
2
) − 1
2
ln( 1
4
+ i t
2
)
+ ln ζ( 1
2
+ it) − ln ζ( 1
2
− it) − it ln πe = 2πi
X
m
H(t − tm).
(20)
Also, from Equation (15), we have
2πiν0
(t) = ln( 1
2
+ it) −
1
( 1
2
+ it)
− ln( 1
2
− it) +
1
( 1
2
− it)
+
ζ0(1
2
+ it)
ζ( 1
2
+ it)
−
ζ0( 1
2
− it)
ζ(1
2
− it)
− i ln π = 2πi
X
m
δ(t − tm).
(21)
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Equation (20) is a very accurate approximation, and it is a sum of differences
between complex numbers and their conjugates, thus the result will always be
imaginary number as expected.
Further approximation of the log part gives
ν(t) = t
2π
ln t
2eπ
+ 7
8
+ 1
2πi

ln ζ( 1
2
+ it) − ln ζ( 1
2
− it)

. (22)
We note from Alhargan [4], that
ln ζ(s) =
X
k∈N
X
p
1
k
e−ks ln p
= s
X
k∈N
Π(ks), (23)
where Π(s) is the s-domain prime-counting function, given by the Laplace
transform of the x-domain prime-counting function π(x), as
Π(s) = L {π(x)} =
X
p
L {H(ln x − ln p)} =
X
p
e−s ln p
s
. (24)
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Now, from equation (23), we have
ln ζ(s) − ln ζ(s̄) =
X
k
1
k
sΠ(ks) − 1
k
s̄Π(ks̄); (25)
i.e.
ln ζ( 1
2
+ it) − ln ζ( 1
2
− it) = 2i
X
p
X
k
1
k
p− k
2 sin(tk ln p), (26)
giving
ν(t) = t
2π
ln t
2eπ
+ 7
8
+ 1
π
X
p
X
k
1
k
p− k
2 sin(tk ln p). (27)
We observe from Equation (25), the direct relation between the
zero-counting function ν(t) and the s-domain prime-counting function Π(s).
Furthermore, we observe in Equation (27), the direct relationship between
the zeta zero-counting function ν(t), and the sum of the prime harmonics.
Although the equation is slow for computational purposes, it reveals the
underlying relationship between the zero-counting function and the primes.
Moreover, it exposes the source of the sawtooth-like waveform effect as the
spectrum sum of the prime harmonics.
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Computation
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
The sawtooth-like waveform component [ln ζ( 1
2
+ it) − ln ζ( 1
2
− it)] of ν(t)
is shown in Figure (3). It is observed that the component magnitude is less
than one.
However, it has a vital contribution to the accuracy of the zero-counting
function; which turns it into a Heaviside staircase step function, as shown in
Figure (4), this vital component has been overlooked in the literature.
Figure 3: The sawtooth-like waveform component of ν(t).
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Finally, Figure (4) shows comparisons between ν(t) and N(t), and it confirms
that the zero counting function is a Heaviside staircase step function, and its
differential ν0(t) is an impulse Dirac delta function; as can be seen in Figure (5).
Figure 4: ν(t) vs. N(t).
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Figure 5: |ν0
(t)| .
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
References
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
References
Riemann, Bernhard (1859). Über die Anzahl der Primzahlen unter einer
gegebenen Grösse. Monatsberichte der Berliner Akademie.. In
Gesammelte Werke, Teubner, Leipzig (1892), Reprinted by Dover, New
York (1953).
Mangoldt, H. von (1905), Zur Verteilung der Nullstellen der
Riemannschen Funktion ξ(t). Mathematische Annalen 1905, Vol. 60, pp.
1-19, https://gdz.sub.uni-goettingen.de/id/PPN235181684_0060
Ivic, A. (1985). The Riemann Zeta Function, John Wiley  Sons.
Alhargan, Fayez (2021), A Concise Proof of the Riemann Hypothesis via
Hadamard Product,
https://hal.archives-ouvertes.fr/hal-03294415/document.
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
Summary
Zeta Zero-Counting
Function
Fayez A. Alhargan
Background
New Formulation
Approximation
Computation
References
Summary
Background New Formulation Approximation Computation References Summary
The Zero-Counting Function Proof on One Slide
The zero-counting function ν(t) of the number of zeros of ξ(s), in the range {s, s̄}
enclosed by the contour D, is defined as
4πiν(t) =
I
D
h
ξ0
(s)
ξ(s)
i
ds =
I
D
h
ζ0
(s)
ζ(s)
+
1
(s − 1)
+
1
s
+
Γ0
( s
2 )
Γ( s
2 )
−
1
2
ln π
i
ds.
