Miscellaneous Problems
[52/88%]If the function is regular, single valued and bounded in the strip , and vanishes there at the points () then either the series of positive terms
is convergent, or is identically equal to .
See Problem 297 of Part III.
Assume that the coefficient of the linear homogeneous differential equation
is an entire function. The necessary and sufficient condition that the general solution of this differential equation be an entire function is that the remaining coefficients are also entire functions.
Let the function be regular (possibly many-valued) in the annular region , , and satisfy there identically an equation of the form
where are regular in a neighbourhood of the point . If there exists a power series such that the function remains bounded in the neighbourhood of for infinitely many values of , then is regular in the neighbourhood of , and we have .
Let the function be regular and single-valued for , . Then there exists an integer , an entire function and a power series
convergent for , such that for we have
If in the assumption as well as in the conclusion we replaced the inequality by the inequality , the theorem obtained would be invalid.
Let be a meromorphic periodic function of period that has in the strip only a finite number of zeros and poles. Denote by the maximum and by the minimum of for . If it is the case that
then must be a rational function of .
Let be an analytic function, , and let the square of the absolute value of
be an algebraic function of the real variables and . Then the function is itself an algebraic function of .
H. A. Schwarz, oral communication.
There does not exist a function which is regular analytic along the real axis and which assumes for real values of the variable every value in the interior of a fixed circle. In brief: There does not exist an analytic Peano-curve.
E. Landau.
Find, if possible, analytic functions , which differ from each other not merely by constant factors, are regular in a domain and for which the relation
holds in .
Find, if possible, two non-constant analytic functions and , which are regular in a domain and for which the relation
holds in .
See Problem 58 of Part III.
The modular graph (see Volume I, p. 130) of an entire function is everywhere convex from below in just two cases: Either when
or when
where and are arbitrary complex numbers, a non-negative integer.
See the definition preceding Problem 130 of Part III. Cf. G. Polya, problem: Jber. deutsch. Math. Ver., Section 2, 35, p. 48 (1926). Solution by H. Kneser, op. cit. 35, p. 119 (1926), and by N. Tchebotarev, op. cit. 36, pp. 40-41 (1927).
The modular graph (see Volume I, p. 130) of an entire function is everywhere convex from below in just two cases: Either when
or when
where and are arbitrary complex numbers, a non-negative integer.
See the definition preceding Problem 130 of Part III. Cf. G. Polya, problem: Jber. deutsch. Math. Ver., Section 2, 35, p. 48 (1926). Solution by H. Kneser, op. cit. 35, p. 119 (1926), and by N. Tchebotarev, op. cit. 36, pp. 40-41 (1927).
We say that two entire functions and have the same -points if the two functions
are both entire. Find two distinct entire functions, which have the same -, - and -points. (Naturally we require , , .)
Note that there do not exist two distinct entire functions of finite order that have the same -, -, - and -points ( all distinct). G. Polya: Nyt Tidsskr. for Math. (B) 32, p. 21 (1921).
Does there exist an entire function which satisfies the equations
if the sequence of numbers is prescribed arbitrarily?
For the analogous interpolation problem for polynomials cf. Problems 75, 76 of Part VI.
Given the numbers
for subject to the conditions:
is a positive integer, however the are unrestricted.
Then there exists an entire function such that
for , .
The condition prescribes the initial terms of the expansion of about the point
for .
Given the numbers
for subject to the conditions:
is a positive integer, however the are unrestricted.
Then there exists an entire function such that
for , .
The condition prescribes the initial terms of the expansion of about the point
for .
Suppose that and are entire functions that have no common zeros. Then there exist two entire functions and such that
Suppose that and are entire functions that have no common zeros. Then there exist two entire functions and such that
Let be regular for and set . Then we have
(continued). If is defined for the function in the same manner as for , , then we have
E. Landau.
With the aid of Problem 123 of Part II, obtain a new proof for the Hadamard three-circle theorem (Problem 304 of Part III).
E. Landau.
Prove the following generalization of problem 160: If is defined as in problem 157, then under the assumptions of problem 160 we have the following estimate of the coefficients
I. Schur.
Assume the Bernstein theorem for trigonometric polynomials (Problem 82 of Part VI) in the following imprecise form: There exists an absolute constant , with the property that, if denotes a trigonometric polynomial of th order whose absolute value does not exceed , then we have
Find a method of deducing from this estimate the sharper estimate
There exist entire functions that increase arbitrarily rapidly as along a ray. More precisely: If is an arbitrary, strictly positive, monotonically increasing function defined for , there exists an entire function , which assumes real values for real and satisfies for the inequality . (See Problem 290 of Part III.)
