<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Complex Analysis on Nam Le</title><link>https://blog.namln.org/en/tags/complex-analysis/</link><description>Recent content in Complex Analysis on Nam Le</description><generator>Hugo</generator><language>en-US</language><lastBuildDate>Wed, 27 May 2026 00:00:00 +0000</lastBuildDate><atom:link href="https://blog.namln.org/en/tags/complex-analysis/index.xml" rel="self" type="application/rss+xml"/><item><title>Something Like Picard for 1-Forms</title><link>https://blog.namln.org/en/posts/something-like-picard-for-1-forms/</link><pubDate>Wed, 27 May 2026 00:00:00 +0000</pubDate><guid>https://blog.namln.org/en/posts/something-like-picard-for-1-forms/</guid><description>&lt;p&gt;Picard&amp;rsquo;s great theorem is a statement about how wildly a holomorphic function can
behave near an essential singularity. The conjecture below asks whether injectivity
of local primitives of a 1-form is enough to rule out such wild behaviour at the
origin, forcing the 1-form to extend meromorphically across the puncture.&lt;/p&gt;
&lt;div style="padding:10px 14px; border:2px solid dodgerblue; border-radius:6px; margin:16px 0;"&gt;
&lt;span style="color:dodgerblue; font-weight:bold;"&gt;Conjecture (Elsner, 2010)&lt;/span&gt;
&lt;p&gt;Let $D$ be the open unit disk and let $U_1,\dots,U_n$ be open sets with
$\bigcup_{j=1}^n U_j = D\setminus{0}$. Suppose there are injective holomorphic
functions $f_j : U_j \to \mathbb{C}$ such that
$$\mathrm{d}f_j = \mathrm{d}f_k \quad \text{on every connected component of } U_j \cap U_k.$$
Then the $\mathrm{d}f_j$ glue together to a &lt;strong&gt;meromorphic&lt;/strong&gt; 1-form on $D$.&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;The problem is rated &lt;em&gt;medium importance&lt;/em&gt; on the
&lt;a href="http://www.openproblemgarden.org/op/something_like_picard_for_1_forms"&gt;Open Problem Garden&lt;/a&gt;
and is not recommended for undergraduates, reflecting the depth of the tools involved.
It arises from Elsner&amp;rsquo;s study of hyperelliptic action integrals in the context of the
exact WKB method for Schrödinger equations with polynomial potential
(Elsner, &lt;em&gt;Ann. Inst. Fourier&lt;/em&gt; &lt;strong&gt;49&lt;/strong&gt;(1), 1999).&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="setup-and-interpretation"&gt;
 Setup and Interpretation&lt;span class="heading__anchor"&gt; &lt;a href="#setup-and-interpretation"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;The compatibility condition $\mathrm{d}f_j = \mathrm{d}f_k$ on each connected
component of $U_j \cap U_k$ is equivalent to saying $f_j - f_k$ is locally constant
there. The local differentials therefore glue together unambiguously to a global
holomorphic 1-form
$$\omega \in \Omega^1(D\setminus{0})$$
whose restriction to each $U_j$ equals $\mathrm{d}f_j$. The conjecture asserts that
$\omega$ does not have an essential singularity at the origin: it extends to a
meromorphic 1-form on all of $D$, meaning near $0$ it looks like
$$\omega = \left(\frac{c_{-m}}{z^m} + \cdots + \frac{c_{-1}}{z} + c_0 + c_1 z + \cdots\right)dz$$
for some $m \ge 0$.&lt;/p&gt;
&lt;p&gt;The injectivity of each $f_j$ is the crucial hypothesis. Without it the statement is
false: any holomorphic 1-form $\omega$ on $D\setminus{0}$ with an essential
singularity at $0$ is locally $\mathrm{d}f_j$ for some holomorphic $f_j$, and these
$f_j$ can be chosen on contractible pieces of the cover; injectivity is what
prohibits essential singularities from arising.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="what-is-already-known"&gt;
 What Is Already Known&lt;span class="heading__anchor"&gt; &lt;a href="#what-is-already-known"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;div style="padding:10px 14px; border:2px solid #27ae60; border-radius:6px; margin:16px 0;"&gt;