(28)
where the closed contour D encompasses the critical strip [0 ≤ (s) ≤ 1]. Thus,
4πiν(t) =
I
L1
h
ζ0
(s)
ζ(s)
+
Γ0
( s
2 )
Γ( s
2 )
−
1
2
ln π
i
ds +
I
L2
h
1
(s − 1)
+
1
s
i
ds. (29)
Integrating, using line integral for L1 and residue theorem for L2, we have
2πiν(t) = ln ζ(s) − ln ζ(s̄) + ln Γ( s
2 ) − ln Γ( s̄
2 ) + ln π
− s
2 − ln π
− s̄
2 + 2πi. (30)
Utilizing Stirling approximation, we have
2πiν(t) =( 1
4 + i t
2 ) ln( 1
4 + i t
2 ) − ( 1
4 − i t
2 ) ln( 1
4 − i t
2 )
+ 1
2 ln( 1
4 − i t
2 ) − 1
2 ln( 1
4 + i t
2 )
+ ln ζ( 1
2 + it) − ln ζ( 1
2 − it) − it ln πe = 2πi
X
m
H(t − tm).
(31)
Q.E.D.  
Fayez A. Alhargan

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Zeta Zero-Counting Function

  • 1. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Zeta Zero-Counting Function Prof. Fayez A. Alhargan, PhD. BEng. 21 July 2021
  • 2. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Background
  • 3. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Introduction The estimation of the number of zeta zeros was introduced by Riemann in his landmark paper in 1859, as an approximate expression. Then in 1905 H. von Mangoldt proved the approximation. Also, Aleksandar Ivic restated the proof using contour integration. In this presentation, a more accurate expression of the zeta zero-counting function is developed exhibiting the expected step function behavior and its relation to the primes is demonstrated. This presentation is based on the paper: Alhargan, Fayez (2021), A Concise Proof of the Riemann Hypothesis via Hadamard Product, https://hal.archives-ouvertes.fr/hal-03294415/document.
  • 4. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Riemann Expression In the range {0, T}, the number of roots of ξ(s); was conjectured by Riemann [1], as approximately = T 2π ln T 2π − T 2π , (1) and some 46 years later was proved by H. von Mangoldt [2], the prove was outlined by Ivic ([3], p. 17), where he showed using contour integration, that the number of zeros is given approximately by N(T) = T 2π ln T 2π − T 2π + 7 8 + 1 π = Z L ζ0(s) ζ(s) ds, (2) and demonstrated that = Z L h ζ0(s) ζ(s) i ds = O(ln T). (3) Although the integral in Equation (3) is small compared to the major elements in Equation (2), it still contains the sawtooth-like waveform component, that I will demonstrate later.
  • 5. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Now, recalling Riemann [1] main justification of Equation (1), quoted as follows: "because the integral R d log ξ(t), taken in a positive sense around the region consisting of the values of t whose imaginary parts lie between 1 2 i and −1 2 i and whose real parts lie between 0 and T, is (up to a fraction of the order of magnitude of the quantity 1 T ) equal to (T log T 2π − T)i; this integral however is equal to the number of roots of ξ(t) = 0 lying within this region, multiplied by 2πi. One now finds indeed approximately this number of real roots within these limits, and it is very probable that all roots are real." In essence, Riemann instinctively was invoking Cauchy’s argument principle, for ξ(s) is a meromorphic function inside and on some closed contour D, and ξ(s) has no zeros or poles on D, thus 1 2πi I D ξ0(s) ξ(s) ds = Z − P, (4) where Z and P denote the number of zeros and poles of ξ(s); inside the contour D.
  • 6. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary New Formulation
  • 7. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Formal Definition Figure (1) shows that the zero-counting function is a staircase step function. Thus, we can utilize the Heaviside function, to formally define the zero-counting function ν(t), as ν(t) := X m H(t − tm), (5) where the sum is over tm, the imaginary values of the ζ(s) zeros. ν(t) t 14.13 21.02 25.01 30.42 1 2 3 4 Figure 1: Zeros-Counting Heaviside Step Function.
  • 8. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Cauchy’s Argument Principle Now, from the proof of the Riemann Hypothesis [4], which implies that ξ(s) has simple zeros only on the critical line <(s) = 1 2 , at s = sm and s = s̄m. Then, we can invoke Cauchy’s argument principle, to define the zero-counting function ν(t), in the range {s, s̄} enclosed by the contour D, see Figure (2), for the number of zeros of ξ(s), as 4πiν(t) = I D h ξ0(s) ξ(s) i ds. (6) Noting that ξ(s) = 1 2 ζ(s)(s − 1)sΓ( s 2 )π− s 2 , taking the log and differentiating, Equation (6) can be expressed in terms of zeta function as 4πiν(t) = I D ζ0(s) ζ(s) + 1 (s − 1) + 1 s + Γ0( s 2 ) Γ( s 2 ) − 1 2 ln π ds, (7) where the closed contour D encompasses the critical strip [0 ≤ (s) ≤ 1].
