NEWSLETTER OF THE EUROPEAN MATHEMATICAL SOCIETY
Features Elliptic Functions According to Eisenstein and Kronecker Wrinkles: From the Sea to Mathematics Kardar–Parisi–Zhang Universality
Photo courtesy of Dyrol Lumbard, Oxford Interview Sir Andrew Wiles S E European September 2016 M M Mathematical Issue 101 History E S Society ISSN 1027-488X Göttingen State and University Library Journals published by the
ISSN print 2313-1691 Published by Foundation Compositio Mathematica and EMS ISSN online 2214-2584 Managing Editors: 2016. Vol. 3 Gavril Farkas (Humboldt Universität zu Berlin, Germany); Yuri Tschinkel (New York University, USA) Approx. 600 pages. 21.0 x 28.0 cm Aims and Scope Price of subscription: Algebraic Geometry is an open access journal owned by the Foundation Compositio Mathematica. The Online free of charge purpose of the journal is to publish first-class research papers in algebraic geometry and related fields. All 198 ¤ print (1 volume, hard cover) contributions are required to meet high standards of quality and originality and are carefully screened by experts in the field.
ISSN print 2308-5827 Annales de l’Institut Henri Poincaré D ISSN online 2308-5835 Editors-in-Chief: 2017. Vol. 4. 4 issues Gérard H. E. Duchamp (Université Paris XIII, France); Vincent Rivasseau (Université Paris XI, France); Approx. 400 pages. 17.0 x 24.0 cm Alan Sokal (New York University, USA and University College London, UK) Price of subscription: Managing Editor: 198 ¤ online only Adrian Tanasa˘ (Université de Bordeaux, France) 238 ¤ print+online Aims and Scope The journal is dedicated to publishing high-quality original research articles and survey articles in which combinatorics and physics interact in both directions. Combinatorial papers should be motivated by potential applications to physical phenomena or models, while physics papers should contain some interesting combinatorial development.
ISSN print 0010-2571 A journal of the Swiss Mathematical Society ISSN online 1420-8946 Editor-in-Chief: 2017. Vol. 92. 4 issues Eva Bayer-Fluckiger (École Polytechnique Fédérale de Lausanne, Switzerland) Approx. 800 pages. 17.0 x 24.0 cm Price of subscription: Aims and Scope 328 ¤ online only The Commentarii Mathematici Helvetici was established on the occasion of a meeting of the Swiss 388 ¤ print+online Mathematical Society in May 1928, the first volume published in 1929. The journal soon gained international reputation and is one of the world’s leading mathematical periodicals. The journal is intended for the publication of original research articles on all aspects in mathematics.
ISSN print 0013-6018 A journal of the Swiss Mathematical Society ISSN online 1420-8962 Managing Editor: 2017. Vol. 72. 4 issues Norbert Hungerbühler (ETH Zürich, Switzerland) Approx. 180 pages. 17.0 x 24.0 cm Price of subscription: Aims and Scope 74 ¤ online only (institutional) Elemente der Mathematik publishes survey articles about important developments in the field of mathe- 90 ¤ print+online (institutional) matics; stimulating shorter communications that tackle more specialized questions; and papers that 52 ¤ print (individual) report on the latest advances in mathematics and applications in other disciplines. The journal does not focus on basic research. Rather, its articles seek to convey to a wide circle of readers (teachers, students, engineers, professionals in industry and administration) the relevance, intellectual challenge and vitality of mathematics today.
ISSN print 2308-2151 Editors in Chief: ISSN online 2308-216X Nicola Bellomo (Politecnico di Torino, Italy); Simon Salamon (King’s College London, UK) 2017. Vol. 4. 2 double issues Aims and Scope Approx. 400 pages. 17.0 x 24.0 cm The EMS Surveys in Mathematical Sciences is dedicated to publishing authoritative surveys and high-level Price of subscription: expositions in all areas of mathematical sciences. It is a peer-reviewed periodical which communicates ¤ 198 online only advances of mathematical knowledge to give rise to greater progress and cross-fertilization of ideas. ¤ 238 print+online Surveys should be written in a style accessible to a broad audience, and might include ideas on conceivable applications or conceptual problems posed by the contents of the survey.
ISSN print 0013-8584 Official organ of The International Commission on Mathematical Instruction ISSN online 2309-4672 Editors: 2017. Vol. 63. 2 double issues A. Alekseev, D. Cimasoni, P. de la Harpe, A. Karlsson, T. Smirnova-Nagnibeda, A. Szenes (all Université de Approx. 450 pages. 17.0 x 24.0 cm Genève, Switzerland); N. Monod (Ecole Polytechnique Fédérale de Lausanne, Switzerland; V. F. R. Jones Price of subscription: (University of California at Berkeley, USA); J. Steinig 198 ¤ online only Aims and Scope 238 ¤ print+online L’Enseignement Mathématique was founded in 1899 by Henri Fehr (Geneva) and Charles-Ange Laisant (Paris). It is intended primarily for publication of high-quality research and expository papers in mathematics. Approximately 60 pages each year will be devoted to book reviews.
European Mathematical Society Publishing House Scheuchzerstrasse 70 [email protected] Seminar for Applied Mathematics, ETH-Zentrum SEW A27 CH-8092 Zürich, Switzerland www.ems-ph.org Contents Editorial Team Editor-in-Chief Vladimir R. Kostic European (Social Media) Valentin Zagrebnov Department of Mathematics Institut de Mathématiques de and Informatics Marseille (UMR 7373) – CMI University of Novi Sad Mathematical Technopôle Château-Gombert 21000 Novi Sad, Serbia 39, rue F. Joliot Curie e-mail: [email protected] 13453 Marseille Cedex 13, France Eva Miranda Society e-mail: [email protected] (Research Centres) Department of Mathematics Copy Editor EPSEB, Edifici P Universitat Politècnica Newsletter No. 101, September 2016 Chris Nunn de Catalunya 119 St Michaels Road, Av. del Dr Maran˜on 44–50 Aldershot, GU12 4JW, UK 08028 Barcelona, Spain Editorial – V. A. Zagrebnov...... 3 e-mail: [email protected] e-mail: [email protected] EMS Executive Committee Meeting in Stockholm – R. Elwes...... 3 Editors Vladimir L. Popov Meeting of Presidents of Mathematical Societies in Budapest – Steklov Mathematical Institute Ramla Abdellatif Russian Academy of Sciences S. Verduyn Lunel & R. Elwes...... 5 LAMFA – UPJV Gubkina 8 2016 Kamil Duszenko Prize Goes to Kate Juschenko...... 7 80039 Amiens Cedex 1, France 119991 Moscow, Russia e-mail: [email protected] e-mail: [email protected] Elliptic Functions According to Eisenstein and Kronecker: An Update – P. Charollois & R. Sczech...... 8 Jean-Paul Allouche Themistocles M. Rassias (Book Reviews) (Problem Corner) Wrinkles: From the Sea to Mathematics – F. Laudenbach...... 15 IMJ-PRG, UPMC Department of Mathematics Kardar–Parisi–Zhang Universality – I. Corwin...... 19 4, Place Jussieu, Case 247 National Technical University 75252 Paris Cedex 05, France of Athens, Zografou Campus Interview with Abel Laureate Sir Andrew Wiles – M. Raussen & e-mail: [email protected] GR-15780 Athens, Greece C. Skau...... 29 e-mail: [email protected] Jorge Buescu Göttingen’s SUB as Repository for the Papers of Distinguished (Societies) Volker R. Remmert Mathematicians – D. E. Rowe...... 39 Dep. Matemática, Faculdade (History of Mathematics) de Ciências, Edifício C6, IZWT, Wuppertal University Club de Mathématiques Discrètes Lyon – B. Lass...... 45 Piso 2 Campo Grande D-42119 Wuppertal, Germany Moscow University Maths Department for Schoolchildren – 1749-006 Lisboa, Portugal e-mail: [email protected] e-mail: [email protected] A. V. Begunts & A. E. Pankratiev...... 46 Vladimir Salnikov Mathematics in Kolmogorov’s School – N. Salnikov & Lucia Di Vizio University of Luxembourg LMV, UVSQ Mathematics Research Unit K. Semenov...... 48 45 avenue des États-Unis Campus Kirchberg Ludus’ 10th Anniversary – J. N. Silva...... 50 78035 Versailles cedex, France 6, rue Richard Coudenhove- e-mail: [email protected] Kalergi e-Math Workshops: a Forum for Exchanging Experiences of L-1359 Luxembourg Mathematics e-Learning at University Level – A. F. Costa, Jean-Luc Dorier [email protected] (Math. Education) F. P. da Costa & M. A. Huertas...... 52 FPSE – Université de Genève Dierk Schleicher New zbMATH Atom Feed – F. Müller...... 54 Bd du pont d’Arve, 40 Research I 1211 Genève 4, Switzerland Jacobs University Bremen MSC2020 – E. G. Dunne & K. Hulek...... 55 [email protected] Postfach 750 561 Book Reviews...... 56 28725 Bremen, Germany Javier Fresán [email protected] Solved and Unsolved Problems – T. M. Rassias...... 58 (Young Mathematicians’ Column) Departement Mathematik Olaf Teschke The views expressed in this Newsletter are those of the ETH Zürich (Zentralblatt Column) 8092 Zürich, Switzerland authors and do not necessarily represent those of the FIZ Karlsruhe EMS or the Editorial Team. e-mail: [email protected] Franklinstraße 11 10587 Berlin, Germany ISSN 1027-488X e-mail: [email protected] © 2016 European Mathematical Society Jaap Top Published by the University of Groningen EMS Publishing House Department of Mathematics ETH-Zentrum SEW A27 P.O. Box 407 CH-8092 Zürich, Switzerland. 9700 AK Groningen, homepage: www.ems-ph.org The Netherlands Scan the QR code to go to the e-mail: [email protected] Newsletter web page: For advertisements and reprint permission requests http://euro-math-soc.eu/newsletter contact: [email protected]