&lt;span style="color:#27ae60; font-weight:bold;"&gt;Partial Result&lt;/span&gt;
&lt;p&gt;Under the hypotheses of the conjecture:&lt;/p&gt;
&lt;ol&gt;
&lt;li&gt;The 1-form $\omega$ is holomorphic on $D\setminus{0}$.&lt;/li&gt;
&lt;li&gt;If the residue of $\omega$ at the origin vanishes, Picard&amp;rsquo;s big theorem can be
applied to conclude that $\omega$ extends meromorphically across $0$.&lt;/li&gt;
&lt;/ol&gt;
&lt;/div&gt;
&lt;p&gt;Point (1) is straightforward: each $\mathrm{d}f_j$ is holomorphic on $U_j$ and the
local forms agree on overlaps, so $\omega$ is holomorphic wherever it is defined,
i.e. on $D\setminus{0}$.&lt;/p&gt;
&lt;p&gt;Point (2) is the key partial result recorded by Elsner. If $\operatorname{Res}_0\omega = 0$,
then $\omega$ has trivial monodromy around the origin and admits a single-valued
holomorphic primitive $F$ on the punctured disk: $\omega = \mathrm{d}F$. The
injectivity of each local branch $f_j$ then forces $F$ itself to be injective on
some punctured neighbourhood of $0$ (since $f_j = F + c$ locally). An injective
holomorphic function on a punctured disk cannot have an essential singularity there,
and this is where Picard enters: at an essential singularity, by Picard&amp;rsquo;s big theorem,
every value is taken infinitely often in any punctured neighbourhood, contradicting
injectivity. Hence $F$ has at most a pole at $0$, and $\omega = \mathrm{d}F$ is meromorphic.&lt;/p&gt;
&lt;p&gt;The &lt;strong&gt;open case&lt;/strong&gt; is when $\operatorname{Res}_0\omega \ne 0$, so that $\omega$ has
non-trivial monodromy and no single-valued global primitive exists. The local
primitives $f_j$ then experience monodromy as one loops around the origin, and the
injectivity constraint must be leveraged in this more delicate multi-valued setting.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="connection-to-picards-theorem"&gt;
 Connection to Picard&amp;rsquo;s Theorem&lt;span class="heading__anchor"&gt; &lt;a href="#connection-to-picards-theorem"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;The title of the conjecture reflects a precise structural analogy.&lt;/p&gt;
&lt;div style="padding:10px 14px; border:2px solid #c0392b; border-radius:6px; margin:16px 0;"&gt;
&lt;span style="color:#c0392b; font-weight:bold;"&gt;Theorem (Picard's Great Theorem)&lt;/span&gt;
&lt;p&gt;If $f$ has an essential singularity at $z_0$, then in every punctured neighbourhood
of $z_0$ the function $f$ takes every value in $\mathbb{C}$, with at most one exception,
infinitely many times.&lt;/p&gt;
&lt;/div&gt;
&lt;p&gt;In particular, a function with an essential singularity is far from injective near
that point. The conjecture elevates this observation to the level of 1-forms: an
injective holomorphic primitive should preclude essential singularities in the
1-form itself, even when the primitive is only locally and multi-valuedly defined.&lt;/p&gt;
&lt;p&gt;Standard Picard covers the zero-residue case by reducing to a single-valued primitive.
The conjecture asks for an analogue that works when the monodromy is non-trivial, a
genuinely new statement about multi-valued functions and their differential geometry.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="origin-hyperelliptic-action-integrals"&gt;
 Origin: Hyperelliptic Action Integrals&lt;span class="heading__anchor"&gt; &lt;a href="#origin-hyperelliptic-action-integrals"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;p&gt;The problem arises from the &lt;em&gt;exact WKB method&lt;/em&gt; applied to the stationary
Schrödinger equation $-\psi&amp;rsquo;&amp;rsquo; + V(x)\psi = E\psi$ with polynomial potential $V$.
