Sequences of Analytic Functions
[59/98%]We use the same notation and hypothesis as before and expand
Derive this formula from Lagrange's formula or Lagrange's formula from this one by correctly using the generality of both formulas. [The existence of one formula for a certain implies immediately the other formula for another .]
Prove the formula in problem 207 directly by expressing the coefficient of as a Cauchy integral.
Expand in ascending powers of the solution of the transcendental equation
that vanishes for .
(continued). Expand in powers of where is an arbitrary constant.
Expand in ascending powers of the solution of the trinomial equation
that becomes for .
(continued). Expand in powers of , where denotes an arbitrary constant. ( is the solution of the trinomial equation
(continued). Note the cases and derive problems 209, 210 by taking the limit in problems 211, 212.
Evaluate the sum of the power series
What is its radius of convergence?
Prove problem 156 with the help of the results of problem 214.
Let and denote rational numbers. Then the series
represents an algebraic function of .
Arrange the successive powers of the trinomial in a regular triangular array
The sum of the middle terms (in boldface: ) is
Arrange the successive powers of the binomial in a regular triangular array (Pascal's triangle)
Find the sum of the middle terms (in boldface) and, more generally, the sum of any column.
Find the generating functions of the polynomials , , , defined by the formulas
(Legendre's polynomials);
, , (Jacobi's polynomials);
, (generalized Laguerre's polynomials).
Cf.Part VI, problems 84, 98, 99. The generating function of the Legendre polynomials is the series
the sum of which has to be found as a function of and ; similarly in the other two cases.
Let be a constant of sufficiently small modulus. Then the following formulas are valid for :
The four formulas mentioned in problem 220 hold for any polynomial . (In this case the series are obviously finite.)
The formulas (1), (2) given in problem 220 are also valid for any rational function if the real part of is larger than the real part of any of the finite poles of ; formula (1) requires the additional condition that be regular for . --Do the formulas (3) and (4) hold for rational but not entire functions?
where , , denote arbitrary constants.
Define
and establish the relation
Define
and show that
Define
and show that
is a single-valued function of . The expansion of in powers of contains only positive coefficients (except the constant term) [problem 227].
Prove that
We assume that the function
Express the coefficients in terms of the real and the imaginary part resp.of on the circle , .
(continued). We set and assume that is real and . Then
(continued). Suppose does not vanish on and that its zeros in the disk are . Then we have for
where is a real constant. [Consequence of problem 231 as problem 120 is a consequence of problem 119.]
The function is regular, its real part is positive in the open disk and continuous in the closed disk . If the real part becomes identically zero on an arc of the circle the imaginary part of changes on this arc always in the same sense: it decreases as increases.
Let be regular in the disk , , are real. Then the equation
holds for provided that it holds for .
The function
is assumed to be regular and to have positive real part in the open disk . Then , In none of these inequalities can we replace by a smaller number.
Suppose that the function
on the disk . Then the inequality
holds for . Example: , , .
We assume that the Laurent series
converges on the annulus (sphere from which two points have been removed) and that and are essential isolated singular points. The maximum of the real part of on the circle is denoted by . increases to faster than any power of as and faster than any power of as . Precisely
We assume that the function is regular in the disk and we denote by the largest oscillation of the real part of in , i.e. is the least upper bound of for , . Then we have
The factor cannot be replaced by a smaller one.
Interpret this proposition geometrically.
Let the function be regular in the disk and denote by the largest oscillation of for , i.e. is the least upper bound of for , . Then we have
The factor can not be replaced by a smaller one. Interpret this proposition geometrically.
Let the function satisfy the following conditions:
-
is regular, in the disk ;
-
does not vanish in the closed half-disk , ;
-
has in the disk the zeros . Then
[We may assume ; problems 232, 120.]
Suppose that the unit circle is the circle of convergence of a certain power series and that there are only poles of first order on this circle (no other singularities). Then the sequence of coefficients is bounded.
If there is only one singular point on the circle of convergence of and if is a pole then
Let be the expansion into a power series of a rational function whose denominator (relative prime to the numerator) has degree . The radius of convergence is called and denotes the largest among the numbers . Then
(lim not lim sup!)