EMS Newsletter September 2016 1 EMS Agenda EMS Executive Committee EMS Agenda
President Prof. Gert-Martin Greuel 2016 (2013–2016) Prof. Pavel Exner Department of Mathematics 4 – 6 November (2015–2018) University of Kaiserslautern EMS Executive Committee Meeting, Tbilisi, Georgia Doppler Institute Erwin-Schroedinger Str. Czech Technical University D-67663 Kaiserslautern 2017 Brˇehová 7 Germany CZ-11519 Prague 1 e-mail: [email protected] 1 – 2 April Czech Republic Prof. Laurence Halpern Presidents Meeting, Lisbon, Portugal e-mail: [email protected] (2013–2016) Laboratoire Analyse, Géométrie Vice-Presidents & Applications UMR 7539 CNRS EMS Scientific Events Université Paris 13 Prof. Franco Brezzi 2016 (2013–2016) F-93430 Villetaneuse Istituto di Matematica Applicata France e-mail: [email protected] 18 – 22 September e Tecnologie Informatiche del 7th International Conference on Advanced Computational C.N.R. Prof. Volker Mehrmann Methods in Engineering, Ghent, Belgium via Ferrata 3 (2011–2018) http://www.acomen.ugent.be/ I-27100 Pavia Institut für Mathematik Italy TU Berlin MA 4–5 26 – 30 September e-mail: [email protected] Strasse des 17. Juni 136 10th Euro-Maghrebian Workshop on Evolutions Equations Prof. Martin Raussen D-10623 Berlin Heinrich Fabri Institute, Blaubeuren, Germany (2013–2016) Germany http://euromaghreb10.math.kit.edu Department of Mathematical e-mail: [email protected] Sciences Prof. Armen Sergeev 25 September – 1 October Aalborg University (2013–2016) 50th Jubilee Sophus Lie Seminar Fredrik Bajers Vej 7G Steklov Mathematical Institute Banach Conference Center, Bedlewo DK-9220 Aalborg Øst Russian Academy of Sciences Distinguished EMS Lecturer: Ernest Vinberg Denmark Gubkina str. 8 http://50sls.impan.pl e-mail: [email protected] 119991 Moscow Russia 3 – 4 November Secretary e-mail: [email protected] Geometry and Lie theory. Applications to classical and quan- tum mechanics. Dedicated to 70th birthday of Eldar Straume. Prof. Sjoerd Verduyn Lunel EMS Secretariat NTNU Trondheim, Norway (2015–2018) https://www.math.ntnu.no/~mariusth/Eldar70/ Department of Mathematics Utrecht University Ms Elvira Hyvönen Department of Mathematics 14 – 16 November Budapestlaan 6 ICERI2016 (9th Annual International Conference of Education, NL-3584 CD Utrecht and Statistics P. O. Box 68 Research and Innovation), Seville, Spain The Netherlands http://iated.org/iceri e-mail: [email protected] (Gustaf Hällströmin katu 2b) 00014 University of Helsinki 8 – 12 December Treasurer Finland Tel: (+358) 2941 51141 International Conference Geometric Analysis and Control e-mail: [email protected] Theory, Sobolev Institute of Mathematics, Novosibirsk, Russian Prof. Mats Gyllenberg Web site: http://www.euro-math-soc.eu Federation (2015–2018) http://gct.math.nsc.ru/?event=geometric-analysis-and-control- Department of Mathematics EMS Publicity Officer theory and Statistics University of Helsinki Dr. Richard H. Elwes 19 – 23 December P. O. Box 68 School of Mathematics International Conference “Anosov systems and modern dy- FIN-00014 University of Helsinki University of Leeds namics”. Dedicated to the 80th anniversary of Dmitry Anosov. Finland Leeds, LS2 9JT Steklov Mathematical Institute, Moscow, Russian Federation e-mail: [email protected] UK http://anosov80.mi.ras.ru/ e-mail: [email protected] Ordinary Members 2017
Prof. Alice Fialowski 24 – 28 July (2013–2016) 31st European Meeting of Statisticians Institute of Mathematics Helsinki Eötvös Loránd University EMS-Bernoulli Society Joint Lecture: Alexander Holevo Pázmány Péter sétány 1/C H-1117 Budapest Hungary e-mail: [email protected]
2 EMS Newsletter September 2016 Editorial Editorial
Valentin A. Zagrebnov (Institut de Mathématiques de Marseille, France), Editor-in-Chief of the EMS Newsletter
Dear EMS Newsletter Readers, the labyrinth of the production process of the previous newsletter issue (June 2016). Secondly, she armed me It is at once an honour and a great with a detailed and transparent memorandum covering challenge for me to take over the the activity of the editor-in-chief of the Newsletter, which editorship of the EMS Newsletter, has served me well for the practical exercise of preparing starting with this September 2016 this, my first issue of the Newsletter. issue. The outgoing editor Lucia Di Lucia left me the EMS Newsletter in very good shape Vizio did a superb job of managing and I shall do my best to keep its high standards and rep- the publication of the newsletter utation. In this role, I can only aspire to similar success. over the previous four years. She has put a lot of energy With the aid of the editorial board, I am optimistic that into advancing the quality and visibility of the journal. we can keep bringing to your attention insightful per- I hope to profit from her experience as a member spectives on research, news and other items of interest of the editorial board. My personal thanks to Lucia are in mathematics. We hope that all readers will feel free to twofold. Firstly, I am grateful for her endless patience in contact the editorial board whenever they have ideas for the instructive and attentive way she guided me through future articles, comments, criticisms or suggestions.
Report from the EMS Executive Committee Meeting in Stockholm, 18–20 March 2016
Richard Elwes, EMS Publicity Officer
This Spring, the Executive Committee gathered in investments and that financial gains should be reflected Stockholm for a meeting at the historic Institut Mittag- in increases in the budget for scientific activities. At the Leffler of the Royal Swedish Academy of Sciences. To EMS council meeting in July, the treasurer will propose mutual regret, the institute’s director (and former EMS a detailed plan to enact the agreed strategy. President) Ari Laptev was unable to greet the assem- bled company in person. Instead, on Friday evening, the Membership committee enjoyed a short film telling the fascinating The committee expressed regret that the Belgian Sta- story of the institute, which is the oldest mathematics re- tistical Society had cancelled its Class 1 Membership search facility in the world. of the society. Meanwhile, the status of the Armenian Mathematical Union’s application for Class 1 Member- Officers’ Reports ship is unclear. The invitation to present this application The President Pavel Exner welcomed the Executive for approval at the forthcoming council meeting remains Committee to the meeting before relating his recent ac- open. tivities. He reminded the committee of the news that the At the start of 2016, the President wrote to a num- Simons Foundation has decided to support mathematics ber of member societies who have not paid their dues in Africa through the EMS with 50,000 euros per year for several years. The committee expressed sympathy for five years. This development was enthusiastically for the financial difficulties in which learned societies welcomed. may find themselves. However, member societies strug- The treasurer then presented his summary of the gling to pay their dues are expected to contact the EMS budget, income and expenditure of the society for 2015, to negotiate a way forward. The committee agreed that reporting a surplus. The committee then discussed future membership will be terminated for any society who financial strategy. As points of principle, it was agreed neither pay their dues nor respond to letters from the that the society should take a low risk approach to its President.
