§14.2 Properties of and the First Fundamental Theorem
14.2 Properties of and the First Fundamental Theorem
Proposition 14.2.1.
If () are meromorphic in , then for ,
- .
- (subadditivity).
- .
- .
- .
- .
Proof.
Let be an arbitrary point in the disk. If is the pole order of at (0 if it is not a pole), then the pole order at of does not exceed . It is hence clear that .
Moreover, if are the poles of in the disk counted according to orders, and are the poles of , then
Recognizing that
Part 2 then follows. Since the pole order at of does not exceed , it also follows that . The same logic can be applied henceforth to prove Part 1.
Part 3 and Part 4 are clear from Proposition 14.1.2. Part 5 and Part 6 follow the previous inequalities.
Theorem 14.2.2.
Let be meromorphic such that . For ,
where is the first nonzero coefficient of the innermost Laurent expansion of at the origin.Proof.
For , from (14.1.2) on (let be the first nonzero coefficient of the innermost Laurent series) we obtain
Therefore, by integrating in ,
For any ,
which follows directly from Jensen’s formula on the function (by considering when and ). Letting , we have by setting ,
Hence, from absolute convergence we have
From (14.2.1), it follows that
If , then subtracting from does not modify the first nonzero coefficient of the innermost Laurent series (). Thus, in this case
Otherwise, unless this quantity is 0 (cancels), which can happen for at most one value, which is negligible when integrated. Thus by (14.2.2),
Theorem 14.2.3.
For (non-constant) meromorphic in , is a non-decreasing convex (not necessarily strictly convex) function of (for ).Proof.
Applying to Theorem 14.2.2, we have
by Lebesgue’s Dominated Convergence Theorem. Because the counting function is non-decreasing in , it is also non-decreasing in . Theorem 14.2.4 (First Fundamental Theorem of Nevanlinna Theory).
Let be (non-constant) meromorphic on where . Then for any ,
where for and is the first nonzero coefficient of the innermost Laurent series expansion of about the origin.Proof.
Since for , by the properties of as in Proposition 14.1.2,
Integrating over implies
From
we obtain
Letting , the two proximity-related inequalities give
Then by Proposition 14.1.5, and the fact that the poles of match those of (more importantly, ),
For , we have
which shows that is essentially independent of the choice of , except for a bounded term. Thus, this motivates why is characteristic of .
As we have seen before, it is often pedantic and somewhat annoying to account for cases where is either zero or infinity, which is a minor grievance in Nevanlinna theory. Expositions from [5] and [3] tend to leave out this tedious treatment. However, here we will make this distinction whenever necessary for completeness.
Corollary 14.2.4.1.
Let be (non-constant) meromorphic on . Then for ,
Proof.
By the First Fundamental Theorem (Theorem 14.2.4), we have
where and is the first nonzero coefficient of the Laurent expansion for . Hence,
By Theorem 14.2.2, we thus have
This implies thatRemark.
Since is bounded in the integrated sense, if is generally large, then for most values, will be nearly equal to .Proposition 14.2.5.
Let be meromorphic on and suppose . For any , the following properties hold:
- .
- .
- .
- .
Proof.
Since
and by
it follows that
and the conclusions of Part 1 and Part 2. Part 3 is a corollary of the First Fundamental Theorem (Theorem 14.2.4). Lastly, because a pole of has order times of that of , it follows that . If , it follows that exactly. If , . Hence, .
Adding the two quantities and together gives Part 4.
We now provide some classical examples of the Nevanlinna characteristic:
Let
be an arbitrary rational function in reduced form. If , then for sufficiently large , in every direction. This implies for any complex and sufficiently large (). This implies . Additionally, the equation has complex solutions by the Fundamental Theorem of Algebra (Theorem 3.3.1). Thus, for sufficiently large (), any has the property that ,
Hence,
Similarly, by a preceding result. It then follows that if ,
Lastly, the case where (derived with ) is resolvable with
In all cases,
where is defined to be the degree of the rational function .
Unless , the proximity function vanishes for sufficiently large . In this case, let be the multiplicity at which attains at . If is finite,
If has a pole of order at , we have likewise that
Consider
By its entireness, for any , and the proximity is given by
Therefore,
Moreover, and , whereas for , the solutions to are in the form of , where . The condition is equivalent to
It follows that