  • 9. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary D L1 L2 σ t 1 2 sm s s̄m s̄ Figure 2: ζ(s) Critical Strip, Contours D, L1 and L2. From Figure (2), we see that • all the poles of [ζ0(s)/ζ(s) + Γ0( s 2 )/Γ( s 2 )] are on the critical line (s) = 1 2 , • the contour L1 encloses all the sm poles in the range from s̄ to s, • the contour L2 encloses only the two poles s = 0 and s = 1.
  • 10. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Thus, we can rearrange Equation (7), as 4πiν(t) = I L1 ζ0(s) ζ(s) + Γ0( s 2 ) Γ( s 2 ) − 1 2 ln π ds + I L2 h 1 (s − 1) + 1 s i ds. (8) Now, the contour integration around L1, can be transformed to a line integral, as I L1 = lim →0 Z s+ s̄+ + Z s− s+ − Z s̄− s− − Z s̄+ s̄− = 2 Z s s̄ (9) and using the residue theorem for the contour integral around L2, we obtain I L2 h 1 (s − 1) + 1 s i ds = 4πi, (10) thus, Equation (8) becomes 2πiν(t) = Z s s̄ ζ0(s) ζ(s) + Γ0( s 2 ) Γ( s 2 ) − 1 2 ln π ds + 2πi. (11)
  • 11. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Integrating Equation (11), we have 2πiν(t) = ln ζ(s) + ln Γ( s 2 ) − s 2 ln π s s̄ + 2πi. (12) Thus, finally we have 2πiν(t) = ln ζ(s) − ln ζ(s̄) + ln Γ( s 2 ) − ln Γ( s̄ 2 ) + ln π− s 2 − ln π− s̄ 2 + 2πi, (13) with s = 1 2 + it, we have 2πiν(t) = ln ζ(1 2 + it) − ln ζ( 1 2 − it) + ln Γ( 1 4 + i t 2 ) − ln Γ( 1 4 − i t 2 ) − it ln π + 2πi. (14) Differentiating Equation (14), we have 2πiν0 (t) = ζ0( 1 2 + it) ζ( 1 2 + it) − ζ0( 1 2 − it) ζ( 1 2 − it) + Γ0( 1 4 + i t 2 ) Γ( 1 4 + i t 2 ) − Γ0( 1 4 − i t 2 ) Γ( 1 4 − i t 2 ) − i ln π. (15)
  • 12. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Approximation
  • 13. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Now, utilizing the first few terms in the Stirling approximation; i.e. Γ(z) ∼ (z)z e−z z− 1 2 √ 2π, (16) and the first few terms in the asymptotic expansion of the digamma function; i.e. Γ0(z) Γ(z) ∼ ln z − 1 2z . (17) Therefore, we have ln Γ( s 2 ) − ln Γ( s̄ 2 ) ∼ s 2 ln s 2 − s̄ 2 ln s̄ 2 + 1 2 ln s̄ − 1 2 ln s − it, (18) and Γ0( 1 4 + i t 2 ) Γ( 1 4 + i t 2 ) − Γ0( 1 4 − i t 2 ) Γ( 1 4 − i t 2 ) = ln( 1 2 +it)− 1 ( 1 2 + it) −ln(1 2 −it)+ 1 (1 2 − it) . (19)
  • 14. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Thus, finally we have 2πiν(t) =( 1 4 + i t 2 ) ln( 1 4 + i t 2 ) − ( 1 4 − i t 2 ) ln( 1 4 − i t 2 ) + 1 2 ln( 1 4 − i t 2 ) − 1 2 ln( 1 4 + i t 2 ) + ln ζ( 1 2 + it) − ln ζ( 1 2 − it) − it ln πe = 2πi X m H(t − tm). (20) Also, from Equation (15), we have 2πiν0 (t) = ln( 1 2 + it) − 1 ( 1 2 + it) − ln( 1 2 − it) + 1 ( 1 2 − it) + ζ0(1 2 + it) ζ( 1 2 + it) − ζ0( 1 2 − it) ζ(1 2 − it) − i ln π = 2πi X m δ(t − tm). (21)
  • 15. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Equation (20) is a very accurate approximation, and it is a sum of differences between complex numbers and their conjugates, thus the result will always be imaginary number as expected. Further approximation of the log part gives ν(t) = t 2π ln t 2eπ + 7 8 + 1 2πi ln ζ( 1 2 + it) − ln ζ( 1 2 − it) . (22) We note from Alhargan [4], that ln ζ(s) = X k∈N X p 1 k e−ks ln p = s X k∈N Π(ks), (23) where Π(s) is the s-domain prime-counting function, given by the Laplace transform of the x-domain prime-counting function π(x), as Π(s) = L {π(x)} = X p L {H(ln x − ln p)} = X p e−s ln p s . (24)
  • 16. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Now, from equation (23), we have ln ζ(s) − ln ζ(s̄) = X k 1 k sΠ(ks) − 1 k s̄Π(ks̄); (25) i.e. ln ζ( 1 2 + it) − ln ζ( 1 2 − it) = 2i X p X k 1 k p− k 2 sin(tk ln p), (26) giving ν(t) = t 2π ln t 2eπ + 7 8 + 1 π X p X k 1 k p− k 2 sin(tk ln p). (27) We observe from Equation (25), the direct relation between the zero-counting function ν(t) and the s-domain prime-counting function Π(s). Furthermore, we observe in Equation (27), the direct relationship between the zeta zero-counting function ν(t), and the sum of the prime harmonics. Although the equation is slow for computational purposes, it reveals the underlying relationship between the zero-counting function and the primes. Moreover, it exposes the source of the sawtooth-like waveform effect as the spectrum sum of the prime harmonics.
