5 Entire Functions
3.2 Example: the product formula for the sine function
Before proceeding with the general theory of Weierstrass products, we consider the key example of the product formula for the sine function:
(3) sin πz
This identity will in turn be derived from the sum formula for the cotan-gent function (cot πz = cos πz/ sin πz): The first formula holds for all complex numbers z, and the second when-ever z is not an integer. The sum∞
n=−∞1/(z + n) needs to be properly understood, because the separate halves corresponding to positive and negative values of n do not converge. Only when interpreted symmetri-cally, as limN→∞
|n|≤N1/(z + n), does the cancellation of terms lead to a convergent series as in (4) above.
3. Infinite products 143 We prove (4) by showing that both π cot πz and the series have the same structural properties. In fact, observe that if F (z) = π cot πz, then F has the following three properties:
(i) F (z + 1) = F (z) whenever z is not an integer.
(ii) F (z) = 1
z + F0(z), where F0 is analytic near 0.
(iii) F (z) has simple poles at the integers, and no other singularities.
Then, we note that the function
∞
also satisfies these same three properties. In fact, property (i) is simply the observation that the passage from z to z + 1 merely shifts the terms in the infinite sum. To be precise,
Letting N tend to infinity proves the assertion. Properties (ii) and (iii) are evident from the representation z1+∞
n=1 2z
z2−n2 of the sum.
Therefore, the function defined by
∆(z) = F (z)−
∞ n=−∞
1 z + n
is periodic in the sense that ∆(z + 1) = ∆(z), and by (ii) the singularity of ∆ at the origin is removable, and hence by periodicity the singularities at all the integers are also removable; this implies that ∆ is entire.
To prove our formula, it will suffice to show that the function ∆ is bounded in the complex plane. By the periodicity above, it is enough to do so in the strip |Re(z)| ≤ 1/2. This is because every z∈ C is of the form z= z + k, where z is in the strip and k is an integer. Since ∆ is holomorphic, it is bounded in the rectangle|Im(z)| ≤ 1, and we need only control the behavior of that function for |Im(z)| > 1. If Im(z) > 1 and z = x + iy, then
cot πz = i eiπz+ e−iπz
eiπz− e−iπz = i e−2πy+ e−2πix e−2πy− e−2πix,
144 Chapter 5. ENTIRE FUNCTIONS
and in absolute value this quantity is bounded. Also 1 therefore if y > 1, we have
Now the sum on the right-hand side is majorized by
∞
0
y y2+ x2 dx ,
because the function y/(y2+ x2) is decreasing in x; moreover, as the change of variables x → yx shows, the integral is independent of y, and hence bounded. By a similar argument ∆ is bounded in the strip where Im(z) <−1, hence is bounded throughout the whole strip |Re(z)| ≤ 1/2.
Therefore ∆ is bounded in C, and by Liouville’s theorem, ∆(z) is con-stant. The observation that ∆ is odd shows that this constant must be 0, and concludes the proof of formula (4).
To prove (3), we now let
Proposition 3.2 and the fact that
1/n2<∞ guarantee that the prod-uct P (z) converges, and that away from the integers we have
P(z)
and so P (z) = cG(z) for some constant c. Dividing this identity by z, and taking the limit as z→ 0, we find c = 1.
Remark. Other proofs of (4) and (3) can be given by integrating analogous identities for π2/(sin πz)2 derived in Exercise 12, Chapter 3, and Exercise 7, Chapter 4. Still other proofs using Fourier series can be found in the exercises of Chapters 3 and 5 of Book I.
4. Weierstrass infinite products 145 4 Weierstrass infinite products
We now turn to Weierstrass’s construction of an entire function with prescribed zeros.
Theorem 4.1 Given any sequence {an} of complex numbers with
|an| → ∞ as n → ∞, there exists an entire function f that vanishes at all z = an and nowhere else. Any other such entire function is of the form f (z)eg(z), where g is entire.
Recall that if a holomorphic function f vanishes at z = a, then the multiplicity of the zero a is the integer m so that
f (z) = (z− a)mg(z),
where g is holomorphic and nowhere vanishing in a neighborhood of a.
Alternatively, m is the first non-zero power of z− a in the power series expansion of f at a. Since, as before, we allow for repetitions in the sequence {an}, the theorem actually guarantees the existence of entire functions with prescribed zeros and with desired multiplicities.
