How to use this course
Gösta Mittag-Leffler is known to every student of complex analysis for one theorem: a meromorphic function can be built with poles and principal parts prescribed at will. To historians he is better known as an organizer. He founded Acta Mathematica in 1882 and made it, within a decade, one of the leading journals in the world. He published Georg Cantor when Berlin would not, launched Henri Poincaré’s work on Fuchsian functions, arranged the King Oscar prize that produced Poincaré’s memoir on the three-body problem, and secured for Sofia Kovalevskaya the first full professorship of mathematics held by a woman in modern Europe. His villa at Djursholm became the Institut Mittag-Leffler, still a leading research institute.
- A first course in complex analysis: power series, Laurent series, residues, Liouville’s theorem.
- Uniform convergence and basic point-set topology of the plane.
- For Lesson 08, the Gamma function; for Lesson 09, partial derivatives in several variables; for Lesson 10, groups and exact sequences.
Each technical lesson opens with a paragraph for the general reader, then gives precise statements, proof sketches and exercises with folded solutions. Lessons 04–06 follow the theorem from Weierstrass’s products to its general form of 1884. Lessons 07–08 treat his later work on analytic continuation and summation. Lessons 09–10 follow two ideas descended from his theorem into twentieth-century mathematics.
Timeline
| 1846 | Born Gösta Leffler in Stockholm, 16 March, eldest child of the schoolteacher Johan Olof Leffler and Gustava Wilhelmina Mittag. |
| c. 1866 | Adds his mother’s surname to his own. |
| 1865 | Enters Uppsala University. |
| 1872 | Doctorate at Uppsala under Göran Dillner, on separating the roots of an analytic function; appointed docent. |
| 1873 | October: arrives in Paris on a travel scholarship and attends Charles Hermite’s lectures. |
| 1873–76 | Studies in Paris, Göttingen and Berlin, where the lectures of Karl Weierstrass shape all his later work. |
| 1876 | Visits Sofia Kovalevskaya in St Petersburg. First notes on the theorem on prescribed poles, in Swedish. |
| 1877 | Professor of mathematics at the University of Helsinki (Helsingfors), succeeding Lorenz Lindelöf. |
| 1881 | First professor of mathematics at the new Stockholm University College (Stockholms högskola). |
| 1882 | Marries Signe Lindfors, from a wealthy Finnish family. Founds Acta Mathematica; volume 1 opens with Poincaré’s Théorie des groupes fuchsiens. |
| 1883 | Member of the Royal Swedish Academy of Sciences. Publishes French translations of Cantor’s papers on set theory. Kovalevskaya arrives in Stockholm late in the year. |
| 1884 | General form of his theorem, Sur la représentation analytique des fonctions monogènes uniformes, in Acta 4. Kovalevskaya appointed professor for five years. |
| 1885 | Announces in Acta the prize competition for the sixtieth birthday of King Oscar II. |
| 1889 | 21 January: the prize goes to Poincaré. Kovalevskaya appointed professor for life. Buys land at Djursholm. |
| 1890 | Poincaré’s corrected memoir on the three-body problem fills Acta 13. |
| 1891 | Kovalevskaya dies, 10 February. The Djursholm villa is completed. |
| 1896 | Foreign member of the Royal Society of London. |
| 1899–1905 | Five notes in Acta on the analytic representation of a branch of a monogenic function: the star. |
| 1903 | Introduces the function \(E_\alpha\). Alerts Pierre Curie that the Nobel nomination omits Marie Curie. |
| 1911 | Retires from his chair; continues to edit Acta. |
| 1916 | On his seventieth birthday, he and Signe make public the will that leaves their villa, library and fortune to a mathematical foundation: the Institut Mittag-Leffler. |
| 1921 | Signe Mittag-Leffler dies. |
| 1922 | Financial losses bring him close to bankruptcy. |
| 1927 | Dies at Djursholm, 7 July, aged 81. |
Stockholm and Uppsala, 1846–1873
Gösta Leffler was born in Stockholm on 16 March 1846. His father, Johan Olof Leffler, was a schoolteacher who became headmaster of a Stockholm school and sat in the Swedish parliament. His mother was Gustava Wilhelmina Mittag. Gösta was the eldest of four children, and all of them made names for themselves. His sister Anne Charlotte Leffler became a well-known writer, his brother Frits a linguist, and his brother Artur a civil engineer. At about twenty Gösta added his mother’s surname to his own, and became Mittag-Leffler.
He entered Uppsala University in 1865, supporting himself in part by private tutoring, and at first trained in actuarial work before settling on mathematics. In 1870 his father fell ill, and the family’s finances became tighter. In 1872 he took his doctorate at Uppsala with a thesis, written under Göran Dillner, on separating the roots of an analytic function of one variable, an application of the argument principle. His biographers have not rated it highly. He was made docent at Uppsala the same year.
Swedish mathematics was then provincial, and Mittag-Leffler knew it. In 1873 he won a travel scholarship, the Byzantine stipend, which allowed him three years abroad. He went first to Paris.
