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Suggested Solution of HW4

1) The document provides solutions to homework problems from Chapter 6 involving gamma functions and their properties. 2) Key steps are shown to derive Wallis' product formula for pi using limits of factorials and the Gauss formula for the gamma function. 3) The derivatives of the function f(z) = 1/(1-z)^α are computed inductively to relate them to the gamma function. 4) An contour integral argument is used to relate the integrals of e^-t t^s-1 from 0 to infinity over real and imaginary axes, relating them to the gamma function.

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Rodrigo Kosta
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0% found this document useful (0 votes)
143 views8 pages

Suggested Solution of HW4

1) The document provides solutions to homework problems from Chapter 6 involving gamma functions and their properties. 2) Key steps are shown to derive Wallis' product formula for pi using limits of factorials and the Gauss formula for the gamma function. 3) The derivatives of the function f(z) = 1/(1-z)^α are computed inductively to relate them to the gamma function. 4) An contour integral argument is used to relate the integrals of e^-t t^s-1 from 0 to infinity over real and imaginary axes, relating them to the gamma function.

Uploaded by

Rodrigo Kosta
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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Suggested solution of HW4

Chapter 6 Q1: By the product formula of Γ, we have for all z,



1 sin πz Y z
= Γ(1 − z) = eγz z (1 + )e−z/n
Γ(z) π n=1
n

where γ is the Euler’s constant.


N
Y z −z/n (z + 1)(z + 2) · ·(z + N ) −z(PN 1
eγz z(1 + )e = eγz z e n=1 n −log N ) · e−z log N
n=1
n N!

z(z + 1) · ·(z + n)
→ lim ,
n→∞ nz n!

whenever z 6= 0, −1, −2, ....

Chapter 6 Q3: Recall Walliss product formula stating that


∞  
π Y 2n 2n
= ·
2 n=1
2n − 1 2n + 1

2·2 4·4 2m · 2m
= lim · ...
m→∞ 1 · 3 3 · 5 (2m − 1)(2m + 1)
24 · 44 ...(2m)4
= lim · (2m + 1)
m→∞ 12 · 22 · 32 · ...(2m + 1)2

(m!)4 24m
= lim (2m + 1).
m→∞ [(2m + 1)!]2

Recall the Gauss formula,

ns n!
Γ(s) = lim .
n→∞ s(s + 1)...(s + n)

Direct substitution yields the following



n2s+1/2 (n!)2 4n+1 (n!)2 n2s n
=
s(s + 1/2)(s + 1)...(s + n)(s + 1/2 + n) (2s)(2s + 1)...(2s + 2n + 1)
 n√
(2n + 1)2s (2n + 1)! 4 2n + 1(n!)2 4n2s+1/2

= · ·
(2s)...(2s + 2n + 1) (2n + 1)! (2n + 1)2s+1/2
π 3/2−2s √ 1−2s
r
→ Γ(2s) · ·2 = π2 Γ(2s).
2

Chapter 6 Q4: For f (z) = 1/(1 − z)α = exp [−α log(1 − z)], we have

(1 − z)f 0 (z) = exp [−α log(1 − z)] = αf (z)

(1 − z)f 00 (z) = (α + 1)f 0 (z)

Inductively, we have

(1 − z)f (n) (z) = (α + n − 1)f (n−1) (z) = (α + n − 1) · (α + n − 2) · ·(α + 1)f (z).

1
Put z = 0, we have

f (n) (0) = (α + n − 1)f (n−1) (z) = (α + n − 1) · (α + n − 2) · ·(α + 1).

Since an (α) = f (n) (0)/n! , we have


an (α) (α + n − 1) · (α + n − 2) · ·(α + 1)
α−1
= → Γ(α).
n nα−1
R∞ R∞
Chapter 6 Q10: (a) Our goal is to comparer the integral 0 e−t ts−1 dt with 0 e−it ts−1 dt. So
we consider the meromorphic function f (w) = e−w wz−1 for a fixed z ∈ C on
{z : Re(z) ≥ 0}.
Consider the contour suggested in textbook and denote it by γ = γ1 ∪ γ2 ∪ γ3 ∪ γ4
where γ1 is on the real axis, γ2 is the large circular arc, γ3 is on the imaginary
axis and γ4 is the smaller γ4 . As it is holomorphic, by cauchy theorem,
I I I I I
0= f (w) dw = + + + f (w) dw.
γ γ1 γ2 γ3 γ4

We compute them separately.