The formal WKB ansatz $\psi \sim e^{S/\hbar}$ produces a multivalued &lt;em&gt;action integral&lt;/em&gt;
$$\mathcal{I}(E) = \int_\gamma \sqrt{V(x) - E}\mathrm{d}x$$
defined on a hyperelliptic Riemann surface whose branch structure depends on the
energy parameter $E$. Elsner&amp;rsquo;s 1999 paper constructs the Riemann surface of
$\mathcal{I}$ explicitly and shows its branch points accumulate densely in the
value plane, a phenomenon that obstructs Borel–Laplace resummation of the
WKB symbols.&lt;/p&gt;
&lt;p&gt;In this setting the local inverses of $\mathcal{I}$ play the role of the $f_j$: they
are locally injective holomorphic functions whose differentials agree on overlaps.
The conjecture asks whether the obstruction to global meromorphic extension can
arise only from a pole, a controlled singularity, rather than an essential one.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="research-directions"&gt;
 Research Directions&lt;span class="heading__anchor"&gt; &lt;a href="#research-directions"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;h3 class="heading" id="1-the-non-zero-residue-case"&gt;
 1. The Non-Zero Residue Case&lt;span class="heading__anchor"&gt; &lt;a href="#1-the-non-zero-residue-case"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h3&gt;&lt;p&gt;The open heart of the problem is the case $\operatorname{Res}_0\omega \ne 0$. Here
$\omega$ is not exact near $0$, the monodromy of the primitive is a non-trivial
translation $f_j \mapsto f_j + 2\pi i, \operatorname{Res}_0\omega$, and no single
injective function encompasses the full behaviour near the singularity.&lt;/p&gt;
&lt;p&gt;A natural approach is to pass to a cyclic cover $\tilde D \to D$ that trivialises the
monodromy, construct a single-valued primitive on $\tilde D\setminus{0}$, and
then appeal to the zero-residue argument there. The key difficulty is that the
injectivity of each $f_j$ on $U_j$ does not immediately imply injectivity of the
lifted primitive on $\tilde D$, since different sheets can collide. Making this
argument precise, or finding a counterexample, is the main open problem.&lt;/p&gt;
&lt;h3 class="heading" id="2-quantitative-control-via-nevanlinna-theory"&gt;
 2. Quantitative Control via Nevanlinna Theory&lt;span class="heading__anchor"&gt; &lt;a href="#2-quantitative-control-via-nevanlinna-theory"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h3&gt;&lt;p&gt;An alternative strategy replaces Picard&amp;rsquo;s theorem by its quantitative form. If $F$ is
a meromorphic function on the punctured disk with an essential singularity, the
Nevanlinna characteristic $T(r,F)$ grows faster than any power of $\log(1/r)$ as
$r\to 0$. For an injective function the counting functions $N(r,a,F)$, recording
how often $F = a$ in the punctured disk, satisfy strong constraints.&lt;/p&gt;
&lt;p&gt;Nevanlinna-theoretic methods might give a direct bound on $T(r,f_j)$ in terms of the
geometry of the cover ${U_j}$ and the injectivity of $f_j$, ruling out essential
singularities of $\omega$ without passing through the monodromy argument. This would
require adapting the standard Nevanlinna machinery to functions that are only locally
defined on an open cover.&lt;/p&gt;
&lt;h3 class="heading" id="3-replacing-injectivity-by-finite-valence"&gt;
 3. Replacing Injectivity by Finite Valence&lt;span class="heading__anchor"&gt; &lt;a href="#3-replacing-injectivity-by-finite-valence"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h3&gt;&lt;p&gt;One can ask whether the conjecture remains true if &amp;ldquo;injective&amp;rdquo; is weakened to
&amp;ldquo;at most $d$-to-one&amp;rdquo; for some fixed integer $d$. Finite-valence holomorphic functions
cannot have essential singularities either, by a Picard-type argument (a function of
valence at most $d$ takes each value at most $d$ times, so in any neighbourhood of an
essential singularity it must omit a set of positive capacity, contradicting Picard).&lt;/p&gt;
&lt;p&gt;If the conjecture extends to finite valence, the proof strategy will likely yield a
valence-independent argument that illuminates the zero-residue case more transparently.