Paris and Berlin, 1873–1876
He arrived in Paris in October 1873 to learn from Charles Hermite. He found Hermite’s lectures hard to follow but formed a lasting friendship with him, and met Jean-Claude Bouquet, Charles Briot, Michel Chasles, Gaston Darboux and Joseph Liouville. Hermite told him, again and again, that the master of analysis was in Berlin, and that he should go to Weierstrass. After a stay in Göttingen, Mittag-Leffler went to Berlin.
Weierstrass’s lectures on the theory of analytic functions changed his mathematics for good. Weierstrass built function theory on power series and analytic continuation, with a rigour unknown elsewhere, and in 1876 he published his theorem on entire functions with prescribed zeros (Lesson 04). Mittag-Leffler set himself the matching problem for poles. He also came to know Leopold Kronecker, and he absorbed the Berlin standard of proof.
In Berlin he heard from Weierstrass about his former private student Sofia Kovalevskaya, then living in Russia and outside mathematics. In 1876 Mittag-Leffler visited her in St Petersburg and was deeply impressed. The friendship that began there would bring her to Stockholm seven years later.
Helsinki, 1877–1881
In 1877 Mittag-Leffler won the competition for the chair of mathematics at the University of Helsinki, then the Imperial Alexander University of the Grand Duchy of Finland, succeeding Lorenz Lindelöf. There he developed his theorem on meromorphic functions in a series of notes, and he trained his first doctoral students, among them Hjalmar Mellin, later known for the Mellin transform, who took his degree in Helsinki in 1882.
In Helsinki he also met Signe Lindfors, daughter of a wealthy Finnish family; they married in 1882. Her fortune would support his projects for the rest of his life.
Meanwhile Stockholm was building a new kind of institution. Stockholms högskola, a private university college supported by donors, opened in 1878 with the aim of research and public lectures, free of the old universities’ regulations. Mittag-Leffler was appointed its first professor of mathematics in 1881. He resigned from Helsinki and came home with two projects: an international journal and a research school in Stockholm.
Weierstrass products
For the general reader. A polynomial is determined, up to a constant, by its roots. Can we build a function with infinitely many prescribed zeros? Simply multiplying the factors \((1-z/a_n)\) usually fails, because the infinite product diverges. Weierstrass found convergence factors that tame the product without adding new zeros. Mittag-Leffler’s theorem is the analogue for poles, and its proof copies Weierstrass’s idea.
- Define Weierstrass’s elementary factors and estimate them.
- Prove the Weierstrass product theorem.
- Recognize the shared pattern: a divergent sum or product, corrected term by term.
Elementary factors
For an integer \(p\ge0\) define
\[ E_0(z)=1-z,\qquad E_p(z)=(1-z)\exp\Big(z+\frac{z^2}{2}+\cdots+\frac{z^p}{p}\Big). \]The exponential cancels the first \(p\) terms of \(\log(1-z)=-\sum_k z^k/k\), so \(E_p(z)\) is close to 1 when \(|z|\) is small.
For \(|z|\le1\) and \(p\ge0\), \(\ |1-E_p(z)|\le|z|^{p+1}\).
Let \((a_n)\) be a sequence of non-zero complex numbers with \(|a_n|\to\infty\), repetitions allowed, and let \(m\ge0\). Then
\[ f(z)=z^m\prod_{n=1}^{\infty}E_{n-1}\Big(\frac{z}{a_n}\Big) \]converges uniformly on compact sets to an entire function whose zeros are exactly 0 (order \(m\)) and the \(a_n\), with multiplicity. Every entire function with these zeros is \(f\,e^{g}\) with \(g\) entire.
Proof. Fix \(R>0\). For all but finitely many \(n\), \(|a_n|\ge2R\), and then for \(|z|\le R\) the lemma gives \(|1-E_{n-1}(z/a_n)|\le2^{-n}\). A product \(\prod(1+u_n)\) with \(\sum|u_n|\) uniformly convergent converges uniformly, and it vanishes only where a factor does. The last claim follows because the quotient of two entire functions with the same zeros is entire and zero-free, hence of the form \(e^g\) on the simply connected plane.
Exercise 4.1Prove the lemma.
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Exercise 4.2Show that \(\prod_{n\ge1}(1-z/n)\) diverges for every \(z\notin\{0,1,2,\dots\}\), but that \(\prod_{n\ge1}(1-z/n)e^{z/n}\) converges to an entire function with zeros at the positive integers.
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The Mittag-Leffler theorem in the plane
For the general reader. A rational function can be written as a sum of simple fractions, one for each pole. Mittag-Leffler showed that the same is true for functions with infinitely many poles, once each fraction is corrected by a polynomial so that the infinite sum converges. Any list of poles going off to infinity, with any prescribed singular behaviour at each, belongs to some function. Classical formulas such as the partial-fraction expansion of the cotangent become special cases.
- State and prove the theorem for the whole plane.
- Derive the expansion of \(\pi\cot\pi z\) and evaluate \(\sum1/n^2\).
- Check convergence of the Weierstrass \(\wp\)-function.