EMS Newsletter September 2016 3 EMS News
There was also concern about individual members The next society meeting will be the meeting of the who fail to pay their dues promptly, especially when Presidents of Members Societies in Budapest in April these people are active in EMS bodies. The committee (see separate report). agreed to bring a proposal to the council to add to Rule 23 of the by-laws on sub-committee membership the Standing Committees sentence: “Each member should be an individual mem- The Executive Committee agreed to improve the data- ber of the EMS in good standing.” base of past members/chairs of EMS committees (a task, To make membership more appealing to younger it was noted, which may require some time and work to mathematicians, the committee also agreed to propose complete). It then considered reports from the Chairs of to the council a modification of Rule 30 as follows: “Any- the Committees on Applied Mathematics, Developing one who is a student at the time of becoming an indi- Countries, Electronic Publishing, Ethics, European Soli- vidual EMS member, whether PhD or in a more junior darity and Raising Public Awareness of Mathematics. category, shall enjoy a three-year introductory period Following the report from the ERCOM (European with membership fees waived. All the standard benefits Research Centres On Mathematics) Committee, the Ex- will be granted during this time, except printed copies of ecutive Committee was pleased to approve BCAM (the the Newsletter.” Basque Centre for Applied Mathematics in Bilbao) as a The committee was pleased to approve a list of 90 new ERCOM centre. new individual members. It then discussed a proposal for a new lifetime membership, the major question be- Projects ing how to compute a fair fee. The treasurer Mats Gyl- The European Digital Mathematics Library (EuDML) lenberg proposed a formula (due to Euler!) that pur- initiative is progressing at pace, with Volker Mehrmann portedly solves this problem. The Executive Committee to be the EMS representative on the EuDML Board. agreed that Mats Gyllenberg will present his proposal at Volker Mehrmann then reported on the activities the forthcoming council meeting. and the new board make-up of EU-MATHS-IN (the European Service Network of Mathematics for Indus- Scientific Meetings try and Innovation), which is coordinating proposals for The Executive Committee discussed the report from three infrastructure calls. Volker Mehrmann on the preparations for the 7th Euro- pean Congress of Mathematics in Berlin in July. The com- Publicity, Publishing and the Web mittee expressed its sincere appreciation to the local or- The committee discussed the report of the publicity of- ganisers and its confidence in the success of the congress. ficer and plans for a future letter-writing campaign to Over the weekend, the committee heard presenta- increase membership. As stocks of flyers and posters are tions from both bids to host the 8th European Congress now beginning to run low, it was also agreed that a new of Mathematics in 2020, in either Sevilla in Spain or set of publicity materials will be designed and printed Portorož in Slovenia. It was clear that both bids have later in the year or early next year. The committee heard merit and should proceed to the EMS Council in July, from the web team, including a discussion of ways to in- where a final decision will be taken by a simple major- crease the EMS online presence. One possibility is the ity vote. (The Executive Committee will neither issue a incorporation of a blog on the EMS website, perhaps recommendation to the council nor provide evaluation with cooperation from member societies. criteria for the delegates.) The committee continued its contemplation of the The President reported that memoranda of un- future direction of the EMS Publishing House and was derstanding have been signed for the seven Summer pleased to hear that JEMS (the Journal of the EMS) is Schools that will be supported by the EMS in 2016. currently functioning well. In a report on the EMS Newsletter, the committee Society Meetings heard that transition is underway between the outgoing Preparations for the council meeting in Berlin in July are Editor-in-Chief Lucia Di Vizio and her replacement Val- well underway. The committee agreed the draft agenda entin Zagrebnov. The committee again thanked Lucia and heard that the nominations of delegates to repre- Di Vizio for her invaluable work. sent associate, institutional and individual members at A report from Olaf Teschke on Zentralblatt was the council are now closed, with no need for elections. received. The President recalled that Klaus Hulek will Associate members are represented by one delegate replace Gert-Martin Greuel as Editor-in-Chief of Zen- (the maximum permitted), institutional members are tralblatt from April 2016. The President thanked Gert- represented by three delegates (the maximum allowed Martin Greuel for his hard work and offered the opinion is four) and individual members are represented by 25 that Zentralblatt has improved significantly under his delegates (the maximum allowed is 26). One task for the tenure. council will be the replenishment of the Executive Com- mittee, with at least three new officers required. It was Relations with Political and Funding Bodies decided to organise the election in two rounds using an The President reported on the latest developments re- electronic voting system. garding Horizon 2020, notably its running calls, its open
4 EMS Newsletter September 2016 EMS News consultation on mathematics and the installation of the The 2017 EMS-Bernoulli Society Joint Lecture will High Level Group of Scientific Advisors of the EC Sci- be delivered by Alexander Holevo at the 31st European entific Advice Mechanism, with Cédric Villani as a rep- Meeting of Statisticians in Helsinki, 24-28 July 2017. resentative for mathematics. Alice Fialowski presented a report on the activities of The President reported on the latest developments the TICMI (Tbilisi International Centre of Mathematics regarding the new legal status of ISE (the Initiative for and Informatics). The Executive Committee will gather Science in Europe) and reminded the committee that in November in Tblisi and it was agreed that EMS Presi- the membership fee for the EMS is set to double to 3,000 dent Pavel Exner will meet the Director of TICMI. euros. After two years, the Executive Committee will re- Gert-Martin Greuel took the opportunity to adver- evaluate the benefits of ISE membership. The commit- tise the Snapshot series from Oberwolfach on modern tee heard that, in July, Roberto Natalini (Chair of the developments in mathematics, which is aimed at the Committee on Raising Public Awareness) will organise general public (http://www.mfo.de/math-in-public/snap- a session at ESOF (EuroScience Open Forum) in Man- shots). chester, UK, about Alan Turing, in which the EMS Pub- The committee was delighted to hear that agree- licity Officer Richard Elwes will also participate. Mean- ments for collaboration and reciprocity membership while, the President is also involved in an ESOF session have been signed between EMS and the Mathematical about the ERC. Society of Japan (MSJ). The committee then considered The committee regretted that attempts to secure the possibility of holding a joint meeting. funding for EMS Summer Schools from the COST programme were not successful. It was suggested that Other Business prospects for funding EMS activities through this pro- The Executive Committee was alarmed at developments gramme may generally be poor. in Turkey, which have seen a colleague imprisoned for The committee was delighted to hear that there will signing the Academics for Peace petition. It was decided be a mathematics session at the World Economic Forum to write letters of concern to the Turkish prime minister in Davos and considered what input the EMS might and to the President of the European Parliament, and make. to follow developments closely. Copies of these letters were sent to our sister organisations at the European Relations with Mathematical Organisations level and to the Presidents of our Member Societies. The committee discussed news from the IMU, the ICIAM and other mathematical bodies. It then con- Conclusion gratulated Andrew Wiles for his Abel Prize. Following a The committee expressed its gratitude to the Insti- long tradition, EMS Vice-President Martin Raussen will tut Mittag-Leffler and, in absentia, to its director Ari interview the Abel Prize winner in May but confirmed Laptev, for the magnificent hospitality it enjoyed over that this will be his last year doing so. the weekend.