If it fails for finite valence, the counterexample geometry would clarify what role
injectivity plays beyond the mere avoidance of essential singularities.&lt;/p&gt;
&lt;h3 class="heading" id="4-several-complex-variables"&gt;
 4. Several Complex Variables&lt;span class="heading__anchor"&gt; &lt;a href="#4-several-complex-variables"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h3&gt;&lt;p&gt;In $\mathbb{C}^n$ for $n \ge 2$ the theory of isolated singularities of holomorphic
functions changes dramatically: by Hartogs&amp;rsquo; extension theorem, isolated singularities
of holomorphic functions are always removable. One would expect the analogous
conjecture for holomorphic 1-forms in $\mathbb{C}^n$ to be more tractable, or even to
follow from known extension results.&lt;/p&gt;
&lt;p&gt;Formulating the precise analogue, replacing the punctured disk by a domain
$\Omega\setminus{0}$ in $\mathbb{C}^n$, and specifying what &amp;ldquo;meromorphic 1-form&amp;rdquo;
means on a higher-dimensional domain, and checking whether Hartogs-type arguments
already resolve it would clarify which features of the problem are genuinely
one-dimensional.&lt;/p&gt;
&lt;h3 class="heading" id="5-geometric-formulation-on-riemann-surfaces"&gt;
 5. Geometric Formulation on Riemann Surfaces&lt;span class="heading__anchor"&gt; &lt;a href="#5-geometric-formulation-on-riemann-surfaces"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h3&gt;&lt;p&gt;The disk $D$ and the puncture at $0$ are not special: the same question can be posed
on any Riemann surface $X$ with a marked point $p$. Given an open cover of
$X\setminus{p}$ and injective holomorphic functions $f_j$ on each piece with
compatible differentials, does $\omega = \mathrm{d}f_j$ extend meromorphically
across $p$?&lt;/p&gt;
&lt;p&gt;The answer may depend on the genus and the function theory of $X$. For the disk
(simply connected, genus 0) the monodromy is a simple translation; for a torus or
higher-genus surface the monodromy group is richer and the argument structure should
change. Comparing these cases may isolate the essential input from the topology versus
the analysis.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 class="heading" id="references"&gt;
 References&lt;span class="heading__anchor"&gt; &lt;a href="#references"&gt;#&lt;/a&gt;&lt;/span&gt;
&lt;/h2&gt;&lt;ol&gt;
&lt;li&gt;Elsner, B. (1999). Hyperelliptic action integral. &lt;em&gt;Annales de l&amp;rsquo;Institut Fourier&lt;/em&gt;, &lt;strong&gt;49&lt;/strong&gt;(1), 303–331. &lt;a href="https://www.numdam.org/item/AIF_1999__49_1_303_0/"&gt;https://www.numdam.org/item/AIF_1999__49_1_303_0/&lt;/a&gt;&lt;/li&gt;
&lt;li&gt;Ahlfors, L. V. (1979). &lt;em&gt;Complex Analysis&lt;/em&gt; (3rd ed.). McGraw-Hill.&lt;/li&gt;
&lt;li&gt;Conway, J. B. (1978). &lt;em&gt;Functions of One Complex Variable&lt;/em&gt; (2nd ed.). Springer.&lt;/li&gt;
&lt;li&gt;Nevanlinna, R. (1970). &lt;em&gt;Analytic Functions&lt;/em&gt;. Springer.&lt;/li&gt;
&lt;li&gt;Forster, O. (1981). &lt;em&gt;Lectures on Riemann Surfaces&lt;/em&gt;. Springer.&lt;/li&gt;