A principal part at a point \(a\) is a polynomial in \(1/(z-a)\) without constant term, \(P\big(\tfrac{1}{z-a}\big)=\sum_{k=1}^{N}\frac{c_k}{(z-a)^k}\).
Let \(a_1,a_2,\dots\) be distinct complex numbers with \(|a_n|\to\infty\), and for each \(n\) let \(P_n\big(\tfrac{1}{z-a_n}\big)\) be a principal part. Then there are polynomials \(T_n\) such that
\[ f(z)=\sum_{n=1}^{\infty}\Big[P_n\Big(\frac{1}{z-a_n}\Big)-T_n(z)\Big] \]converges uniformly on compact sets away from the \(a_n\). The function \(f\) is meromorphic in \(\mathbb C\), with poles exactly at the \(a_n\) and principal part \(P_n\) at \(a_n\). Every meromorphic function with these poles and principal parts is \(f+g\) with \(g\) entire.
Proof. If some \(a_n=0\), keep that term without correction. For \(a_n\ne0\), the function \(P_n\big(\tfrac{1}{z-a_n}\big)\) is holomorphic in \(|z|<|a_n|\), so its Taylor series at 0 converges uniformly on \(|z|\le|a_n|/2\). Let \(T_n\) be a partial sum with \(\big|P_n\big(\tfrac{1}{z-a_n}\big)-T_n(z)\big|<2^{-n}\) there. On a disc \(|z|\le R\), all but finitely many \(n\) have \(|a_n|/2\ge R\), so the tail of the series is dominated by \(\sum2^{-n}\), and it converges uniformly to a holomorphic function. The finitely many remaining terms supply the poles. The difference of two solutions has no poles, so it is entire.
The cotangent
The function \(\pi\cot\pi z\) has simple poles of residue 1 at every integer. The principal parts \(\frac{1}{z-n}\) need only the constant correction \(T_n=-\frac1n\):
\[ \pi\cot\pi z=\frac1z+\sum_{n\ne0}\Big(\frac{1}{z-n}+\frac1n\Big)=\frac1z+\sum_{n=1}^{\infty}\frac{2z}{z^2-n^2}. \]To prove equality, call the difference \(g\). It is entire, and differentiating gives \(g'(z)=-\frac{\pi^2}{\sin^2\pi z}+\sum_{n\in\mathbb Z}\frac{1}{(z-n)^2}\). This is entire, periodic with period 1, and bounded as \(|\operatorname{Im}z|\to\infty\) (both terms tend to 0), so by Liouville’s theorem it is a constant, which must be 0. Thus \(g\) is constant, and since \(g\) is odd, \(g=0\).
Exercise 5.1From \(\dfrac{\pi^2}{\sin^2\pi z}=\sum_{n\in\mathbb Z}\dfrac{1}{(z-n)^2}\), deduce \(\sum_{n\ge1}\dfrac{1}{n^2}=\dfrac{\pi^2}{6}\).
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Exercise 5.2Let \(\Lambda=\mathbb Z\omega_1+\mathbb Z\omega_2\) be a lattice. Show that \(\wp(z)=\dfrac1{z^2}+\sum_{\omega\in\Lambda\setminus0}\Big(\dfrac{1}{(z-\omega)^2}-\dfrac{1}{\omega^2}\Big)\) converges uniformly on compact sets away from \(\Lambda\). Why is the correction \(-1/\omega^2\) needed?
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Exercise 5.3Construct a meromorphic function with a simple pole of residue 1 at each positive integer and no other poles.
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Arbitrary open sets and Cantor’s point sets
For the general reader. Mittag-Leffler wanted his theorem not only for the whole plane but for any region, where poles may pile up at the boundary instead of at infinity. To describe how a set of points can accumulate, he used the new language of Georg Cantor’s set theory, at a time when most mathematicians regarded it with suspicion. His 1884 memoir in Acta Mathematica was one of the first places where Cantor’s ideas did real work in analysis.
- State the theorem for an arbitrary open set.
- See how Runge’s approximation theorem lets the correcting functions have poles on the boundary.
- Construct explicit examples with poles accumulating at a boundary point.
Let \(\Omega\subseteq\mathbb C\) be open, let \(A\subset\Omega\) be a set with no limit point in \(\Omega\), and for each \(a\in A\) let \(P_a\big(\frac1{z-a}\big)\) be a principal part. Then there is a function \(f\) meromorphic in \(\Omega\) whose poles are exactly the points of \(A\), with principal part \(P_a\) at each \(a\).
In Mittag-Leffler’s formulation, one starts with a set \(Q\) of isolated points in the extended plane and its set of limit points \(Q'\), which Cantor called the derived set. Any prescribed principal parts at the points of \(Q\) belong to a single-valued function that is meromorphic on the complement of \(Q'\). Taking \(Q'=\partial\Omega\) recovers the modern statement.