Report on the Meeting of Presidents of Mathematical Societies in Budapest, 2–3 April 2016
Sjoerd Verduyn Lunel, Secretary of the EMS, and Richard Elwes, EMS Publicity Officer
Pavel Exner, President of the European Mathematical EMS Business Society and Chair of the meeting, opened proceedings Pavel Exner gently reminded the assembled company of by greeting everyone present and thanking our hosts, the the importance of member societies and individuals pay- Alfred Rényi Institute of Mathematics of the Hungar- ing their dues on time. (If they have difficulty doing so, ian Academy of Sciences. After a Tour De Table in which they should get in touch with the EMS directly to negoti- the guests introduced themselves and their Society, Gy- ate an arrangement.) ula Katona, President of the János Bolyai Mathematical The Chair reported on the EMS’s wide range of sci- Society delivered a presentation on its fascinating history entific activities, and encouraged member societies to as well as its current activities. prepare proposals for scientific activities, such as Joint
EMS Newsletter September 2016 5 EMS News
Mathematical Weekends. (Proposals for 2017 can be sub- sessment (PISA) survey, mathematics curricula are un- mitted via the EMS website.) dergoing transformations in many countries. The meet- After discussing the work of the EMS’s eleven Stand- ing agreed that is vital to exchange information about ing Committees, he spoke about its online presence, a this changing landscape. major way of keeping in contact with members and the In Germany, a catalogue has been compiled of the broader mathematical community. He encouraged mem- minimal requirements that students should meet when ber societies to get involved, and to contact Richard El- finishing secondary school, to study engineering or natu- wes, Publicity Officer of the EMS, with any new ideas in ral sciences. Of course, its contents are controversial. The this area. meeting considered whether the EMS Education Com- mittee might play a role in drafting standards of this kind, Presentations which could then be used as guidelines in national dis- The meeting then heard a number of presentations: cussions. A number of presidents recommended becom- - Volker Bach described progress towards the 7th ECM ing directly, personally involved in national curriculum (Berlin, 18–22 July 2016) committees. - Betül Tanbay, member of the EMS Ethics Committee, Another area of significant difference between coun- reported on its work on the application of the EMS tries is that of teacher training. In some countries, this is Code of Practice and towards a new edition of the completely separate from standard university education. Code in due course. She welcomed comments and sug- In other countries, there are multiple tracks to become a gestions for additional areas to be addressed, for ex- teacher, via a university degree or via a teacher training ample, regarding unethical behaviour with respect to school. In some countries there are special schemes to ‘open access’ publications. support a later career change into teaching. There was a - Waclaw Marzantowicz, President of the Polish Math- general agreement that the Education Committee should ematical Society, reported on its recently established become more directly involved with issues of mathemat- Mathematical Information Service. ics education at secondary school, curriculum planning, - Mercedes Siles Molina, Vice-President of the Royal and teacher training. It is also recommended that the Spanish Mathematical Society (RSME), described Education Committee should work with the EMS spon- connections between RSME and the mathematical so- sored EuroMath initiative, aimed at students between 9 cieties of South America. She stressed that the RSME and 18. (See www.euromath.org.) is keen to facilitate further mathematical interactions between Europe (via the EMS and its member socie- Other Business ties) and South America. The Chair discussed the political situation in Turkey - The rival bids for hosting the 8th ECM in 2020 were where a colleague was imprisoned for signing the Aca- presented, with Klavdija Kutnar presenting the bid for demics For Peace petition. He reported that he had writ- Portorož, Slovenia, and Juan González-Meneses pre- ten letters of concern, on behalf of the European Math- senting that for Sevilla, Spain. ematical Society, to the Turkish prime minister and to the President of the European Parliament. The meeting was Discussion on Mathematical Education unanimously supportive of this initiative. It was agreed to The meeting then held an open discussion of Math- follow developments closely and also to investigate what ematical Education. A focus was the balance between steps might be taken at a national level to express the challenging ‘gifted’ students on one hand, and, on the strong concern of our community about the situation. other, attaining a decent level for all students enrolled on mathematics courses. This latter group is increasing Closing in size, because of the need for mathematical skills in On behalf of all participants, the Chair thanked the local subjects such as engineering and natural sciences. Ap- organizers for their excellent preparations, and for the proaches vary from country to country. For example, generous hospitality offered by the Alfred Rényi Insti- Hungary and Romania have special programs for gifted tute of Mathematics of the Hungarian Academy of Sci- students. However, these countries also feel the effects of ences. ‘brain drain’, with many high-achieving students opting The next meeting of Presidents of Mathematical Soci- to study abroad after high school. eties will be held in the Spring of 2017 in Lisbon, hosted With this shifting balance, and also as a consequence by the Portuguese Mathematical Society. of the OECD Programme for International Student As-
6 EMS Newsletter September 2016 News 2016 Kamil Duszenko Prize Goes to Kate Juschenko
Kate Juschenko of Northwestern acting on the Cantor set. To a homeomorphism T of the University has been named the re- Cantor set one associates the topological full group [[T]] cipient of the 2016 Kamil Dusze- consisting of homeomorphism piecewise given by pow- nko Award, awarded for outstand- ers of T. Matui showed that for suitably chosen T the ing research in Geometric Group commutator subgroup of [[T]] is finitely generated and Theory. simple. Juschenko and Monod proved that these groups Kate Juschenko got her PhD in are also amenable, thus providing the first examples of 2011 at Texas A& M. Her advisor finitely generated amenable simple groups. Later, with was Gilles Pisier. She held posi- Nekrashevych and de la Salle she extended this result tions at EPFL, Vanderbilt University and CNRS. She has and devised a new method of proving amenability, set- been at Northwestern University since 2013. tling some open cases and unifying many known ones. Kate Juschenko started her mathematical education Moreover, Juschenko found a powerful method to dem- and work in Ukraine. She was then interested in opera- onstrate that many groups acting on trees are not ele- tor algebras, and participated in exploring the notion and mentary amenable. providing examples of *-wild C*-algebras. She was also The Kamil Duszenko Award has been set up in mem- engaged in investigating multi-dimensional Schur mul- ory of an outstanding young mathematician who died in tilpiers for C*-algebras. 2014 of acute lymphoblastic leukaemia at the age of 28. Her work connected to geometric group theory is The webpage with more information is concentrated on the notion of amenability. She was able (with various coauthors) to deeply explore it for groups http://kamil.math.uni.wroc.pl/en/mathematics/about/
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EMS Newsletter September 2016 7 Feature Elliptic Functions Functions According According to to Eisenstein and and Kronecker: Kronecker: An An Update Update Newly found notes of lectures by Kronecker Newly found notes of lectures by Kronecker on the work of Eisenstein Pierre Charollois (Université Paris 6, France) and Robert Sczech (Rutgers University, Newark, USA) Pierre Charollois (Université Paris 6, France) and Robert Sczech (Rutgers University, Newark, USA)
This article introduces a set of recently discovered lecture notes from the last course of Leopold Kronecker, delivered a few weeks before his death in December 1891. The notes, written by F. von Dalwigk, elaborate on the late recognition by Kronecker of the importance of the “Eisenstein summation process”, invented by the “companion of his youth” in order to deal with conditionally convergent series that are known today as Eisenstein series. We take this opportunity to give a brief update of the well known book by André Weil (1976) that brought these results of Eisenstein and Kronecker back to light. We believe that Eisenstein’s approach to the theory of elliptic functions was in fact a very important part of Kro- necker’s planned proof of his visionary “Jugendtraum”. Gotthold Eisenstein (1823–1852) and Leopold Kronecker (1823–1891) (left to right) 1 Introduction