I Z R
f (w) dw = e−t tz−1 dt,
γ1 
I Z π/2

f (w) dw = e−Re (eiθ )z−1 Rz dθ.
γ2 0
I Z R Z R
f (w) dw = − e−it (it)z−1 i dt = −iz e−it tz−1 dt,
γ3  
I Z π/2

f (w) dw = − e−e (eiθ )z−1 z dθ.
γ4 0

Letting  → 0, we see that the fourth term goes to 0 if Re(z) > 0. Let R → ∞,
we see that the second term goes to 0 as illustrated below.
Z
π/2 Z π/2
−Reiθ iθ z−1 z
e (e ) R dθ ≤ RRe(z) · e−R cos θ dθ.


0 0

Let t = cos θ, we have


π/2 1
e−Rt
Z Z
e−R cos θ dθ = √ dt → 0.
0 0 1 − t2
R1 R 1/2
The convergence can be seen by splitting it into two parts, 1/2
, 0
, or simply
using Lebesgue’s monotone convergence theorem. Thus, if Re(z) ∈ (0, 1), we
have Z
π/2
−Reiθ iθ z−1 z
e (e ) R dθ → 0


0

as R → ∞. So we yield the following result.


Z ∞ Z ∞
e−it tz−1 dt = i−z e−t tz−1 dt = e−iπz/2 Γ(z).
0 0

Part (a) follows from taking real part and imaginary part of this expression.

2
(b) For t ∈ (0, 1), we have sin t ≤ t. So, whenever Re(z) ∈ (−1, 1),
Z 1
sin t
Z 1
dt ≤ 1
dt < ∞.
0
t1−z
0 t−Re(z)

On the other hand,


Z ∞ Z ∞
sin t
dt = − cos 1 + (z − 1) cos (t)tz−2 dt.
1 t1−z 1

Thus, M (sin)(z) define a analytic function on −1 < Re(z) < 1 . By analytic


continuation, the second equality holds on the large strip. Put z = 0 and z =
−1/2 to obtain the conclusion.

Chapter 6,Q14: (a) First part follows from the Fundamental theorem of calculus. And the second
part follows from integrating log x.
(b) By (a), and monotonicity of Γ(x), for large n, we have
Z n+1
log n + log Γ(n) = log Γ(n + 1) ≥ log Γ(t) dt = n log n − n + c ≥ log Γ(n).
n

So, we have the following inequality,

n log n − n + c ≥ log Γ(n) ≥ (n − 1) log n − n + c

1 c log Γ(n) n−1 1 c


1− + ≥ ≥ − + .
log n n log n n log n n log n n log n

Take n → ∞ to obtain the asymptotic behaviour. Indeed, one can observe


log Γ(n) ∼ n log n + O(n) from the first inequality.

chapter 6, Q15:
Z ∞ Z ∞
Γ(s) = e−t ts−1 dt = ns e−nt ts−1 dt;
0 0

That is
Z ∞
n−s Γ(s) = e−nt ts−1 dt.
0

Summing over all n yield


∞ Z
X ∞
ζ(s)Γ(s) = e−nt ts−1 dt
n=1 0

Z ∞ ∞
X
= ts−1 e−nt dt
0 n=1

ts−1
Z
= dt.
0 et − 1

Chapter 6,Q16: You may follow the step suggested in the tutorial class on 3/11 by proving the Rie-
mann’s Functional Equation. Or use the hints suggested in the textbook as stated in

3
the following.

By Q15, we can write


∞ 1 ∞
ts−1 ts−1 ts−1
Z Z Z
Γ(s)ζ(s) = dt = dt + dt
0 et − 1 0 et − 1 1 et − 1
As the function in the second integral is of exponential decay, it defines a entire
function. Now we take a look on the first integral. By expanding the power series of
z/(ez − 1) at z = 0, we have

1 X Bm m−1
= z
ez − 1 m=0 m!

where
Bm 1/m

1
lim sup
= . (1)
m→∞ m! 2π

by Cauchy Hadamard theorem and the fact that radius of convergence of z/(ez − 1)
is 2π. Using this, we are able to represent the first integral in the following form.
1 ∞
ts−1
Z X Bm
t
dt = .
0 e −1 m=0
m!(s + m − 1)

By the control of (1), the series converges uniformly on any compact set away from
{1, 0, −1, ...}. It gives a meromorphic function on C with simple pole at {1, 0, −1, ...}.
But since 1/Γ(s) is a entire funtion with simple zero at {0, −1, −2, ...}. So
Z 1 s−1
1 t
dt
Γ(s) 0 et − 1
define a meromorphic function with a simple pole at s = 1.