Proof sketch
Exhaust \(\Omega\) by compact sets \(K_1\subset K_2\subset\cdots\), each in the interior of the next, such that every bounded component of \(\mathbb C\setminus K_n\) contains a point outside \(\Omega\). Let \(Q_n\) be the sum of the principal parts at the finitely many points of \(A\cap(K_n\setminus K_{n-1})\). It is holomorphic near \(K_{n-1}\). By Carl Runge’s theorem of 1885, it can be approximated uniformly on \(K_{n-1}\), within \(2^{-n}\), by a rational function \(R_n\) whose poles lie outside \(\Omega\). Then \(f=\sum_n(Q_n-R_n)\) converges uniformly on each \(K_m\) after discarding finitely many terms, and has the right poles. When \(\Omega=\mathbb C\), the poles of \(R_n\) can be put at infinity, so \(R_n\) is a polynomial, as in Lesson 05.
Combined with Weierstrass’s product theorem for open sets, the result gives two classical corollaries: every meromorphic function on \(\Omega\) is a quotient of two holomorphic functions on \(\Omega\), and every open set is the natural domain of existence of some holomorphic function.
Exercise 6.1In the unit disc, let \(a_n=1-2^{-n}\). Show that \(f(z)=\sum_{n\ge1}\Big(\dfrac{1}{z-a_n}-\dfrac{1}{z-1}\Big)\) is meromorphic in the disc with simple poles of residue 1 at the \(a_n\).
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Exercise 6.2In \(\Omega=\mathbb C\setminus\{0\}\), construct a meromorphic function with simple poles of residue 1 at the points \(1/n\), \(n\ge1\).
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The star and analytic continuation
For the general reader. A power series converges only in a disc, whose edge is set by the nearest singularity, even though the function it represents may extend much further. Weierstrass extended functions by re-expanding series at new centres, chain after chain. Mittag-Leffler wanted a single formula, computed from the original Taylor coefficients, that converges to the function in as large a region as possible. The natural region is a star, and between 1899 and 1905 he gave such formulas in five notes in Acta.
- Define the Mittag-Leffler star of a power series.
- State Mittag-Leffler’s representation theorem and his summation method.
- Compute stars and compare with Borel’s polygon.
The star
Let \(f(z)=\sum_{k\ge0}a_kz^k\) have positive radius of convergence. Say that a point \(z\) belongs to the star \(S_f\) if \(f\) can be continued analytically along the whole segment \([0,z]\), that is, along \(t\mapsto tz\), \(0\le t\le1\). On each ray from 0 the continuation stops at the first singular point met, so \(S_f\) is the plane with a closed ray removed behind each singularity visible from the origin. It is open and star-shaped about 0, contains the disc of convergence, and on it the continuation of \(f\) is single-valued.
There are constants \(c_{n,k}\), depending only on \(n\) and \(k\) and not on \(f\), such that for every power series \(f=\sum a_kz^k\) the polynomials
\[ p_n(z)=\sum_{k=0}^{k_n}c_{n,k}\,a_k\,z^k \]converge to the analytic continuation of \(f\) uniformly on compact subsets of the star \(S_f\). One such method is
\[ f(z)=\lim_{\alpha\to0^+}\ \sum_{k=0}^{\infty}\frac{a_k\,z^k}{\Gamma(1+\alpha k)},\qquad z\in S_f. \]Why the second formula works. For \(\alpha>0\), the factor \(1/\Gamma(1+\alpha k)\) decays faster than any geometric sequence, so the series defines an entire function of \(z\). Writing \(a_k=\frac{1}{2\pi i}\oint f(w)w^{-k-1}\,dw\) and summing under the integral,
\[ \sum_{k\ge0}\frac{a_kz^k}{\Gamma(1+\alpha k)}=\frac{1}{2\pi i}\oint f(w)\,E_\alpha\Big(\frac zw\Big)\frac{dw}{w},\qquad E_\alpha(t)=\sum_{k\ge0}\frac{t^k}{\Gamma(1+\alpha k)}. \]As \(\alpha\to0^+\), \(E_\alpha(t)\) tends to \(\frac1{1-t}\) for \(t\) outside a sector around \([1,\infty)\) whose opening shrinks with \(\alpha\), and in that limit the integral is Cauchy’s formula for \(f(z)\). Since the kernel is large only when \(z/w\) lies near \([1,\infty)\), that is, when \(w\) lies near the segment \([0,z]\), the contour can be deformed far into the star while avoiding that segment. Making this precise needs the asymptotics of \(E_\alpha\) in Lesson 08.
Émile Borel’s method of summation, based on the Laplace transform, converges in a smaller region, the Borel polygon, which is always contained in the star.
Exercise 7.1Find the stars of \(\dfrac1{1-z}\), \(\log(1+z)\) and \(\dfrac1{1+z^4}\), and the radius of convergence of each Taylor series at 0.
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Exercise 7.2For the geometric series \(\sum z^k\), compute \(\sum_k\frac{z^k}{\Gamma(1+\alpha k)}\) for \(\alpha=1\) and \(\alpha=2\), and the formal value at \(\alpha=0\).
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The function \(E_\alpha\)
For the general reader. The exponential function solves the simplest growth and decay equations. In 1903 Mittag-Leffler introduced a family of functions \(E_\alpha\) that interpolate between the exponential and other elementary functions, as a tool for his summation method. A century later they became the basic special functions of fractional calculus, describing anomalous diffusion and the slow relaxation of viscoelastic materials, polymers and glasses.