Born in 1823, Leopold Kronecker died in Berlin on 29 De- with many appendices, partly written by von Dalwigk, relying cember 18911 at the age of 68, precisely 15 days after deliver- on published papers of Kronecker as well as unpublished pa- ing the last lecture of his university course entitled “On ellip- pers from Kronecker’s “Nachlass”. Dalwigk explicitly men- tic functions depending on two pairs of real variables”. This tions the word “Nachlass” in the manuscript. He is likely to historical information was gathered from recently discovered have had access to that specific document from his colleague lecture notes at the library of the University of Saarbrücken. Hensel in Marburg, who was in possession of all the scientific Before discussing the content and the author of these hand- papers of Kronecker at the time. As we learned from Hasse written notes, we wish to recall the circumstances of their and Edwards [Ed], the personal papers of Kronecker were lost discovery. The original discovery is due to Professor Franz in the chaotic events surrounding World War II. Most proba- Lemmermeyer, who started but did not finish the task of re- bly, they were destroyed by a fire caused by exploding muni- typing the text written in old style German cursive handwrit- tions in an old mine near Göttingen. That mine was used to ing. The manuscript then got lost during a library move. Being store some of the collections of the Göttingen Library in 1945. interested to learn more about Kronecker’s work and gain in- This dramatic event is only part of the long-lasting spell put sight into his so-called “liebster Jugendtraum”, we decided to on the posterity of Eisenstein’s ideas, as predicted by André enlist the help of Simone Schulze at the library in finding it. Weil in his essay [We1]. After a search effort which lasted a few weeks, the complete At any rate, the care and the amount of detail included in set of notes was finally found and the library even produced a the manuscript is extraordinary and leads us to think that it high quality digital copy, which is now available to the public was written with the ultimate intention to publish it as a book. [Cw]. We thank Ms Schulze for her help and we also thank We know from a letter of Kronecker to his friend Georg Franz-Josef Rosselli, who undertook the effort to translate the Cantor, who was the first president of the newly founded Ger- cursive German handwriting (prevailing in the 19th century) man Mathematical Association (DMV) and who invited Kro- into modern German typeface [Cw]. necker to deliver the opening address at the first annual meet- The manuscript was written by Friedrich von Dalwigk, a ing of the DMV in 1891, that Kronecker intended to talk at graduate student at the time, who was just finishing his dis- that meeting about the “forgotten” work of Eisenstein. In that sertation on theta functions of many variables [vD]. Later, letter, Kronecker apologises for not being able to attend the von Dalwigk became a professor of applied mathematics at meeting due to the death of his wife Fanni. It is very likely the University of Marburg (1897–1923). Although the course that the lecture notes in question are an expanded version of only consisted of six lectures (due to the premature death of his intended talk. Kronecker), the whole manuscript is more than 120 pages, Kronecker was indeed a great mathematician who made fundamental contributions to algebra and number theory. We 1 According to the tombstone on his grave, Kronecker died on 23 Decem- mention here only his “Jugendtraum”, which, historically, ber 1891. gave rise to class field theory and to Hilbert’s 12th prob-
8 EMS Newsletter September 2016 Feature lem (the analytic generation of all abelian extensions of a Following Eisenstein, we define given number field), one of the great outstanding problems 1 1 ∞ 1 1 in classical algebraic number theory. The celebrated conjec- φ(u) = lim = + + t + m u u + n u n tures of Stark (published in a sequence of four papers during → ∞ m Z+u, n=1 − ∈m EMS Newsletter September 2016 9 Feature and its Cayley transform relates φ(u,ξ) to the Eisenstein function φ. The right side c(u) + i of Equation (4) is essentially the generating function for the e(u) = . c(u) i Bernoulli polynomials. Expanding the left side into a power − series in u, one obtains the Fourier expansion of the Bernoulli The addition formula (2) immediately implies polynomials. The above proof of the addition formula for the e(u)e(v) = e(u + v). cotangent function applies to φ(u,ξ) as well and yields addi- From here, it follows that e(u) = e2πiu and c(u) = cot(πu). tion formulas for the Bernoulli polynomials. Due to the fac- Iterating the addition formula for the cotangent function, i.e. tor e( nξ) in the numerator, the convergence of this series is − c(u)c(v) 1 slightly better than that of the cotangent series but is still con- c(u + v) = − , ditional. A substantial part of the lecture notes is devoted to c(u) + c(v) the study of the elliptic analogue of (4), written in Kronecker’s we obtain the formula notation, Un c(u) c(nu) = , n = 1, 2, 3, 4,..., (3) N M V c(u) e( mξ + nη) n Ser (ξ, η, u,τ) = lim lim − , (5) N + M + u + nτ + m with polynomials Un, Vn Z[t] given explicitly by → ∞ → ∞ n= N m= M ∈ − − n n Un(t) = Re (t + i) , Vn(t) = Im (t + i) . where ξ, η is a pair of real variables and τ is a point in the A formula of type (3) was called a “transformation formula” upper half space. The complex variable u must be restricted to Z + τZ C. = στ + ρ in the 19th century. The elliptic analogues of (3) played a the complement of the lattice in Writing u τ ffi σ, ρ, prominent role in the work of Kronecker. Taking u Q with as a linear combination of and 1 with real coe cients ∈ denominator n > 1, we conclude that the numbers c(u) are this series can be viewed as a function of two pairs of real variables (ξ, η), (σ, ρ), the ones referred to in the title of the the roots of Vn(t) = 0, that is, c(u) is a real algebraic number whenever u is a non-integral rational number. One can refine lecture notes. this result and give a more precise proof: Various alternative ways to sum the conditionally conver- gent series (5) are discussed in the manuscript. It is a remark- Proposition 2.2. The number c(u) is an algebraic integer if able fact that, in all cases, the value obtained for the sum is and only if n is not the power of an odd prime. If n = pk, with independent of the limiting process chosen. Kronecker’s main an odd prime p and k > 0, then pc(u) is an algebraic integer. result expresses these series in terms of Jacobi theta series. Let Moreover, c(u) is a unit if and only if neither n nor n/2isa n2τ 1 power of an odd prime. ϑ(z,τ) = ϑ (z,τ) = e + n z 1 2 − 2 n Z+ 1 Theorem 2.3 (Kronecker-Weber). The set of real numbers ∈2 1 n n n c(Q Z) generates the real subfield of the maximal abelian = 2 q 8 sin(πz) (1 q ) 1 q e(z) 1 q e( z) , \ − − − − extension of Q. n 1 ≥ Kronecker was interested in generalising these results to with a complex variable z, a point τ in the upper half plane the case of elliptic functions with period lattice being an ideal and q = e(τ). ffi in an imaginary quadratic field. One of the di culties he faced Theorem 2.4 (Kronecker). Suppose 0 < Im u < Im τ and was that the addition formula for elliptic functions is in gen- 0 <ξ<1. Then, eral algebraic and not rational, as in the case of the cotangent ϑ(0,τ)ϑ(u + η + ξτ, τ) function. To the best of our knowledge, the proof of the Ju- Ser (ξ, η, u,τ) = e(ξu) . (6) gendtraum as envisioned by Kronecker has never been com- ϑ(u,τ)ϑ(η + ξτ, τ) pleted.2 Except for the case of imaginary quadratic fields and This result is reminiscent of the so-called limit formula the case of the rational number field (both closely related of Kronecker, which is not discussed in the lecture notes but to the work of Kronecker), we do not even know whether deserves to be stated here: let τ, τ be two complex numbers Hilbert’s 12th problem has a solution. This is partly related to with Im τ>0 and Im τ < 0 and let 0 ξ, η < 1 be two ≤ a classical theorem of Weierstrass asserting that every mero- real numbers, not both equal to zero. Writing u = η ξτ, v = − morphic function with algebraic addition law is either elliptic, η ξτ, the second limit formula is the identity circular or rational. − (τ τ) e(mξ + nη) Instead of the series defining φ(u), Kronecker preferred to − π τ + τ + study the more general series 2 i , (m n)(m n) m n 2 ∞ e( nξ) e(ξu) ϑ(u,τ)ϑ(v, τ) (u v) φ(u,ξ) = − = 2πi , 0 <ξ<1, (4) = log − πi − , (7) + − η(τ)η( τ ) − τ τ n= u n e(u) 1 −∞ − − − where u is again a complex number that is not an integer. The where η(τ) refers to the Dedekind eta function and the term introduction of the second variable ξ is very natural and is (m, n) = (0, 0) needs to be excluded from the sum. Again, con- suggested by Fourier analysis. Note that the limiting case vergence is only conditional so a specific order of summation as in (5) needs to be observed. lim φ(u,ξ) = φ(u) iπ ξ 0 − Historically, the notion of complex multiplication of ellip- → ξ>0 tic functions appeared for the first time in the work of Abel. Pages 64–67 of Kronecker’s lecture notes are devoted to the 2 See the comment linked to interpretation (c) in [HH]. task of expressing the elliptic functions used by Abel in terms 10 EMS Newsletter September 2016 Feature of the Kronecker series Ser(ξ, η, u,τ). This is perhaps one of Given a pair of integers a 0, b > 0 and z , w C, the ≥ 0 0 ∈ the highlights of the manuscript and deserves special atten- Eisenstein–Kronecker numbers are defined as tion. It is very likely that Kronecker’s conception of the Ju- e∗ (z , w ,τ) = K∗ (z , w , b,τ). gendtraum was the result of a close study of the work of Abel. a,b 0 0 a+b 0 0 When b > a + 2, these numbers include, in particular, the 3 Recent developments values of the absolutely convergent partial Hecke L-series a λ It would be wise to leave the complete discussion of the e∗ (0, 0,τ) = , a,b λb legacy of Eisenstein or Kronecker to serious historians. We λ Z+τZ ∈ offer, instead, a brief survey of several recent developments which should be considered as elliptic analogues of the that feature Eisenstein’s summation process and Kronecker’s Bernoulli numbers. As such, the Eisenstein–Kronecker num- Theorem 2.4 for the series Ser (ξ, η, u,τ) bers can be packaged into a generating series that is the ellip- tic analogue of the cotangent function and its relative φ(u,ξ). Algebraicity and p-adic interpolation of To obtain the nice two-variables generating series, it is enough Eisenstein–Kronecker numbers to translate and slightly alter the Kronecker theta function in It was already observed by Weil in his 1976 book that the order to define combination of the methods of Eisenstein and Kronecker (z0+z)w0+wz0 A gives direct access to Damerell’s classical result (1971) on Θz0,w0 (z, w) = e− Θ(z0 + z, w0 + w). the algebraicity of values of L-functions attached to a Hecke Its Laurent expansion around z = w = 0 displays exactly the Grössencharakter of an imaginary quadratic field. collection of Eisenstein–Kronecker numbers. Weil also anticipated that their methods would extend to Proposition 3.1. Fix z , w C. We have the following Lau- the investigation of the p-adic properties of these algebraic 0 0 ∈ numbers. In the following 10 years, the works of Manin- rent expansion near z = w = 0: Visik,˘ Katz and Yager among others provided the expected δ(z0) δ(w0) p-adic interpolation of this family of special values. To give a Θ , (z, w) = ψ(w z ) + z0 w0 0 0 z w taste of the results in question, we wish to introduce a recent e∗ (z , w ,τ) a+b 1 a,b 0 0 b 1 a work by Bannai-Kobayashi (2010), based on Kronecker’s se- + ( 1) − z − w , (9) − a!Aa ries, that enables a similar construction. a 0,b>0 Our first task is to connect the series Ser to a series that ≥ where δ(u) = 1 if u Λ and 0 otherwise. includes an s-parameter pertaining to the style of Hecke. Let ∈ Imτ τ be a complex number in the upper half plane and let A = π If, in addition, τ is a CM point and z0, w0 are torsion points be the area of the fundamental domain of the lattice Λ=Z + over the lattice Λ then these coefficients are algebraic. z z τZ divided by π. Let ψ be the character ψ(z) = e −A . For a 0 ≥ Theorem 3.2. Let Λ=Z + τZ be a lattice in C. Assume that an integer, we introduce the Kronecker-Eisenstein series as the complex torus C/Λ has complex multiplication by the ring ∗ (z + λ)a of integers of an imaginary quadratic field k, and possesses a Ka∗(z, w, s,τ) = ψ(zw), Re(s) > a/2 + 1, 2 3 z + λ 2s Weierstrass model E : y = 4x g2 x g3 defined over a λ Λ | | − − ∈ number field F. Fix N > 1 an integer. For z0, w0, two complex where the means that the summation excludes λ = z ∗ − numbers such that Nz0, Nw0 Λ, the Laurent expansion in (9) if z Λ. It is a continuous function of the parameters ∈ 2 ∈ has coefficients in the number field F(E[4N ]). In particular, z C Λ, w C and it has meromorphic continuation to ∈ \ ∈ the rescaled Eisenstein–Kronecker numbers the whole s-plane, with possible poles only at s = 0 (if a = 0 a and z Λ) and s = 1 (if a = 0 and w Λ). Moreover, it sat- ea∗,b(z0, w0,τ)/A ∈ ∈ isfies a functional equation relating the value at s to the value are algebraic. at a + 1 s. Write w = η + ξτ with real variables ξ, η and ab- − We refer to [BK], Th. 1 and Cor. 2.11 for the proofs. The breviate the central value K1∗(z, w, 1,τ) by K(z, w) when there is no ambiguity on the lattice. This specific function is related above construction enables Bannai and Kobayashi to recover to Kronecker’s series by the identity Damerell’s result along the way. Let p be a prime number. Bernoulli numbers and Bernoulli , = , , ,τ = ξ, η, ,τ , K(z w) K1∗(z w 1 ) Ser ( z ) polynomials satisfy a whole collection of congruences mod- where w = η + ξτ, at least if z, w Λ, using [We1, §5, p. 72]. ulo powers of p, known as “Kummer congruences". These In this new set of notations, Theorem 2.4 can be restated as congruences are incorporated in the construction of the Kubota- Leopoldt p-adic zeta function ζ (s), s Z , which interpo- K(z, w) = ezw/A Θ(z, w), p ∈ p lates the values of the Riemann zeta function at negative inte- where gers, as given by the Bernoulli numbers. ϑ(0,τ)ϑ(z + w,τ) Θ(z, w) = (8) Similarly, Eisenstein–Kronecker numbers satisfy a col- ϑ(z,τ)ϑ(w,τ) lection of congruences that are the building blocks for the denotes the meromorphic function appearing as the ratio in construction of p-adic L-functions of two-variables. Since Equation (6). It will play a major role in the remainder of this Bannai-Kobayashi also have a generating series at their dis- text so we name it the “Kronecker theta function”, in agree- posal, they can interpolate the Eisenstein–Kronecker numbers ment with the terminology in [BK]. p-adically, not only when p splits in k, like in the work of Katz EMS Newsletter September 2016 11 Feature (ordinary case), but also when p is inert in k (supersingular coefficients in the number field generated by the Fourier co- case). efficients of f. As a consequence, for each integer k > 0, the It seems appropriate to remark in passing that in this p- finite sum adic setting, the Kronecker limit formula (7) also has a coun- 1 Ccusp(X, Y,τ) = R (X, Y) f (τ) terpart. It has been originally obtained by Katz (1976) and k (k 2)! f f cusp proved to be crucial in the study of Euler systems attached to − ∈Bk elliptic units. belongs to Q[X, Y][[q]]. Zagier starts to complete this cus- To complete this p-adic picture and set the stage for a re- pidal term by a contribution that arises from the Eisenstein curring theme for sections to come, we would like to men- series in Mk, using the following convenient recipe. For any tion a generalisation by Colmez-Schneps [CS] of the above even k > 0, let Bk be the usual k-th Bernoulli number and let construction of Manin-Visik˘ and Katz. Colmez and Schneps 2k k 1 m E (τ) = 1 d − q consider the case where the Hecke character is attached to an k − B k m 1 d m extension F of degree n over the imaginary quadratic field k ≥ | n = F be the normalised weight k Eisenstein series for SL2(Z). Its (the previous setting thus corresponds to 1). The field 1 might not necessarily be a CM field. Building on the tech- pair of period functions in X− Q[X] is defined by the odd (and niques of [Co], they can construct a p-adic L-function for F even) rational fractions by interpolating the algebraic numbers arising from the Lau- k od Bh Bk h h 1 ev k 2 r (X) = − X − , r (X) = X − 1 rent expansion of certain linear combinations of products of Ek h! (k h)! Ek − n generating series of Kronecker’s type, each of them being h=0 − evaluated at torsion points over the lattice Λ. The juxtaposi- and they make up the contribution of Eisenstein series by the tion of n copies of Proposition 3.1-Theorem 3.2 allows them rule Eis ev od od ev to bootstrap the case n = 1 to arbitrary n 1 using their C (X, Y,τ) = r (X)r (Y) + r (X)r (Y) Ek(τ). ≥ k Ek Ek Ek Ek identity [CS, Eq. (31)]. − The main identity of Zagier then establishes a remarkable closed formula for the generating series Periods of Hecke eigenforms + ∞ Let (z0, w0) be a fixed pair of N-torsion points over the lat- (X Y)(XY 1) cusp Eis k 2 Cτ(X, Y, T) = − + (C + C )T − , Λ. τ X2Y2T 2 k k tice As functions of the variable, the modular forms k=2 e (z , w ,τ) are Eisenstein series for the principal congru- a∗,b 0 0 which factorises as a product of two Kronecker theta func- Γ . ence subgroup (N) In particular, the Laurent expansion (9) tions: for the translated Kronecker theta function at z = w = 0 is a 2 generating series for Eisenstein series of increasing weight Theorem 3.3 (Zagier [Za1]). In (XYT)− Q[X, Y][[q, T]], we and fixed