Chapter 7,Q1: By summation by part formula, we can reformulate the Dirichlet series in the following
way,
N N −1  
X an AN X 1 1
= s − An − s .
n=1
ns N n=1
(n + 1)s n

Noted that in general, the mean value theorem does not hold for holomorphic function.
So we argue in the following way.

For a fixed s ∈ C, define a holomorphic function f (z) = z −s on the right half plane.
Consider the straight line γ from n + 1 to n.

1 1

(n + 1)s − = |f (n + 1) − f (n)|
ns
Z n+1
f 0 (t) dt

=
n
Z n+1
≤ |f 0 (t)| dt ≤ sup{|f 0 (t)| : t ∈ [n, n + 1]}.
n

4
Within [n, n + 1], for Re(s) > 0,

|s| |s| |s|


|f 0 (x)| = ≤ Re(s)+1 ≤ Re(s)+1
|xs+1 | x n

Combine this to the series, we obtain

N −1 N −1
X 1 1 X M |s|
|An |
− s ≤ .
n=1
(n + 1)s n n=1
nRe(s)+1


X an
The series is absolutely convergent. So converge. And the convergence is
n=1
ns
uniform on any compact set due to the above estimate.
P P
Chapter 7,Q2: (a) We claim that for two absolutely convergent series an , bn ,


X ∞
X ∞ X
X
ak · bm = ak bm .
k=1 m=1 n=1 mk=n

Let  > 0, there exists N such that,



X ∞
X
|ak | + |bm | < .
k=N m=N

On the other hand,



N2 X N2 N2
N N
X X X X X X X


ak · bm − ak bm ≤
|ak bm | + |ak bm | .
k=1 m=1 n=1 mk=n n=N +1 mk=n;m>N n=N +1 mk=n;k>N

Due to the symmetry, it suffices to estimate one of terms in the right hand side.
2 2
N
X X N
X N
X
|ak bm | ≤ |ak | · |bm |
n=N +1 mk=n;k>N k=N +1 m=1

∞ ∞ ∞
!
X X X
≤ |ak | · |bm | <  |bm | .
k=N m=1 m=1

∞ ∞
X 1 X 1 X 1
(b) Since (ζ(s))2 = s
· s
= .
k m=1 m (mk)s
k=1 k,m

For each n ∈ N, the number of divisors is equal to the number of ways of repre-
senting n by mk. Thus,

X 1 X d(n)
= .
(mk)s n=1
ns
k,m

Similarly,
X ma
ζ(s)ζ(s − a) =
(mk)s
k,m

5
For a given n ∈ N, we sum over all ma where m is a divisor of n. Thus


X σa (n)
ζ(s)ζ(s − a) = .
n=1
ns

Chapter 7-Q3: (a) By Euler’s identity,



1 Y 1 X an
= (1 − s ) = .
ζ(s) p
p n=1
ns

If n = 1, a1 = 1 clearly. If n = p1 p2 · ·pk , where pj are all distinct prime. Then


an = (−1)k . Result follows from unique factorization of integer.
1
(b) Since 1 = ζ(s) · ζ(s) ,

∞ ∞ ∞
X 1 X µ(k) X an
1= · =
m=1
ms ks n=1
ns
k=1

P P
where an = mk=n µ(k) = k|n µ(k). By comparing coefficient, we show the
claim.

Chapter 7-Q5: (a) This is a special case of Q1 in Ch7.


(b)
∞ ∞
X 1 1 X 1
ζ(s) − ζ̃(s) = s
= s s
= 2−s ζ(s).
n=1
(2n) 2 n=1
n

Rearrange it to obtain the desired equation.


(c) For s ∈ (0, 1), since
1 1
− >0
(2k − 1)s (2k)s

for all k ∈ N, we have ζ̃(s) > 0. By analytic continuation, equation in part (b)
holds on the whole complex plane. So, ζ(s) has no zero on (0, 1).
According to the functional equation,

Γ((1 − s)/2)
ζ(s) = π s−1/2 ζ(1 − s) .
Γ(s/2)

At s = 0, the simple pole at s = 0 for ζ(1 − s) is cancelled out with the simple
zero of Γ(s/2). Thus, ζ has no zero at s = 0.

