Erdős Problem #1116
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For a meromorphic function, let $n(r,a)$ count solutions of $f(z)=a$ in $|z|<r$, with multiplicity; $n(r,\infty)$ counts poles. We construct a meromorphic function for which \[ \limsup_{r\to\infty}\frac{n(r,a)}{n(r,b)}=\infty \qquad(a\ne b,\ a,b\in\widehat{\mathbb C}). \] This answers the meromorphic alternative, even including the value $\infty$. Toppila proved this and the stronger entire-function version for finite values. The construction below reconstructs the separated zero--pole cluster mechanism; no novelty is claimed. It does not reconstruct the entire-function refinement.
Restatement from Math-6170-A1 r1, with the source manuscript’s qualifications.
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GPT 6 Astra Ultra attempt on Math-6170
Erdős Problem 1116: separating every pair of value counts
Statement and scope
For a meromorphic function, let $n(r,a)$ count solutions of $f(z)=a$ in $|z|<r$, with multiplicity; $n(r,\infty)$ counts poles. We construct a meromorphic function for which \[ \limsup_{r\to\infty}\frac{n(r,a)}{n(r,b)}=\infty \qquad(a\ne b,\ a,b\in\widehat{\mathbb C}). \] This answers the meromorphic alternative, even including the value $\infty$. Toppila proved this and the stronger entire-function version for finite values. The construction below reconstructs the separated zero--pole cluster mechanism; no novelty is claimed. It does not reconstruct the entire-function refinement.Normalized clusters
Choose positive integers \[ t_n\ge n^2\left(1+\sum_{j<n}t_j\right), \] and a sequence of angles $\theta_n$ which visits every open arc infinitely often. For large radii $R_n$, to be chosen inductively, set \[ \phi_{nk}=\frac{k}{n^2t_n},\qquad a_{nk}=R_ne^{i\phi_{nk}}\quad(1\le k\le t_n). \] All zeros in the $n$th cluster thus have exactly the same modulus, but are mutually far apart when $R_n$ is large. Define \[ B_n(z)=\prod_{k=1}^{t_n} \frac{1-z/a_{nk}}{1-z/(a_{nk}+\delta_n)},\qquad F_n(z)=z\prod_{j\le n}B_j(z), \] where $|\delta_n|=1$. If $F_{n-1}$ is already chosen, write \[ A_n=\lim_{z\to\infty}\frac{F_{n-1}(z)}z =\prod_{\substack{j<n\\k\le t_j}}\left(1+\frac{\delta_j}{a_{jk}}\right), \qquad \delta_n=e^{i(\theta_n+\arg A_n)}. \] Require $R_n>10R_{n-1}$, $R_n>10$, and $t_n/R_n\le2^{-n}/100$. The estimate $|\log(1+w)|\le2|w|$ for $|w|\le1/2$ shows that $A_n$ converges to a nonzero $A$ and \[ 0.9<|A_n|<1.1. \tag{1} \] None of the specified zeros or poles cancel: within a cluster the anchor separation can exceed ten, and different clusters occupy disjoint annuli.The local estimates that choose the radii
Here $n,t_n,F_{n-1},\delta_n$ are fixed while $R=R_n\to\infty$. Uniformly on $R/2\le|z|\le2R$, $F_{n-1}(z)/z\to A_n$. For $z=a_{nk}+u/R$ with $|u|\le100n$, the $k$th factor is \[ \left(1+\frac{\delta_n}{a_{nk}}\right) \frac{-u/R}{\delta_n-u/R}, \] and all the other factors tend uniformly to one. Consequently, uniformly in $k$ and this $u$-disk, \[ F_n(a_{nk}+u/R) =-\frac{A_ne^{i\phi_{nk}}}{\delta_n}u+o(1). \tag{2} \] There are only finitely many anchors at this stage, so all these estimates can be imposed simultaneously.We also claim, after increasing $R$, \[ |F_n(z)|>2n \quad\text{on }R/2\le|z|\le2R \text{ outside }\bigcup_k\{|z-a_{nk}|<100n/R\}. \tag{3} \] At a pole the assertion means infinite modulus. To verify it, first consider the disks $|z-a_{nk}|\le2$. All factors other than the $k$th tend uniformly to one there, while \[ \left|\frac{a_{nk}-z}{a_{nk}+\delta_n-z}\right| \ge\frac{|z-a_{nk}|}{3}. \] Also $|F_{n-1}(z)|=(|A_n|+o(1))R$ there. This proves $3$ in those disks, outside the smaller disks. Elsewhere choose a nearest anchor. Its unnormalized factor has modulus at least $2/3$, and all other factors tend uniformly to one because the anchor separations tend to infinity. The normalizing factors tend to one too. Thus the whole product has modulus at least $1/2$, and $|F_{n-1}(z)|\ge(0.9-o(1))R/2$, which proves $3$.