level. Its decomposition under the action of the have 2 Hecke algebra thus possesses only Eisenstein components. Cτ(X, Y, T) =Θ(XT, YT) Θ(T , XYT)/ω , (10) From this perspective, interesting new phenomena start to ap- − where ω = 2πi, T = T/ω. pear when one considers a product of two Kronecker theta functions. Equation (10) shows that complete information on Hecke Such a product encodes all period polynomials of modular eigenforms of any desired weight for SL2(Z) and their period forms of all weights, at least in the level one case.3 This is the polynomial is encoded in the Laurent expansion at T = 0 of content of the main result of Zagier’s paper [Za1], which we the right side. To further support that claim, Zagier explains now describe. in the sequel paper [Za2] how to deduce from Equation (10) Let Mk be the C-vector space of modular forms of weight an elementary proof of the Eichler-Selberg formula for traces k 4 on SL (Z) and let Sk Mk be the subspace of cusp of Hecke operators on SL (Z). ≥ 2 ⊂ 2 forms, equipped with the Petersson scalar product ( f, g) and The period polynomials satisfy a collection of linear rela- cusp its basis of normalised Hecke eigenforms . The period tions under the action of SL (Z). These cocycle relations are Bk 2 polynomial attached to f S k is the polynomial of degree reflected using Equation (10) by relations satisfied by Kro- ∈ k 2 defined by necker’s theta functions, e.g., [Za1, p. 461]. A typical exam- ≤ − i ple is ∞ k 2 r f (X) = f (τ)(τ X) − dτ. 0 − 1 1 Cτ(X, Y, T) + Cτ 1 , Y, TX + Cτ , Y, T(1 X) = 0, − X 1 X − The Eichler-Shimura-Manin theory implies that the maps − f rev and f rod assigning to f the even and the odd (11) → f → f which is the counterpart of the classical relation for the period part of r f are both injective. Moreover, if f is a normalised Hecke eigenform then the two-variables polynomial polynomial ev od od ev 2 1 1 r f (X)r f (Y) + r f (X)r f (Y) r f 1 + U + U = 0, U = − . R (X, Y) = C[X, Y] | 10 f (2i)k 3( f, f ) ∈ − In the remainder of this paper, we explain how the method of transforms under σ Gal(C/Q) as R = σ(R ), so R has ∈ σ( f ) f f Eisenstein–Schellbach, when properly modulated, is the ade- quate tool to produce systematically general (n 1)-cocycle − 3 A very recent preprint [CPZ] indicates that a similar result also holds for relations for GLn(Z) involving products of n Kronecker theta arbitrary squarefree level. functions, including Equation (11) as a very special case. 12 EMS Newsletter September 2016 Feature Trigonometric cocycles on GLn where the role of the function φ(u,ξ) is now played by Kro- Let 0 < a, b < 1 be rational numbers and x, y C Z be necker’s theta function. It will make it clear that the trigono- ∈ \ complex parameters. We use the shorthand 0 < t < 1 for the metric relations we have encountered so far are a specialisa- { } fractional part of a non-integral real number t. From a direct tion of the elliptic ones when q 0, i.e. τ i . → → ∞ computation or a mild generalisation of Lemma 2.1, one de- Kronecker has not been given the opportunity to imple- duces the following relation, which amounts to the addition ment the Eisenstein–Schellbach method in his own elliptic formula for the function φ(u,ξ): investigations. Let us now proceed by fixing τ in the upper half-plane and first perform in Equation (12) the change of e(xa)e(yb) e (x + y)a e y b a { − } variables e(x) 1 e(y) 1 − e(x + y) 1 e(y) 1 − − − − e (x + y)b e x a b x nτ + x, { − } = 0. (12) ← − e(x + y) 1 e(x) 1 y nτ + y. − − ← As pointed out by the second author in [Scz2], this iden- tity can naturally be recast in terms of the cohomology of We also aim to twist that equation by a pair of roots of unity e(nr)e(n s) with r, s Q and then sum over n, n Z. We the group SL2(Z). The building blocks are products of two ∈ ∈ copies of the trigonometric function φ(u,ξ). Given two pairs write x0 = aτ + r, y0 = bτ + s, q = e(τ) so that the real and t x, x , y, y u = (u1, u2) and ξ = (ξ1,ξ2) , we set imaginary parts of 0 0 make up four pairs of real vari- ables. The first summand becomes Φ(u,ξ) = φ(u1,ξ1)φ(u2,ξ2). na n b To any matrix A = ab SL (Z) is associated σ = 1 a e(nr)q q e(n s) cd ∈ 2 0 c ∈ S := e(xa)e(yb) . Z qn x qn y M2( ). If c 0, we define n,n Z e( ) 1 e( ) 1 ∈ − − ab 1 Ψ (u,ξ) = sign(c) Φ(uσ, σ− (µ + ξ)). a cd The assumption 0 < a < 1 ensures that 1 > q > q , and µ Z2/σZ2 b | | | | ∈ similarly for q , so that this double series is absolutely con- If c = 0 then Ψ(A)(u,ξ) = 0 by definition. The next proposi- vergent. The sum S naturally splits as a product, whose value tion stands for the case n = 2 of a more general (n 1)-cocycle is deduced from two consecutive uses of Kronecker’s Theo- − relation for the group GLn(Z) obtained in [Scz3, Cor. p. 598]. rem 2.4: Proposition 3.4. Let A, B SL (Z) be two matrices. For any S = e(xa)e(yb) Θ(x, x0) Θ(y, y0). ∈ 2 u in a dense open domain in C2 and any non-zero ξ Q2, the ∈ following inhomogenous 1-cocycle relation holds: A similar resummation process can be performed on the sec- 1 ond term and the third term of Equation (12). After simplifi- Ψ(AB)(u,ξ) Ψ(A)(u,ξ) Ψ(B)(uA, A− ξ) = 0. − − cation by the common factor e(xa+yb), we obtain the identity The addition law (12) corresponds to the choice of matri- 0 1 11 ces A = and B = in this proposition. Θ(x, x0)Θ(y, y0) Θ(x + y, x0)Θ(y, y0 x0) 10− 10 − − The coefficients of the− Laurent expansion at u = 0 of the Θ(x + y, y0)Θ(x, x0 y0) = 0, (13) general (n 1)-cocycle Ψ carry a great deal of arithmetic infor- − − − mation. According to the main result of [Scz3, Th. 1], the pair- which can be extended analytically to remove the restrictive ing of Ψ with an (n 1)-cycle, built out of the abelian group assumptions made on the parameters. Equation (13) is just an- − generated by the fundamental units of a totally real number other form of the Riemann theta addition relation, also known field F of degree n, produces the values ζF (k) at non-positive as the Fay trisecant identity. It simultaneously implies Equa- integers k of the Dedekind zeta function of F and thereby es- tion (12) when τ i and Equation (11) under the choice of → ∞ tablishes their rationality. This provides a new proof, deeply parameters x = XT , x = YT , y = T , y = XYT . 0 − 0 rooted in the Eisenstein–Schellbach method, of the Klingen– More generally, the resummation of the trigonometric Siegel rationality result. (n 1)-cocycle Ψ gives rise to an elliptic (n 1)-cocycle that − − An integral avatar of the cocycle Ψ was later introduced we name the Eisenstein–Kronecker cocycle κ on GLn(Z). One by Charollois and Dasgupta to study the integrality proper- recovers Ψ from κ by letting τ i . The coefficients of the → ∞ ties of the values ζF (k), enabling them to deduce a new con- Laurent expansion of κ at zero now display modular forms, struction of the p-adic L-functions of Cassou–Noguès and essentially sums of products of n Eisenstein series of various Deligne–Ribet. weights and levels, that are members of a compatible p-adic Combining their cohomological construction with the re- family. cent work of Spiess, they also show in [CD] that the order of When paired with a (n 1)-cycle built out of the funda- − vanishing of these p-adic L-functions at s = 0 is at least equal mental units of a totally real number field F of degree n, the to the expected one, as conjectured by Gross. This result was elliptic cocycle κ produces a generating series for the pull- already known from Wiles’ proof of the Iwasawa Main Con- backs of Hecke–Eisenstein series over the Hilbert modular jecture. group SL ( ), whose constant terms are the values ζ (k) at 2 OF F negative integers k 0. These classical modular forms have ≤ On elliptic functions depending on four pairs of real already played a prominent role in the original proof by Siegel variables of the Klingen–Siegel theorem. More details on the construc- Our goal in this last section is to propose a q-deformation of tion of the Eisenstein–Kronecker cocycle κ and its properties the trigonometric cocycle Ψ to construct an elliptic cocycle, will be given in [Ch]. EMS Newsletter September 2016 13 Feature References [Scha] N. Schappacher. On the history of Hilbert’s twelfth prob- lem. in Matériaux pour l’histoire des mathématiques au [BK] K. Bannai, S. Kobayashi. Algebraic theta functions and XXème siècle, Nice 1996. SMF, Paris (1998) 243–273. the p-adic interpolation of Eisenstein–Kronecker numbers. [Sche] K. H. Schellbach. Die einfachsten periodischen Funktio- Duke Math. J. 153 no. 2 (2010) 229–295. nen. J. Reine Angew. Math. 48 (1854), 207–236. [Cw] P. Charollois. Professional webpage: https: [Scz1] R. Sczech. Dedekindsummen mit elliptischen Funktionen. //webusers.imj-prg.fr/~pierre.charollois/Kronecker.html. Invent. Math. 76 (1984), 523–551. Eventually these documents should be available on the [Scz2] R. Sczech. Eisenstein group cocycles for GL2(Q) and val- arXiv. ues of L-functions in real quadratic fields. Comment. Math. [Ch] P. Charollois. The Eisenstein–Kronecker cocycle on GLn. Helv. 67 (1992), 363–382. In preparation. [Scz3] R. Sczech. Eisenstein group cocycles for GLn and values [CD] P. Charollois, S. Dasgupta. Integral Eisenstein cocycles on of L-functions. Invent. Math. 113 (1993), no. 3, 581–616. GLn, I: Sczech’s cocycle and p-adic L-functions of totally [Si] C. L. Siegel. Advanced Analytic Number Theory. Tata In- real fields. Cambridge J. of Math. 2 no.1 (2014), 49–90. stitute of Fundamental Research, Bombay: 1980. [CPZ] Y. Choie, Y. K. Park, D. Zagier. Periods of modular [V] S. G. Vladut.