Nevanlinna function

Every Nevanlinna function N admits a representation

${\displaystyle N(z)=C+Dz+\int _{\mathbb {R} }\left({\frac {1}{\lambda -z}}-{\frac {\lambda }{1+\lambda ^{2}}}\right)d\mu (\lambda ),\quad z\in \mathbb {H} ,}$

where C is a real constant, D is a non-negative constant and μ is a Borel measure on R satisfying the growth condition

${\displaystyle \int _{\mathbb {R} }{\frac {d\mu (\lambda )}{1+\lambda ^{2}}}<\infty .}$

Conversely, every function of this form turns out to be a Nevanlinna function. The constants in this representation are related to the function N via

${\displaystyle C=\mathrm {Re} (N(i))\qquad {\text{and}}\qquad D=\lim _{y\rightarrow \infty }{\frac {N(iy)}{iy}}}$

and the Borel measure μ can be recovered from N by employing the Stieltjes inversion formula (related to the inversion formula for the Stieltjes transformation):

${\displaystyle \mu ((\lambda _{1},\lambda _{2}])=\lim _{\delta \rightarrow 0}\lim _{\varepsilon \rightarrow 0}{\frac {1}{\pi }}\int _{\lambda _{1}+\delta }^{\lambda _{2}+\delta }\mathrm {Im} (N(\lambda +i\varepsilon ))d\lambda .}$

A very similar representation of functions is also called the Poisson representation.[2]

• Some elementary examples of Nevanlinna functions follow (with appropriately chosen branch cuts in the first three). (${\displaystyle z}$ can be replaced by ${\displaystyle z-a}$ for some real number ${\displaystyle a.}$)

${\displaystyle z^{p}{\text{ with }}0\leq p\leq 1}$

${\displaystyle -z^{p}{\text{ with }}-1\leq p\leq 0}$

These are injective but when p does not equal 1 or −1 they are not surjective and can be rotated to some extent around the origin, such as ${\displaystyle i(z/i)^{p}{\text{ with }}-1\leq p\leq 1.}$

A sheet of ${\displaystyle \ln(z)}$ such as the one with ${\displaystyle f(1)=0.}$

${\displaystyle \tan(z)}$ (an example that is surjective but not injective)

• A Möbius transformation

${\displaystyle z\mapsto {\frac {az+b}{cz+d}}}$

is a Nevanlinna function if (but not only if) ${\displaystyle a^{\ast }d-bc^{\ast }}$ is a positive real number and ${\displaystyle \mathrm {Im} (b^{\ast }d)=\mathrm {Im} (a^{\ast }c)=0.}$ This is equivalent to the set of such transformations that map the real axis to itself. One may then add any constant in the upper half-plane, and move the pole into the lower half-plane, giving new values for the parameters. Example: ${\displaystyle {\frac {iz+i-2}{z+1+i}}}$

• ${\displaystyle 1+i+z}$ and ${\displaystyle i+e^{iz}}$ are examples which are entire functions. The second is neither injective nor surjective.
• If S is a self-adjoint operator in a Hilbert space and f is an arbitrary vector, then the function

${\displaystyle \langle (S-z)^{-1}f,f\rangle }$

is a Nevanlinna function.

• If M(z) and N(z) are Nevanlinna functions, then the composition M(N(z)) is a Nevanlinna function as well.

• Vadim Adamyan, ed. (2009). Modern analysis and applications. p. 27. ISBN 3-7643-9918-X.
• Naum Ilyich Akhiezer and I. M. Glazman (1993). Theory of linear operators in Hilbert space. ISBN 0-486-67748-6.
• Marvin Rosenblum and James Rovnyak (1994). Topics in Hardy Classes and Univalent Functions. ISBN 3-7643-5111-X.