- Define \(E_\alpha\) and identify its elementary special cases.
- Find the order of growth of \(E_\alpha\).
- Solve the fractional relaxation equation with \(E_\alpha\).
For \(\alpha>0\), \(\displaystyle E_\alpha(z)=\sum_{k=0}^{\infty}\frac{z^k}{\Gamma(\alpha k+1)}\). Anders Wiman introduced in 1905 the two-parameter version \(E_{\alpha,\beta}(z)=\sum_k z^k/\Gamma(\alpha k+\beta)\).
Special cases: \(E_1(z)=e^z\), \(E_2(z^2)=\cosh z\), \(E_2(-z^2)=\cos z\), and \(E_{1/2}(z)=e^{z^2}\operatorname{erfc}(-z)\). By Stirling’s formula \(E_\alpha\) is entire of order \(1/\alpha\).
Let \(0<\alpha<2\). As \(|z|\to\infty\),
\[ E_\alpha(z)=\frac1\alpha\exp\big(z^{1/\alpha}\big)-\sum_{k=1}^{N}\frac{z^{-k}}{\Gamma(1-\alpha k)}+O\big(|z|^{-N-1}\big)\quad\text{for }|\arg z|\le\tfrac{\alpha\pi}{2}, \]while for \(|\arg(-z)|<(1-\tfrac\alpha2)\pi\) the exponential term is absent and \(E_\alpha(z)\) decays like \(-\sum_k z^{-k}/\Gamma(1-\alpha k)\), in particular like \(\frac{1}{\Gamma(1-\alpha)}|z|^{-1}\) along the negative axis for \(0<\alpha<1\).
These asymptotics are what Lesson 07 needed: as \(\alpha\to0^+\), the sector where \(E_\alpha\) is exponentially large closes up on the positive real axis, and elsewhere \(E_\alpha(z)\to-\sum_{k\ge1}z^{-k}=\frac1{1-z}\).
Fractional relaxation
For \(0<\alpha\le1\), the Caputo fractional derivative of a function \(y\) on \(t>0\) is \(D^\alpha y(t)=\frac{1}{\Gamma(1-\alpha)}\int_0^t\frac{y'(s)}{(t-s)^{\alpha}}\,ds\) for \(\alpha<1\), and \(D^1y=y'\). On powers, \(D^\alpha t^\beta=\frac{\Gamma(\beta+1)}{\Gamma(\beta+1-\alpha)}t^{\beta-\alpha}\) for \(\beta>0\), and \(D^\alpha1=0\).
For \(\lambda>0\) and \(0<\alpha\le1\), the solution of \(D^\alpha y=-\lambda y\), \(y(0)=1\), is \(y(t)=E_\alpha(-\lambda t^\alpha)\). It decreases from 1 to 0, and for \(\alpha<1\) it decays like \(\frac{t^{-\alpha}}{\lambda\,\Gamma(1-\alpha)}\), a power law instead of an exponential. Harry Pollard proved in 1948 that \(x\mapsto E_\alpha(-x)\) is completely monotone on \([0,\infty)\) for \(0\le\alpha\le1\).
Exercise 8.1Verify \(E_2(-z^2)=\cos z\) and \(E_2(z^2)=\cosh z\).
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Exercise 8.2Using the formula for \(D^\alpha t^\beta\), verify term by term that \(y=E_\alpha(-\lambda t^\alpha)\) solves \(D^\alpha y=-\lambda y\).
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Exercise 8.3Show that \(E_\alpha\) has order \(1/\alpha\), using the fact that an entire function \(\sum c_kz^k\) has order \(\limsup_k\frac{k\log k}{\log(1/|c_k|)}\).
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Several variables: the Cousin problem
For the general reader. In one complex variable, Mittag-Leffler’s theorem always works. In two or more variables, singularities are no longer isolated points but whole surfaces, and the question becomes whether local data can be glued into one global function. Pierre Cousin posed this in 1895. It does not always have a solution, and the search for the right conditions led to sheaf cohomology, one of the central tools of twentieth-century geometry.
- Restate Mittag-Leffler’s theorem as a gluing problem.
- Solve it in one variable with the \(\bar\partial\)-equation.
- See the obstruction in \(\mathbb C^2\setminus\{0\}\).
Mittag-Leffler data
Let \(X\) be a complex manifold with an open cover \(\{U_i\}\). Cousin I data are meromorphic functions \(f_i\) on \(U_i\) such that \(f_i-f_j\) is holomorphic on \(U_i\cap U_j\). A solution is a global meromorphic \(f\) with \(f-f_i\) holomorphic on each \(U_i\). Prescribing principal parts at isolated points is the special case of Lesson 06.
(i) If \(H^1(X,\mathcal O)=0\), every Cousin I problem on \(X\) is solvable. (ii) For every open \(\Omega\subseteq\mathbb C\), \(H^1(\Omega,\mathcal O)=0\). (iii) (Cousin 1895 for product domains; Kiyoshi Oka, 1937) Every Cousin I problem on a domain of holomorphy in \(\mathbb C^n\) is solvable.
