Connection between , , and
[20/100%]For an entire function let
The convergence of the series
is assured, excluded or undecided according as
For the Weierstrass function, in the case when the period parallelogram is a square with sides of length ,
as tends to .
See Hille, Vol. II pp. 132-133 and Hurwitz-Courant, pp. 174-175.
There is an entire function for which
for (see Problem 50 of Part I). Construct an entire function for which
for .
For the entire functions
determine the limits of the quotients
as (or in the first quotient) tends to infinity, and collect the results in a table.
For the first and last quotients are meaningless, for only the third and the last are to be determined under the assumption that the period parallelogram is a square. The last quotient gives the exponent of convergence of the zeros, see Problem 149 of Part II. Use problems 1-4, 13, 27, 28 and Stirling's formula for the asymptotic value of .
For any entire function
(it is obvious that the inequality holds). The common value of these two limits is called the order of the entire function.
The order of an entire function may also be defined as the exponent of convergence (this is the notation of Part I, Chapter 3, Section 2) of the sequence .
The order of an entire function with positive coefficients may also be defined as the following limit:
For entire functions of finite order we have the following result (stronger than problem 51):
For transcendental entire functions the integral
is convergent for .
For any entire function, given any arbitrary , , there exist arbitrarily large values of such that
For an entire function of finite order we have the following result (stronger than problem 56): given any arbitrary , , there exist arbitrarily large values of such that
The order of an entire function of genus zero is equal to the exponent of convergence of its zeros (see Volume I, pp. 25-26, Titchmarsh p. 250, Hille Vol. II, p. 188).
For an entire function of finite order , , whose central index has the jump-points which are regularly spaced in the sense of Chapter 4, Section 1 of Part II, we have
See Problem 159 of Part II. Problems 59-63 are also discussed in G. Polya: Math. Ann. 88, pp. 177-183 (1923).
For entire functions of finite order , , without any special conditions of regularity we have
See Problem 160 of Part II.
Let be the exponent of convergence of the sequence , which is regularly spaced in the sense of Chapter 4, Section 1 of Part II, and let . For the entire function of genus zero
we have
if is a fixed number, .
See Problem 159 of Part II.
For the entire function discussed in problem 61 we have, even without assuming the regular spacing of the sequence ,
See Problem 161 of Part II.
For an entire function whose zeros have a finite exponent of convergence
See problem 32.
Let be an entire function and let and be defined as the geometric means of on the circle , and in the circular disc , respectively (this is the notation of Problem 121 of Part III). If the moduli of the zeros of are regularly spaced (this is the notation of Chapter 4, Section 1 of Part II), then
where , , denotes the exponent of convergence of the zeros. For polynomials the above limit also exists and equals .
(Continued from problem 64.) Without assuming the regular spacing of the zeros we have
Let be an entire function of finite order and and the arithmetic means of on the circle and in the circular disc respectively. Then