§14.4 The Second Fundamental Theorem
14.4 The Second Fundamental Theorem
Whereas the First Fundamental Theorem gives the relation between the general size of relative to and , efforts have been made to quantify the relative size of and . This question was answered by R. Nevanlinna in July 1924 with considerable accuracy via the inequality
where are distinct and is a term that is generally small relative to (is for most ). It also implies that in most cases, will be much larger than . For example, assume ’s meromorphy is on all of . Then if there are two values where the proximity dwarfs the counting function, such as when
then for all other values on the Riemann sphere,
where the precise formulation allows for a sequence diverging to to be chosen so that for in this sequence. This implies . This in turn then proves Picard’s theorems (see Section 14.5.1). As we shall later see, the conclusions of the theorem have even further extensibility.
Regarding Nevanlinna’s original paper containing the result, mathematician Hermann Weyl has stated in 1943 that “the appearance of this paper has been one of the few great mathematical events of our century.”
Theorem 14.4.1 (Second Fundamental Theorem of Nevanlinna Theory, Part 1).
Let be meromorphic and non-constant (). Suppose that are distinct finite complex numbers. Then for any positive ,
where and
where is the first nonzero coefficient of the innermost Laurent expansion of (at the origin).Remark.
For interpretive purposes, will serve the purpose of a generally unimportant small error term. The utility of this theorem is not realized until more useful conclusions are drawn on its estimation, which will be denoted by the second part of the theorem.Proof.
Define
Fixing , we then assume two cases
such that . For any , we have
It follows that
Then
Since
from Proposition 14.1.2, it follows that
Observe that for each , , and therefore
There exists no such . Then all have the property that . It follows that
Then (14.4.2) holds for this case trivially.
Integrating the relation (14.4.2) (which holds in all cases) gives that
Observe that
Let be the first nonzero coefficient of the Laurent expansion for . It follows that
so the first nonzero coefficient of the Laurent expansion of is and that of is . It follows from
that
Combining this with (14.4.3) gives
Using (14.1.2) three times gives that
Thus, we obtain
where is defined as in (14.4.1). This concludes the proof.