Idea of (i). The differences \(g_{ij}=f_i-f_j\) are holomorphic on overlaps and satisfy \(g_{ij}+g_{jk}=g_{ik}\): they form a Čech 1-cocycle with values in \(\mathcal O\). If \(H^1(X,\mathcal O)=0\) it is a coboundary, \(g_{ij}=h_i-h_j\) with \(h_i\) holomorphic on \(U_i\). Then \(f=f_i-h_i\) agrees on overlaps and solves the problem.
Idea of (ii). Using a partition of unity, the cocycle splits smoothly as \(g_{ij}=\varphi_i-\varphi_j\) with \(\varphi_i\) smooth. Then \(\bar\partial\varphi_i=\bar\partial\varphi_j\) on overlaps, so these patch to a global smooth \((0,1)\)-form \(v\,d\bar z\). If \(u\) solves \(\partial u/\partial\bar z=v\), the functions \(h_i=\varphi_i-u\) are holomorphic and \(h_i-h_j=g_{ij}\). In one variable \(\partial u/\partial\bar z=v\) is always solvable on any open set; for compactly supported \(v\) the solution is
\[ u(z)=\frac{1}{\pi}\int_{\mathbb C}\frac{v(w)}{z-w}\,dA(w), \]and an exhaustion argument with Runge’s theorem, the same one as in Lesson 06, handles general \(v\). This proof, from Lars Hörmander’s book, reduces Mittag-Leffler’s theorem to the solvability of the \(\bar\partial\)-equation.
Exercise 9.1On \(X=\mathbb C^2\setminus\{0\}\) with \(U_1=\{z_1\ne0\}\), \(U_2=\{z_2\ne0\}\), let \(f_1=\dfrac{1}{z_1z_2}\) on \(U_1\) and \(f_2=0\) on \(U_2\). Show that these are Cousin I data and that the problem has no solution.
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Exercise 9.2Check that \(u(z)=\frac1\pi\int\frac{v(w)}{z-w}\,dA(w)\) solves \(\partial u/\partial\bar z=v\) when \(v=\partial\psi/\partial\bar z\) for a smooth compactly supported \(\psi\), by identifying \(u\).
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The Mittag-Leffler condition
For the general reader. The proof of Mittag-Leffler’s theorem builds a function in stages, one compact region at a time, and makes the stages fit by small corrections. Nicolas Bourbaki and later algebraists isolated the abstract pattern: when do compatible pieces of information at each stage come from a single global object? The answer, a condition on images in an inverse system, carries Mittag-Leffler’s name throughout algebra, topology and algebraic geometry.
- Define inverse limits, \(\varprojlim^1\), and the Mittag-Leffler condition.
- Prove that the condition kills \(\varprojlim^1\).
- Compute a tower where the condition fails.
Towers and their limits
A tower of abelian groups is a sequence \(A_1\leftarrow A_2\leftarrow A_3\leftarrow\cdots\) of homomorphisms \(f_n:A_{n+1}\to A_n\). Define \(d:\prod_nA_n\to\prod_nA_n\) by \(d(a)_n=a_n-f_n(a_{n+1})\). Then
\[ \varprojlim A_n=\ker d,\qquad \varprojlim{}^1A_n=\operatorname{coker}d. \]A short exact sequence of towers \(0\to A\to B\to C\to0\) gives, by the snake lemma applied to \(d\), an exact sequence
\[ 0\to\varprojlim A\to\varprojlim B\to\varprojlim C\to\varprojlim{}^1A\to\varprojlim{}^1B\to\varprojlim{}^1C\to0. \]Say the tower satisfies the Mittag-Leffler condition if for each \(n\) the images of the composites \(A_m\to A_n\), \(m\ge n\), are eventually constant. Then \(\varprojlim^1A_n=0\). In particular \(\varprojlim\) preserves exactness of \(0\to A\to B\to C\to0\) when \(A\) satisfies the condition.
Proof sketch. If all \(f_n\) are surjective, solve \(a_n-f_n(a_{n+1})=b_n\) by choosing \(a_1=0\) and then each \(a_{n+1}\) as a preimage of \(a_n-b_n\) (Exercise 10.2). In general, the stable images \(A_n'\) form a tower with surjective maps, and the quotient tower \(A_n/A_n'\) has \(\varprojlim^1=0\) because its maps are eventually zero along any composite, which lets one write down a solution of \(d(a)=b\) as a finite sum at each level.
Topological version
Let \(X_1\leftarrow X_2\leftarrow\cdots\) be complete metric spaces with uniformly continuous maps whose images are dense. Then \(\varprojlim X_n\) is non-empty, and its image in each \(X_n\) is dense.
Applied to the spaces of functions meromorphic near the compact sets \(K_n\) of Lesson 06 with the prescribed principal parts, with the topology of uniform convergence, density of the maps is exactly Runge’s theorem, and the theorem returns Mittag-Leffler’s. The condition appears in the Milnor exact sequence for homotopy groups and in Alexander Grothendieck’s theory of formal functions.
