Power Series with Integral Coefficients in the Sense of Hurwitz
[14/100%]If is a power series with H-integral coefficients, then
are also power series with H-integral coefficients.
If and are power series with H-integral coefficients, then
are also power series with H-integral coefficients, and under the further assumption that also
If is a power series with H-integral coefficients and , then
is also a power series with H-integral coefficients, [174].
If and are power series with H-integral coefficients and , then is also a power series with H-integral coefficients.
The function , well defined by the differential equation
and the initial conditions , , may be expanded in a power series with H-integral coefficients.
For every prime number , we have
For every composite number greater than 4 we have
The Bernoulli numbers are defined as the coefficients in the power series expansion
(Problem 154 of Part I). We have
In general we have
where is an integer and denote those prime numbers that exceed by one the divisors of . [Expand first and then in ascending powers of and apply 179--181.]
The coefficients in the series
where denotes the function defined in 178, are rational numbers and moreover the denominator of is not divisible by any square other than 1 and is divisible only by such prime numbers as are . [Expand first and then in ascending powers of .]
The differential equation
has a well-defined solution of the form
( is a particular elliptic function, termed a ``lemniscate function''; its period-parallelogram is a square.) The numbers are rational, and moreover the denominator of is not divisible by any square other than 1, and is divisible only by such prime numbers as are . [Show that , cf. 183. Expand first and then in ascending powers of ; as a function of satisfies a linear differential equation of second order.]
If a power series with H-integral coefficients satisfies a homogeneous linear differential equation with constant coefficients, then the sequence of coefficients is periodic mod after a certain number of terms, where is an arbitrary integer. [Examples of this are found already in 179, 180.]
The power series
shows that theorem 185 cannot without further assumptions be extended to homogeneous linear differential equations whose coefficients are polynomials.
If a transcendental entire function has a power series expansion with H-integral coefficients, then we have for the maximum modulus (Chapter 1 of Part IV) of