Chapter 7-Q6: If a = 1,
Z c+iN  
1 c + iN
ds = log → log(−1) = iπ.
c−iN s c − iN

If a ∈ [0, 1), Since as /s has no pole on the right half plane of the vertical strip,

as
I
1
ds = 0,
2πi γ s

6
where γ is the curve composed of the vertical strip from c − iN to c + iN and a semi-
circle γ 0 from c + iN to c − iN in clockwise direction.
Thus,
c+iN
as as
Z Z
1 1
lim ds = lim ds.
N →∞ 2πi c−iN s N →∞ 2πi −γ 0 s

But
Z π/2 c+N cos t
as
Z
|a |
ds ≤ it |
· N dt

−γ 0 s −π/2 |c + N e
Z π/2 c+N cos t
|a |
≤ · N dt
−π/2 N −c
Z π/2
c
≤ 4a aN cos t dt,
0

for all large N . Via change of coordinate cos t = x, we get


Z 1 Z 1
Nx 1 aN x
a dx = √ dx → 0 as N → ∞.
0 sin t 0 1 − x2
R1 R 1/2
You can show this by splitting the integral into 1/2
and 0
. And followed by direct
integration. Or use dominated convergence theorem. Combine everything to conclude
the case of a ∈ [0, 1).

If a > 1, consider the contour γ composed of the vertical strip from c − iN to c + iN ,


the horizontal strip from c + iN to y-axis, the semi-circle from iN to −iN oriented
in the anticlockwise direction, and then the horizontal strip from −iN to the vertical
strip c + it, t ∈ R. Denote the contour γ by γ1 + γ2 + γ3 + γ4 respectively.

For γ3 , we have
π/2 π/2
as aN cos t
Z Z Z
| ds| ≤ N dt = aN cos t dt.
γ3 s 3π/2 |N eit | 3π/2

Argue similar to above, we have when N → ∞


Z π/2
aN cos t dt → 0.
3π/2

Similarly, the integral over γ2 , γ4 also tends to 0, as N → ∞. By residue theorem, the


integral over γ is 1 which yield our result.

Chapter 7-Q8: (a)

F (−s) = ξ(1/2 − s) = ξ(1 − 1/2 + s) = ξ(1/2 + s) = F (s).

The second equality follows from functional equation of ξ. By expanding its


P∞ n
power series, F (s) = n=0 an s . We conclude that an = 0 if n is odd. So
P∞
G = n=0 a2n sn .

7
(b) The only pole of ζ is at s = 1, so it remains to show the order of growth of
(s − 1)ζ(s). Make use of the following functional equation, for Re(s) < 0,

Γ((1 − s)/2)
ζ(s) = π s−1/2 ζ(1 − s) .
Γ(s/2)
1
Noted that , π s is of order 1.
Γ(s)
Z ∞ Z ∞
−t (−s−1)/2
|Γ((1 − s)/2)| ≤ e |t | dt ≤ e−t t(−Re(s)−1)/2 dt
0 0

≤ Γ((1 − Re(s))/2)

≤ (−Re(s))!

By Stirling formula, it is of order 1. So it suffices to consider Re(s) ≥ 0. But it


has already been done in Proposition 2.7 of ch6.

It remains to show the lower bound. Substitute s = −2n − 1, we have


Γ(n + 1)
|ζ(−2n − 1)| = π −2n−3/2 ζ(2 + 2n)
Γ(−n − 1/2)

n! X 1
= π −2n−3/2 .
Γ(−n − 1/2) k 2+2n
k=1

On the other hand,



π
|Γ(−n − 1/2)| =
(n + 1/2)(n + 1/2 − 1) · · · (3/2)(1/2)

2n π
=
(2n + 1)(2n − 1) · · · (3)(1)

22n n! π
= ·
(2n)!
Also, by comparing to the integral , we have

X 1 1
≈ .
k 2+2n 1 + 2n
k=1

Combine all this, we get


(2n)! 1
|ζ(−2n − 1)| ≈ π
(2π)2n 1 + 2n
Taking log yield
log |ζ(−2n − 1)| ≈ log π + log[(2n)!] − 2n log (2π) − log (1 + 2n)

Since log(2n)! ≈ 2n log(2n) + O(n), we conclude that ζ(−2n − 1) is of order 1.


(c) By Q14 in ch5, G has infinitely many zeros. Since

ξ(s + 1/2) F (s)


ζ(s + 1/2) = π 1/4+s/2 = π 1/4+s/2 ,
Γ(s/2 + 1/4) Γ(s/2 + 1/4)

ζ(s) has infinitely many zeros.

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