Exercise 10.1Let \(A_n=\mathbb Z\) for all \(n\), with every \(f_n\) multiplication by a prime \(p\). Show that the tower fails the Mittag-Leffler condition, that \(\varprojlim A_n=0\), and that \(\varprojlim^1A_n\cong\mathbb Z_p/\mathbb Z\), with \(\mathbb Z_p\) the \(p\)-adic integers.
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Exercise 10.2Prove directly that \(\varprojlim^1A_n=0\) when every \(f_n\) is surjective.
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Stockholm and Acta Mathematica, 1881–1911
The journal
The idea of a Scandinavian mathematics journal came from Sophus Lie in 1881. Mittag-Leffler made it international. Acta Mathematica appeared in 1882, funded by subscriptions, an appeal to donors and his wife’s fortune; King Oscar II was its first subscriber. Its first volume opened with Henri Poincaré’s Théorie des groupes fuchsiens, and Poincaré’s papers on automorphic functions filled much of the early volumes. In 1883 Mittag-Leffler printed French translations of Georg Cantor’s papers on set theory, which German journals had been reluctant to accept. Leopold Kronecker, Cantor’s fiercest critic, refused to publish in Acta. Mittag-Leffler was protective of Cantor but also cautious: in 1885 he persuaded him to withdraw a paper on order types, judging it far ahead of its time. Cantor took the advice badly and their friendship cooled.
Mittag-Leffler edited Acta for 45 years. He judged papers shrewdly, published French and German authors side by side in the years after 1870, when their national journals barely spoke to each other, and wrote tirelessly to bring in the best work. G. H. Hardy, who knew him late in life, called him a mathematician of the front rank and a fine judge of the quality of others’ work.
Kovalevskaya
As soon as he held the Stockholm chair, Mittag-Leffler worked to bring Sofia Kovalevskaya there. The private Stockholms högskola could appoint a woman where the state universities could not. She arrived late in 1883, began lecturing early in 1884, and in June 1884 was appointed professor for five years. She joined the editorial board of Acta. His sister Anne Charlotte Leffler became her close friend, and together they wrote the play The Struggle for Happiness (1887). After Kovalevskaya won the Prix Bordin in 1888, he secured her appointment as professor for life in 1889. When she died in February 1891, he wrote about her life and work and defended her scientific reputation.
The King Oscar prize
In 1885 Mittag-Leffler announced in Acta a prize competition for the sixtieth birthday of King Oscar II of Sweden and Norway. The jury was Mittag-Leffler, Weierstrass and Hermite. The first of four questions asked for series solutions of the \(n\)-body problem converging uniformly for all time. Twelve entries arrived by June 1888, and on the king’s birthday, 21 January 1889, the prize went to Poincaré for his memoir on the three-body problem. While the memoir was being printed, the editor Edvard Phragmén queried some convergence arguments. Poincaré found a far deeper error, and the printed copies had to be recalled and destroyed. Mittag-Leffler handled the affair with discretion; the corrected memoir filled Acta 13 in 1890 and became the starting point of chaos theory.
The Stockholm school
In Stockholm he gathered a remarkable group: Kovalevskaya; Edvard Phragmén, later known for the Phragmén–Lindelöf principle; Ivar Bendixson, of the Poincaré–Bendixson theorem; Helge von Koch, whose snowflake curve appeared in 1904 and who took his doctorate with Mittag-Leffler in 1892; and Ivar Fredholm, who studied with him in Stockholm and published his theory of integral equations in Acta in 1903. Mittag-Leffler wanted the högskola to remain a research school. Bendixson, who wanted a more conventional university, prevailed in the arguments over its future. Mittag-Leffler retired from his chair in 1911.
DiscussionMittag-Leffler’s theorem fills a page; his journal, his prize and his appointments changed the course of mathematics. Judge his career by both measures. What made an editor’s judgement decisive in the 1880s, and is it still?
Djursholm, death, legacy, 1889–1927
From 1889 Mittag-Leffler bought land at Djursholm, a new garden suburb north of Stockholm, and by April 1891 the family villa was complete. It was enlarged around 1900 and 1906. The house held one of the great mathematical libraries, with books going back to the sixteenth century, and from 1904 to 1914 he hosted a celebration there each December during the Nobel festivities. Hardy, who visited him in the country, saw in him both the cosmopolitan scholar and the rural landowner. He was also a businessman: he helped found an insurance company in 1882 and later invested in industrial ventures.
Mittag-Leffler was active in the early Nobel Prizes. In 1903 he alerted Pierre Curie that the nomination for the physics prize named only Pierre and Henri Becquerel; Pierre insisted, and Marie Curie shared the prize. He later campaigned, without success, for a physics prize for Poincaré. Stories that Alfred Nobel left out mathematics because of a rivalry with Mittag-Leffler have no basis in the evidence.
Honours came from across Europe. He was elected to the Royal Swedish Academy of Sciences in 1883, an honorary member of the London Mathematical Society in 1892, a foreign member of the Royal Society in 1896 and a member of the Paris Academy of Sciences in 1900. He spoke at the International Congresses of Mathematicians of 1900 and 1908, and received honorary degrees from Oxford, Cambridge, Aberdeen, St Andrews, Bologna and Christiania (Oslo).