H. Poincare: Amer. J. Math. 14, p. 214 (1892), cf. H. Bohr: Nyt Tidsskr. for Math. (B) 27, pp. 73-78 (1916).
There exist entire functions that tend to along the positive real axis, but tend to along any other ray emanating from the origin as . Can a rational entire function behave in this manner?
There exist transcendental entire functions that tend to along every ray emanating from the origin. --- Can this happen uniformly?
H. von Koch: Ark. for Mat., Astron. och Fys. 1, pp. 627-641 (1903).
There exist entire functions that are real-valued along the positive real axis and along it tend to while tending to along any other ray emanating from the origin. --- Can an entire function of finite order behave in this fashion?
Cf. J. Malmquist: Acta Math. 29, pp. 203-215 (1905); Problems 158, 160 of Part III.
There exist not identically vanishing entire functions that tend to along every ray emanating from the origin.
G. Mittag-Leffler: Proceedings of the 3rd International Congress of Mathematicians in Heidelberg 1904. Leipzig: B. G. Teubner 1905, pp. 258-264. Atti del IV. congr. internaz. dei mat. Roma 1908, 1. Rome: Tip. della Acc. dei Lincei 1909, pp. 67-85.
There exist entire functions that tend to along all rays running from the origin into the interior of the upper half-plane, and that tend to along all rays running from the origin into the interior of the lower half-plane. The convergence is in fact uniform in every sector , or , where .
Let the whole plane be divided into sectors by rays emanating from the origin. There exists an entire function that tends in these sectors (more precisely, as in problem 185) to respectively, where are arbitrarily assigned complex numbers.
G. Polya: Intermed. des math. Series 2, 1, pp. 81-82 (1922).
Let the rays emanating from the origin be divided in any manner into two classes. Does there exist, corresponding to every such division, an entire function that tends to along the rays of the first class, and that tends to along the rays of the second class?
The numbers and are the only asymptotic values of .
The numbers and are the only asymptotic values of the function .
Let be a positive integer. The integral function of order
has exactly distinct finite asymptotic values.
Let the sequence of positive numbers
be chosen such that the series
converges uniformly in every finite domain of the -plane and thus represents an entire function . (Set for example .)
Show that the set of asymptotic values of the entire function thus defined has the power of the continuum. More precisely: All numbers of the form
are asymptotic values.
F. Iversen: Ofversikt av Finska Vetenskaps-Soc. Forh. 58(A), No. 3 (1915-1916).
If an entire function converges to distinct finite asymptotic values along distinct rays emanating from the origin, then its order is not less than .
For every entire function (that is not a constant) the number is an asymptotic value.
Cf. F. Iversen: These, Helsingfors 1914.
Let be the number of zeros of . Determine the polynomial of degree such that is regular in the whole -plane, and then the polynomial of degree at most such that also
is regular in the whole -plane. There hence exists (using problem 193) a continuous curve going to infinity such that at points sufficiently far along it we have
Let be a function that can be analytically continued everywhere in the annular region . If in this process and all its derivatives remain bounded, then is single-valued in this region and regular at the point .
T. Carleman.
If is an entire function of genus and is an arbitrary positive number, then we have
on all circles with sufficiently large radii, and
on certain circles with arbitrarily large radii.
Let be the maximum and the minimum of the absolute value of an entire function on the circumference of the circle . If
and , then we have also
See problem 196, Problem 332 of Part III.
Let be distinct positive numbers such that the series
is divergent. If a function which is properly integrable over the interval satisfies the condition
then at every point of continuity . (A generalization of Problem 139 of Part II.)
is an analytic function of ; see Problem 298 of Part III.
Let be a transcendental entire function of order . Let its coefficients be different from and its zeros be distinct, for . If a function which is defined and properly integrable over the interval satisfies the condition
then at every point of continuity . (See Problem 139 of Part II.)
T. Carleman.
Let be a transcendental entire function of genus with all its zeros , real and distinct. If a function defined and properly integrable in the interval satisfies the condition
then at every point of continuity . (We may, for example, set or .)
T. Carleman.
Set
Assume that there exist two positive constants and such that
-
the sequence is bounded, and
-
for all real values of . Then we have for all real values also
and equality holds only if , where are constants. (A generalization of Problem 82 of Part VI.)