To begin the proof, note first that if f1and f2 are two entire functions that vanish at all z = an and nowhere else, then f1/f2 has removable singularities at all the points an. Hence f1/f2 is entire and vanishes nowhere, so that there exists an entire function g with f1(z)/f2(z) = eg(z), as we showed in Section 6 of Chapter 3. Therefore f1(z) = f2(z)eg(z) and the last statement of the theorem is verified.
Hence we are left with the task of constructing a function that vanishes at all the points of the sequence{an} and nowhere else. A naive guess, suggested by the product formula for sin πz, is the product
n(1− z/an).
The problem is that this product converges only for suitable sequences {an}, so we correct this by inserting exponential factors. These factors will make the product converge without adding new zeros.
For each integer k≥ 0 we define canonical factors by
E0(z) = 1− z and Ek(z) = (1− z)ez+z2/2+···+zk/k, for k≥ 1.
The integer k is called the degree of the canonical factor.
Lemma 4.2 If|z| ≤ 1/2, then |1 − Ek(z)| ≤ c|z|k+1 for some c > 0.
Proof. If |z| ≤ 1/2, then with the logarithm defined in terms of the power series, we have 1− z = elog(1−z), and therefore
Ek(z) = elog(1−z)+z+z2/2+···+zk/k = ew,
146 Chapter 5. ENTIRE FUNCTIONS
where w =−∞
n=k+1zn/n. Observe that since|z| ≤ 1/2 we have
|w| ≤ |z|k+1
∞ n=k+1
|z|n−k−1/n≤ |z|k+1
∞ j=0
2−j ≤ 2|z|k+1.
In particular, we have|w| ≤ 1 and this implies that
|1 − Ek(z)| = |1 − ew| ≤ c|w| ≤ c|z|k+1.
Remark. An important technical point is that the constant c in the statement of the lemma can be chosen to be independent of k. In fact, an examination of the proof shows that we may take c= e and then c = 2e.
Suppose that we are given a zero of order m at the origin, and that a1, a2. . . are all non-zero. Then we define the Weierstrass product by
f (z) = zm
∞ n=1
En(z/an).
We claim that this function has the required properties; that is, f is entire with a zero of order m at the origin, zeros at each point of the sequence{an}, and f vanishes nowhere else.
Fix R > 0, and suppose that z belongs to the disc |z| < R. We shall prove that f has all the desired properties in this disc, and since R is arbitrary, this will prove the theorem.
We can consider two types of factors in the formula defining f , with the choice depending on whether|an| ≤ 2R or |an| > 2R. There are only finitely many terms of the first kind (since|an| → ∞), and we see that the finite product vanishes at all z = an with|an| < R. If |an| ≥ 2R, we have|z/an| ≤ 1/2, hence the previous lemma implies
|1 − En(z/an)| ≤ c
azn
n+1≤ 2n+1c .
Note that by the above remark, c does not depend on n. Therefore, the product
|an|≥2R
En(z/an)
defines a holomorphic function when |z| < R, and does not vanish in that disc by the propositions in Section 3. This shows that the function
5. Hadamard’s factorization theorem 147 f has the desired properties, and the proof of Weierstrass’s theorem is complete.
5 Hadamard’s factorization theorem
The theorem of this section combines the results relating the growth of a function to the number of zeros it possesses, and the above product theorem. Weierstrass’s theorem states that a function that vanishes at the points a1, a2, . . . takes the form
eg(z)zm
∞ n=1
En(z/an).
Hadamard refined this result by showing that in the case of functions of finite order, the degree of the canonical factors can be taken to be constant, and g is then a polynomial.
Recall that an entire function has an order of growth≤ ρ if
|f(z)| ≤ AeB|z|ρ,
and that the order of growth ρ0 of f is the infimum of all such ρ’s.
A basic result we proved earlier was that if f has order of growth≤ ρ, then
n(r) ≤ Crρ, for all large r,
and if a1, a2, . . . are the non-zero zeros of f , and s > ρ, then
|an|−s<∞.
Theorem 5.1 Suppose f is entire and has growth order ρ0. Let k be the integer so that k≤ ρ0 < k + 1. If a1, a2, . . . denote the (non-zero) zeros of f , then
f (z) = eP (z)zm
∞ n=1
Ek(z/an),
where P is a polynomial of degree≤ k, and m is the order of the zero of f at z = 0.
Main lemmas
Here we gather a few lemmas needed in the proof of Hadamard’s theorem.
148 Chapter 5. ENTIRE FUNCTIONS