The Institute
On his seventieth birthday, 16 March 1916, Gösta and Signe Mittag-Leffler made public their will. It left the villa, the library and their fortune to a foundation to promote pure mathematics in the Scandinavian countries, with a research institute, professorships and fellowships. The foundation was placed under the Royal Swedish Academy of Sciences in 1919. The war and inflation eroded the capital; Signe died in 1921, and the crash of 1922 brought Mittag-Leffler close to bankruptcy. He died at Djursholm on 7 July 1927, aged 81.
Torsten Carleman directed the institute until his death in 1949, after which it was for nearly twenty years little more than a library. In 1969 Lennart Carleson revived it as Mittag-Leffler had intended, a centre for visiting researchers and research programmes, which it remains. Acta Mathematica is still published by the institute and is among the most selective journals in mathematics.
Legacy
- Complex analysis: the Mittag-Leffler theorem, with Weierstrass’s product theorem, is the foundation of the theory of meromorphic functions on arbitrary domains.
- Summation and continuation: the Mittag-Leffler star and summation method, and the functions \(E_\alpha\) and \(E_{\alpha,\beta}\), now central to fractional calculus.
- Algebra and geometry: the Cousin problems and the Mittag-Leffler condition carry his idea of gluing local data into sheaf cohomology and homological algebra.
- Institutions: Acta Mathematica and the Institut Mittag-Leffler; a glacier on Spitsbergen also bears his name.
Final projectChoose one theorem from Part II. Write a two-page account for a strong undergraduate that states it, works one example in full, and explains how the idea of correcting a divergent construction term by term, learned from Weierstrass, appears in it.
Connections
People linked to Gösta Mittag-Leffler across this collection. A name without a link has no page here yet. See Gösta Mittag-Leffler in the network of all 337 lives →
Teachers and advisors
- Karl Weierstrass
- Göran Dillner 1872
Students
- Ivar Fredholm
- Helge von Koch 1892
- Hjalmar Mellin 1882
Influenced by
- Charles Hermite 1873-1901
- Karl Weierstrass
Colleagues and collaborators
- Charles Hermite
- G. H. Hardy
- Gaston Darboux
- Georg Cantor
- Henri Poincaré
- Marie Curie
- Pierre Curie
- Sofia Kovalevskaya 1876-1891
- Sophus Lie
- Thomas Joannes Stieltjes 1885-1887
- Edvard Phragmén
- Ivar Bendixson
Rivals
Also mentioned in this life
- Isaac Barrow
- Henri Becquerel
- Émile Borel
- Augustin-Louis Cauchy
- Michel Chasles
- Leonhard Euler
- Alexander Grothendieck
- Pierre-Simon Laplace
- Joseph Liouville
- John Milnor
Fields
- complex analysis 13 lives
On CoursesHub
Sources and further reading
Biography
- J. J. O’Connor and E. F. Robertson, Magnus Gösta Mittag-Leffler, MacTutor History of Mathematics.
- Gösta Mittag-Leffler, Wikipedia.
- Institut Mittag-Leffler, History and The prize competition of King Oscar II.
- Obituary, The Times, July 1927 (MacTutor).
- A. Stubhaug, Gösta Mittag-Leffler: A Man of Conviction, Springer, 2010; reviews.
- G. H. Hardy, Gösta Mittag-Leffler, J. London Math. Soc. 3 (1928), 156–160.
- Gösta Magnus Mittag-Leffler, Mathematics Genealogy Project.
- J. Barrow-Green, Poincaré and the Three Body Problem, American Mathematical Society, 1997.
Mathematics
- G. Mittag-Leffler, Sur la représentation analytique des fonctions monogènes uniformes d’une variable indépendante, Acta Math. 4 (1884), 1–79.
- G. Mittag-Leffler, Sur la représentation analytique d’une branche uniforme d’une fonction monogène, five notes, Acta Math. 23–29 (1900–1905).
- G. Mittag-Leffler, Sur la nouvelle fonction \(E_\alpha(x)\), C. R. Acad. Sci. Paris 137 (1903), 554–558.
- L. E. Turner, The Mittag-Leffler theorem: the origin, evolution, and reception of a mathematical result, 1876–1884, Historia Mathematica 40 (2013), 36–83.
- W. Rudin, Real and Complex Analysis, 3rd ed., McGraw-Hill, 1987, chapters 13 and 15.
- G. H. Hardy, Divergent Series, Oxford, 1949 (Mittag-Leffler summation and the star).
- R. Gorenflo, A. A. Kilbas, F. Mainardi, S. V. Rogosin, Mittag-Leffler Functions, Related Topics and Applications, Springer, 2014; 2nd ed. 2020.
- L. Hörmander, An Introduction to Complex Analysis in Several Variables, North-Holland, 3rd ed. 1990.
- C. A. Weibel, An Introduction to Homological Algebra, Cambridge, 1994, §3.5 (\(\varprojlim^1\) and the Mittag-Leffler condition).