  • 17. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Computation
  • 18. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary The sawtooth-like waveform component [ln ζ( 1 2 + it) − ln ζ( 1 2 − it)] of ν(t) is shown in Figure (3). It is observed that the component magnitude is less than one. However, it has a vital contribution to the accuracy of the zero-counting function; which turns it into a Heaviside staircase step function, as shown in Figure (4), this vital component has been overlooked in the literature. Figure 3: The sawtooth-like waveform component of ν(t).
  • 19. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Finally, Figure (4) shows comparisons between ν(t) and N(t), and it confirms that the zero counting function is a Heaviside staircase step function, and its differential ν0(t) is an impulse Dirac delta function; as can be seen in Figure (5). Figure 4: ν(t) vs. N(t).
  • 20. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Figure 5: |ν0 (t)| .
  • 21. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary References
  • 22. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary References Riemann, Bernhard (1859). Über die Anzahl der Primzahlen unter einer gegebenen Grösse. Monatsberichte der Berliner Akademie.. In Gesammelte Werke, Teubner, Leipzig (1892), Reprinted by Dover, New York (1953). Mangoldt, H. von (1905), Zur Verteilung der Nullstellen der Riemannschen Funktion ξ(t). Mathematische Annalen 1905, Vol. 60, pp. 1-19, https://gdz.sub.uni-goettingen.de/id/PPN235181684_0060 Ivic, A. (1985). The Riemann Zeta Function, John Wiley Sons. Alhargan, Fayez (2021), A Concise Proof of the Riemann Hypothesis via Hadamard Product, https://hal.archives-ouvertes.fr/hal-03294415/document.
  • 23. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary Summary
  • 24. Zeta Zero-Counting Function Fayez A. Alhargan Background New Formulation Approximation Computation References Summary Background New Formulation Approximation Computation References Summary The Zero-Counting Function Proof on One Slide The zero-counting function ν(t) of the number of zeros of ξ(s), in the range {s, s̄} enclosed by the contour D, is defined as 4πiν(t) = I D h ξ0 (s) ξ(s) i ds = I D h ζ0 (s) ζ(s) + 1 (s − 1) + 1 s + Γ0 ( s 2 ) Γ( s 2 ) − 1 2 ln π i ds. (28) where the closed contour D encompasses the critical strip [0 ≤ (s) ≤ 1]. Thus, 4πiν(t) = I L1 h ζ0 (s) ζ(s) + Γ0 ( s 2 ) Γ( s 2 ) − 1 2 ln π i ds + I L2 h 1 (s − 1) + 1 s i ds. (29) Integrating, using line integral for L1 and residue theorem for L2, we have 2πiν(t) = ln ζ(s) − ln ζ(s̄) + ln Γ( s 2 ) − ln Γ( s̄ 2 ) + ln π − s 2 − ln π − s̄ 2 + 2πi. (30) Utilizing Stirling approximation, we have 2πiν(t) =( 1 4 + i t 2 ) ln( 1 4 + i t 2 ) − ( 1 4 − i t 2 ) ln( 1 4 − i t 2 ) + 1 2 ln( 1 4 − i t 2 ) − 1 2 ln( 1 4 + i t 2 ) + ln ζ( 1 2 + it) − ln ζ( 1 2 − it) − it ln πe = 2πi X m H(t − tm). (31) Q.E.D. Fayez A. Alhargan