SearcharxivSearch

arXiv subjects

Genevra Neumann

Publications and source records attributed to Genevra Neumann.

3 recordsLinked to original sources

Cluster points and asymptotic values of planar harmonic functions

A sufficient condition for a cluster point of a planar harmonic function to be an asymptotic value is given, based on a partitioning into regions of constant valence. A sufficient condition for the cluster set of a planar harmonic function to have non-empty interior is given. An example is given of a planar harmonic function where the image of the critical set is not closed and such that the cluster set has non-empty interior and is a proper subset of the image.

math.CV

On the number of zeros of certain rational harmonic functions

Extending a result from the paper of D. Khavinson and G. Swiatek, we show that the rational harmonic function $\bar{r(z)} - z$, where r(z) is a rational function of degree n > 1, has no more than 5n - 5 complex zeros. Applications to gravitational lensing are discussed. In particular, this result settles a conjecture of S. H. Rhie concerning the maximum number of lensed images due to an n-point gravitational lens.

math.CV

Valence of complex-valued planar harmonic functions

The valence of a function $f$ at a point $w$ is the number of distinct, finite solutions to $f(z) = w$. Let $f$ be a complex-valued harmonic function in an open set $R \subseteq \mathbb{C}$. Let $S$ denote the critical set of $f$ and $C(f)$ the global cluster set of $f$. We show that $f(S) \cup C(f)$ partitions the complex plane into regions of constant valence. We give some conditions such that $f(S) \cup C(f)$ has empty interior. We also show that a component $R_0 \subseteq R \backslash f^{-1}(f(S) \cup C(f))$ is a $n_0$-fold covering of some component $Ω_0 \subseteq \mathbb{C} \backslash (f(S) \cup C(f))$. If $Ω_0$ is simply connected, then $f$ is univalent on $R_0$. We explore conditions for combining adjacent components to form a larger region of univalence. Those results which hold for $C^1$ functions on open sets in $\mathbb{R}^2$ are first stated in that form and then applied to the case of planar harmonic functions. If $f$ is a light, harmonic function in the complex plane, we apply a structure theorem of Lyzzaik to gain information about the difference in valence between components of $\mathbb{C} \backslash (f(S) \cup C(f))$ sharing a common boundary arc in $f(S) \backslash C(f)$.

math.CV