See Problem 165 of Part III.
(continued). If is the distance of the point from the real axis (), then
Analogue of Problem 270 of Part III.
Let the entire function satisfy the same conditions as the function in problem 201, and in addition let be an odd function, . Then we have for real
Equality holds only if , and if . (Analogue of Problem 81 of Part VI.)
See Problem 166 of Part III.
(continued). Deduce problem 201 from problem 203.
Cf. Problem 82 of Part VI.
Let be an entire function of order , , that is bounded on the positive real axis. If denotes an arbitrary positive number, then as tends to infinity through positive values we have
We assume that the sequence of complex numbers has the following three properties:
-
The series
are convergent.
-
.
-
There exist two real numbers and such that
Then is convergent.
The conclusion holds under a wider assumption: The series listed in (1) need not be convergent; it is sufficient to assume that their partial sums are bounded. Yet the conclusion becomes invalid if we drop assumption (2) or if we require less than the first part of (3), namely that
Cf. Problem 36 of Part III. G. Polya, problem: Jber. deutsch. Math. Verein. Section 2, 35, p. 48 (1926). Solution by L. Tchakalov, op. cit. 37, pp. 30-33 (1928).
The functions ; are regular analytic in a region of the -plane where
If are linearly independent, then so also are , and
for ; the constants form a unitary matrix.
R. Nevalinna and G. Polya, problem: Jber. deutsch. Math. Verein. Section 2, 40, p. 80 (1931). Solution by H. Schmidt, op. cit. 43, pp. 6-7 (1933).
We consider the approximation of the entire function by polynomials. We define the integer
(termed the degree of approximation of the function on the circle to accuracy ) as the degree of the polynomial of the lowest possible degree for which
(, ). Then
where we keep fixed when computing the first limit and fixed when computing the second limit; is the order of .
Cf. Problem 123 of Part III. See problem 51 for the definition of order. G. Polya, problem: Jber. deutsch. Math. Verein., Section 2, 34, pp. 97-98 (1925). Solution by G. Szego, op. cit. 35, pp. 86-89 (1926).
Let be an entire function whose growth does not exceed the minimum type of order ; that is, remains bounded in the whole -plane provided that is a fixed positive number. Assume that the sequence
is bounded. Then reduces to a constant.
Cf. Problem 220(4), Problem 254 of Part III. G. Polya, problem: Jber. deutsch. Math. Verein., Section 2, 40, pp. 80-81 (1931). Solutions op. cit. 43 (1933) by L. Tchakalov, pp. 10-11 and G. Szego, pp. 11-13; comments by G. Polya, pp. 67-69. See also R. E. A. C. Paley and Norbert Wiener: Fourier transforms in the complex domain, Amer. Math. Soc. Colloquium Publ. 19, New York 1934, pp. 81-83.
We consider square matrices with rows and columns, and let capital letters denote such matrices. Let
be an entire function and a matrix. Then the series
converges to a well-defined matrix.
Given the matrix , when does there exist a matrix such that
See Picard’s theorem, for example in Ahlfors pp. 297-298, Hille Vol. II pp. 219-221 or Titchmarsh pp. 277-284. Cf. problem 194. G. Polya, problem: Jber. deutsch. Math. Verein., Section 2, 40, p. 80 (1931). Solution by G. Szego, op. cit. 43, pp. 7-9 (1933).
Let be a single-valued analytic function which is regular everywhere including the point , except at the point . In a neighborhood of the point it has the expansion
and in a neighborhood of the point the expansion
If there exists a constant such that both and are bounded (), then is a rational function.
G. Polya, problem: Jber. deutsch. Math. Verein. Section 2, 40, p. 81 (1931). Solutions op. cit. 43 by N. Obreschkov, pp. 13-15, G. Szego, pp. 15-16, and N. Tchebotarev, pp. 16-17.
Let the numbers be real, and satisfy
Furthermore, let be continuous in the interval . Then it follows from
for , that vanishes identically. (A fraction of the whole system of Fourier functions is closed over the corresponding fraction of the whole interval.)
Cf. problem 198. G. Polya, problem: Jber. deutsch. Math. Verein., Section 2, 40, p. 81 (1931). Solution by O. Szasz, op. cit. 43, pp. 20-23 (1933). For a stronger result, see Paley and Wiener, op. cit. problem 209, pp. 83-85. See also Norman Levinson: Gap and Density Theorems. Amer. Math. Soc. Colloquium Publications 26, New York 1940, pp. 3-5.