Let be the number of non-zero coefficients among the coefficients . If there are only poles (and no other singularities) on the circle of convergence of the power series the number of such poles is not smaller than
Example: .
We assume that the coefficients of the power series are real and that and are poles and the only singularities on the circle of convergence, . We call the number of changes of sign in the sequence . Then
If there is also a pole among the singularities on the circle of convergence the power series converges at no point of the circle of convergence.
Suppose that the point is a regular point of the power series
that converges inside the unit disk. Then the Dirichlet series, assumed convergent for certain values of ,
defines an entire function. In the case where the point is a pole of order of the function , is a meromorphic function which can have poles only at the points (only the last one must be a pole); the poles are simple. [, cf.Part II, problem 117; is an entire function of if .]
The sequence is assumed to satisfy the condition
Then the series
converges in the infinite strip
of the -plane. The convergence is absolute and uniform in any closed interior strip , ; there the series defines an analytic function . The function vanishes identically only if all the coefficients vanish. [Compute
We assume that the power series
converges inside the unit disk and that and all its derivatives tend to as tends to on the real axis, i.e., Then there are two possibilities:
-
vanishes identically;
-
is a singular point for . If the power series converges in a disk larger than the unit disk, i.e.if
we are necessarily dealing with the first case. The weaker condition
admits the same conclusion. [Construct the function of problem 248.]
The proposition 249 is not valid if the condition on the coefficients of , namely , is replaced by
[Put
If the series
converges at one single point at which is regular then is an entire function and the series converges at every point. The convergence is uniform in any finite domain of the -plane.
If the sequence
is bounded at a single point of the -plane then is an entire function and the sequence stays bounded at all the points of the -plane. It even has the same limit superior at all the points.
Let
be two infinite sequences, the second one being arbitrary, the first one such that , when , and that
converges absolutely. The equations
define a unique polynomial of degree not larger than . If the sequence
converges at a single point different from it converges at every point , even uniformly in any finite domain of the -plane.
Let
denote a sequence that is infinite in two directions and be the polynomial of degree that satisfies the equations
If the sequence of polynomials
converges for two different non-integral values of it converges at every point , even uniformly in any finite domain of the -plane.
The sequence is given. A polynomial of degree not exceeding can be found [Part VI, problem 76] for which
These conditions define uniquely [Part VI, problem 75]. If the sequence
converges at a single point , , it converges at every point , in fact uniformly in every finite domain of the -plane.
We assume that in the unit disk, , the functions are regular and different from zero and that their absolute values are smaller than . If , then in the entire open disk ; the convergence is actually uniform in every smaller disk .
The harmonic functions
are assumed to be regular and positive in a certain open region of the -plane. If the infinite series
converges at a single point of it converges everywhere in ; in fact, it converges uniformly in any closed subdomain of .
We suppose that the functions of the sequence are analytic in the open region and that the sequence of their real parts converges uniformly in every closed subdomain of . Then the sequence of their imaginary parts either diverges at all points or it converges uniformly in any closed subdomain of .
The series
converges uniformly in any domain that lies either entirely inside or entirely outside the unit circle and its sum is or according as or [problem 14 of Part I].
Let denote an arbitrary constant, . The series
converges uniformly for all positive values of ; it represents the function for and a different analytic function for .
The sequence of functions
converges uniformly in any finite domain that does not contain the imaginary axis.
Let
and put
The sequence of iterated functions
converges to , when , to when and diverges when .
Let denote the support function of the infinite convex domain considered in problem 114. The sequence
where , is bounded in the entire half-plane [problems 12, and Part II, problem 220]; is the smallest function of the angle that keeps the sequence bounded.
Let denote the support function of the convex domain considered in problem 115. The sequence
where , is bounded in the entire -plane [problems 13, and Part II, problem 221]; is the smallest function of the angle that keeps the sequence bounded.
Let denote the support function of the convex domain considered in problem 116. Then
, in the entire plane.