&lt;li&gt;Delabaere, E., Dillinger, H., &amp;amp; Pham, F. (1993). Résurgence de Voros et périodes des courbes hyperelliptiques. &lt;em&gt;Annales de l&amp;rsquo;Institut Fourier&lt;/em&gt;, &lt;strong&gt;43&lt;/strong&gt;(1), 163–199.&lt;/li&gt;
&lt;/ol&gt;</description></item><item><title>Collected Lectures on Complex Analysis</title><link>https://blog.namln.org/en/mathematics/analysis/complex-analysis/collected-lectures-ca/</link><pubDate>Mon, 07 Jul 2025 00:00:00 +0000</pubDate><guid>https://blog.namln.org/en/mathematics/analysis/complex-analysis/collected-lectures-ca/</guid><description>&lt;ul&gt;
&lt;li&gt;📝 &lt;a href="https://mtaylor.web.unc.edu/wp-content/uploads/sites/16915/2018/04/complex.pdf"&gt;Introduction to Complex Analysis&lt;/a&gt; - Michael Taylor&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="http://www.math.uiuc.edu/~jpda/jpd-complex-geometry-book-5-refs-bip.pdf"&gt;An Introduction to Complex Analysis and Geometry&lt;/a&gt; - John P. D&amp;rsquo;Angelo (University of Illinois)&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="http://math.sfsu.edu/beck/papers/complex.pdf"&gt;A First Course in Complex Analysis&lt;/a&gt; - Matthias Beck, Gerald Marchesi, Dennis Pixton, Lucas Sabalka&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="http://www.math.wustl.edu/~sk/books/guide.pdf"&gt;A Guide to Complex Variables&lt;/a&gt; - Steven G. Krantz&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="http://www.maths.manchester.ac.uk/~cwalkden/complex-analysis/complex_analysis.pdf"&gt;Complex Analysis&lt;/a&gt; - Charles Walkden&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="http://www.math.ku.dk/noter/filer/koman-12.pdf"&gt;Complex Analysis&lt;/a&gt; - Christian Berg&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="http://people.math.sc.edu/girardi/m7034/book/AshComplexVariablesWithHyperlinks.pdf"&gt;Complex Variables&lt;/a&gt; - R. B. Ash, W.P. Novinger&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="http://www.maths.lth.se/matematiklu/personal/olofsson/CompHT06.pdf"&gt;Complex Analysis&lt;/a&gt; - Christer Bennewitz&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="https://web.archive.org/web/20150620124453/https://www.math.washington.edu/~marshall/math_536/Notes.pdf"&gt;Complex Analysis&lt;/a&gt; - Donald E. Marshall&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="https://gauss.math.yale.edu/~ws442/complex.pdf"&gt;A Concise Course in Complex Analysis and Riemann Surfaces&lt;/a&gt; - Wilhelm Schlag&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="http://people.math.gatech.edu/%7Ecain/winter99/complex.html"&gt;Complex Analysis&lt;/a&gt; - G. Cain (Georgia Tech)&lt;/li&gt;
&lt;li&gt;📝 &lt;a href="https://complex-analysis.com/"&gt;Complex Analysis&lt;/a&gt; - Juan Carlos Ponce Campuzano&lt;/li&gt;
&lt;/ul&gt;</description></item><item><title>Mathematics - Complex Analysis</title><link>https://blog.namln.org/en/mathematics/analysis/complex-analysis/</link><pubDate>Thu, 27 Jun 2024 23:14:15 +0800</pubDate><guid>https://blog.namln.org/en/mathematics/analysis/complex-analysis/</guid><description/></item></channel></rss>