Choose $R_n$ so that the error in $2$ is less than $1/(10n)$ and $3$ holds. Rouché's theorem then says that for every $|w|\le n$ there is exactly one $w$-point, counted with multiplicity, in each disk \[ D_{nk}=\{|z-a_{nk}|<100n/R_n\}. \] On the inner circle $|z|=R_n/2$, $3$ permits a homotopy from $F_n-w$ to $F_n$. The argument principle gives exactly \[ N_{n-1}=1+\sum_{j<n}t_j \tag{4} \] $w$-points inside that circle, since precisely the earlier zeros and poles lie there.
Preserving the estimates in the infinite product
For any fixed compact disk, the normalized factors satisfy \[ \log B_n(z)=O(t_n|z|/R_n^2)\qquad(R_n\to\infty). \tag{5} \] At each stage there are only finitely many earlier annuli to protect. We therefore further enlarge $R_n$ to make the logarithm of $B_n$ uniformly as small as desired on all of them and on $|z|\le n$.More explicitly, after stage $j$ choose $\eta_j>0$ so small that multiplication by any analytic, zero-free factor with $|\log h|<\eta_j$ on $|z|\le2R_j$ preserves $3$ with lower bound $j$, preserves the Rouché inequalities on the small and inner circles, and makes the error in $2$ at most $1/j$. Such a choice exists by the strict margins, compactness of $|w|\le j$, and the bounded values of $F_j$ on the small disks. For every later stage $n>j$ impose \[ \sup_{|z|\le2R_j}|\log B_n(z)|<2^{-n}\eta_j. \] These are finitely many conditions at stage $n$, all attainable by $5$. Also impose $|\log B_n(z)|<2^{-n}$ on $|z|\le n$.
It follows that \[ f(z)=z\prod_{n\ge1}B_n(z) \] converges locally uniformly away from its specified poles to a meromorphic function. The tails are zero-free; its zeros and poles are exactly those specified. All the counting conclusions $3$--$4$ hold for $f$, with the relaxed bound $n$, and its unique $w$-point in $D_{nk}$ satisfies, uniformly for $|w|\le n$, \[ R_n(z_{nk}(w)-a_{nk}) =-\frac{\delta_n w}{A_ne^{i\phi_{nk}}}+O(1/n). \tag{6} \] The constants in this error can be absolute by $1$. This diagonal choice is essential: uniform convergence on each fixed disk alone would not guarantee the later annular counting assertions.
Every ordered pair of finite values
For fixed $w$, expanding the modulus in $6$ gives, uniformly in $k$, \[ \begin{split} R_n\left(|z_{nk}(w)|-R_n\right) &=-\frac{\operatorname{Re}(e^{i\theta_n}e^{-2i\phi_{nk}}w)} {|A_n|}+O(1/n)\\ &=-\frac{\operatorname{Re}(e^{i\theta_n}w)}{|A_n|}+o(1). \end{split} \tag{7} \] Here $\max_k|\phi_{nk}|\le1/n^2$, and $R_n$ may be enlarged to absorb the elementary quadratic error in the modulus expansion.Fix distinct finite $a,b$. Infinitely many $n$ satisfy $\operatorname{Re}(e^{i\theta_n}(a-b))>\varepsilon$ for some fixed $\varepsilon>0$. For all sufficiently large such $n$, $7$ puts every new $a$-point strictly inside every new $b$-point in radial order. Choose $r$ strictly between their moduli. There are no other $a$- or $b$-points in this annulus, so \[ n(r,a)=N_{n-1}+t_n,\qquad n(r,b)=N_{n-1}. \] Their ratio is at least $1+n^2$. The selected radii tend to infinity. The ordered choice of $a,b$ was arbitrary, so the assertion also holds with the two values reversed.
Pairs involving infinity
The new poles have moduli \[ |a_{nk}+\delta_n| =R_n+\operatorname{Re}(\delta_ne^{-i\phi_{nk}})+O(1/R_n). \] Because $A_n\to A\ne0$ and $\theta_n$ visits every arc infinitely often, infinitely many $n$ have $\operatorname{Re}\delta_n>3/4$, and infinitely many have $\operatorname{Re}\delta_n<-3/4$. For each fixed finite $w$, $6$ places all its new points at distance $o(1)$ in modulus from $R_n$.In the first subsequence, choose $r=R_n+1/4$. It includes the $t_n$ new $w$-points and no new poles. Thus \[ \frac{n(r,w)}{n(r,\infty)} \ge\frac{t_n}{\sum_{j<n}t_j}\longrightarrow\infty. \] In the second subsequence choose $r=R_n-1/4$. It includes all new poles and none of the new $w$-points, giving \[ \frac{n(r,\infty)}{n(r,w)} \ge\frac{t_n}{N_{n-1}}\ge n^2. \] All denominators are positive for sufficiently large $n$. This completes the meromorphic construction for every ordered pair on the sphere.