˘ Kronecker’s Jugendtraum and modular func- forms on Γ0(N) and products of Jacobi theta functions. tions. Translated from Russian by M. Tsfasman. Studies in Preprint (2016), available at http://people.mpim-bonn. the Dev. of Modern Math 2, Gordon and Breach Sc. Pub., mpg.de/zagier/files/tex/CPZ/PERIODS.pdf. New-York, 1991. [Co] P. Colmez. Algébricité de valeurs spéciales de fonctions L. [We1] A. Weil. Book review: Gotthold Eisenstein, Mathematis- Invent. Math. 95 (1989), 161-205. che Werke. Bulletin of the AMS 82, vol. 5 (1976), 658– [CS] P. Colmez, L. Schneps. p-adic interpolation of special val- 663. (and Oeuvres Sc., vol. III, [1976c], 368-403). Also ues of Hecke L-functions. Compositio Math. 82 (1992), included as a Foreword to Gotthold Eisenstein’s Mathema- 143-187. tische Werke in 2nd Edition, Chelsea Pub. Comp., 1989, p. [vD] F. von Dalwigk. Beiträge zur Theorie de Thetafunktionen V-XI. von p Variablen. Dissertation, Halle (1891). [We2] A. Weil. Elliptic functions according to Eisenstein and [Ed] H. M. Edwards. On the Kronecker Nachlass. Historia Kronecker. 2nd Edition, Classics in Math. Springer-Verlag, Mathematica 5 (1978), 419–426. Berlin, 1999. (1st Edition 1976.) [Eis1] G. Eisenstein. Bemerkungen zu den elliptischen und [Za1] D. Zagier. Periods of modular forms and Jacobi theta func- Abelschen Transcendenten. J. Reine Angew. Math. 27 tions. Invent. Math. 104 (1991), 449–465. (1844) 185–191 (and Math. Werke I, p. 28–34 New-York. [Za2] D. Zagier. Hecke operators and periods of modular forms. Chelsea (1975)) (and Remarques sur les transcendantes Israel Math. Conf. Proc. 3 (1990), 321–336. elliptiques et abéliennes. Journal de Liouville 10 (1845), 445–450). [Eis2] G. Eisenstein. Genaue Untersuchung der unendlichen Doppelproducte, aus welchen die elliptischen Functionen Pierre Charollois [pierre.charollois@ als Quotienten zusammengesetzt sind, und der mit ih- nen zusammenhängenden Doppelreihen. J. Reine Angew. imj-prg.fr] received his PhD in Bordeaux Math. 35 (1847), 153–274. (and Math. Werke I, 357–478. in 2004. After a postdoctoral stay at New-York. Chelsea (1975)). McGill University (Montréal), he is now [HH] K. Hensel, H. Hasse. Zusätze, in Kronecker’s Werke, Band maître de conférences at Université Paris 6 V, (1930) 507–515. in Jussieu. His focus is on number theory, [Ha] H. Hasse. History of class field theory. in Cassels-Fröhlich modular forms and L-functions, including (eds), Algebraic Number Theory, London: Academic Press a keen interest in the historical grounds (1967), 266–279. [IO] T. Ishii, T. Oda. A short history on investigation of the spe- regarding these objects of study, notably their connections to cial values of zeta and L-functions of totally real number Eisenstein, Kronecker and Lerch. fields. In Automorphic forms and zeta functions. Proc. of the conf. in memory of Tsuneo Arakawa, World Sci. Publ. Robert Sczech [[email protected]] stud- (2006), 198-233. ied mathematics at Bonn University, where [Ma] B. Mazur. Visions, Dreams and Mathematics. in Cir- he received his PhD in 1981. He is cles disturbed: the interplay of Mathematics and presently working at Rutgers University in Narrative. A. Doxiadis, B. Mazur (eds). Prince- Newark, New Jersey. His field of interest is ton Univ. Press (2012) 243–273. With a compan- in number theory and includes the study ion interview, http://thalesandfriends.org/2007/07/23/ mazur-interviewed-by-corfield. of special values of L-functions attached [Ro] D. E. Rowe. Göttingen’s SUB as repository for the papers to number fields (including cohomological interpretation via of distinguished mathematicians. This volume, 39–44. group cocycles and the Stark conjecture). 14 EMS Newsletter September 2016 Feature Wrinkles: From From the the Sea Sea to Mathematics François Laudenbach (Université de Nantes, France) François Laudenbach (Université de Nantes, France) Wrinkles and sealing Nevertheless, the differential df can be deformed to a non-vanishing differential 1-form, denoted df, which co- R The mathematical meaning of wrinkle and its real-life mean- incides with df near a and b. Of course, the corresponding ing are very similar, particularly when the word is used to change in f would have to change the value at one endpoint, describe features on the surface of the sea. Luckily, I was ed- say b. This df is called the regularized differential of f . It R ucated in sailing before learning advanced mathematics so I is unique up to deformation among the non-vanishing differ- spent a lot of time looking at wrinkles on the sea. After a long, ential forms since the constraints near the endpoints define a windless period, it is delightful to observe their birth and the convex set. The name and notation are due to Y. Eliashberg forms they take. Long after learning to sail, I read that these and N. Mishachev [2], the inventors of mathematical wrin- forms bear great similarity to those predicted by R. Thom’s kles. singularity theory (see [15]). On one occasion, wrinkles ap- peared and grew so abruptly that they clearly announced a Wrinkles and immersions strong event; at the same time, the on-board radio issued gale warnings for the forthcoming night. Soon the fog cleared, al- Historically, this first wrinkle (without its name) appeared lowing us to see an enormous cumulonimbus cloud, with its soon after S. Smale’s breakthrough of the sphere eversion white anvil thousands of metres high, indicating the presence [14], a counter-intuitive phenomenon where it is possible to of fantastic thermodynamic machinery. Fortunately, this ex- turn a sphere inside out by allowing only self-intersections perience concluded safely. but no pinching, that is, by moving the sphere through im- mersions. The first person who figured out Smale’s result was Basics about wrinkles A. Shapiro (1961)1 (see, in chronological order, [11], [6] and [9]). The eversion [11], of which Figure 2 shows one stage, Mathematical wrinkles are models for maps Rn Rq, n q, → ≥ exhibits a lot of wrinkles. restricted to some explicit compact subset. The very primitive wrinkle is the one-variable smooth function whose graph is shown in Figure 1. That function f , defined on [a, b], has one maximum and one minimum, both non-degenerate, meaning that the second derivative does not vanish at these critical points; one says that f is a Morse function. It is unique up to reparametrisation of the domain and the range, which can alter, for example, the distance between critical points and critical values. As f (a) > f (b), the maximum principle for real continu- ous functions makes it impossible to deform f to a function without critical points if we insist on keeping f unchanged near the boundary points a and b. Indeed, there must exist a maximum value greater than f (a) and a minimum value less than f (b). f(a) Figure 2. Original drawing for a sphere eversion (courtesy of Anthony f(b) Phillips) 1 Quoting the beginning of Francis & Morin’s article: “We dedicate this a b article to the memory of Arnold Shapiro, who gave the first example of Figure 1. The primitive wrinkle how to turn the sphere inside out, but never published it.” EMS Newsletter September 2016 15 Feature w(c1) w(c2) folded diameter c1 c2 boundary w fold lines Figure 4. The lips wrinkle has cusps at c1 and c2 two fold lines, namely the two open arcs ∂D c , c (see { 1 2} Figure 4). Figure 3. Folded immersion of the 2-disc and one folded diameter The image of the singular locus looks like lips, a famous figure in Cerf’s analysis of pseudo-isotopies [1]. Using hori- zontal coordinate y in [ 1, 1] and x in the fibre over y, A natural question to ask is which immersions of the − (n 1)-sphere into Rn extend to an immersion of the n-ball. w(y, x) = y, fy(x) , − Apart from some obvious homotopy theoretical obstructions, where fy(x) is a 1-parameter family of primitive wrinkles the problem remains open for n > 2. A complete (but diffi- y cult) answer in dimension 2 has been given by S. Blank (see from birth todeath as y traverses the interval [y(c1), y(c2)]. For [12]). further extension to high dimension, one requires the symme- try fy = f y. By regularising the differential dfy smoothly in In 1966, V. Poenaru [13] showed that relaxing the immer- − sion condition on the n-ball by allowing folds (such as, in lo- y, we get a regularised differential: cal coordinates, x x2 in dimension one or (x, y) (x2, y) 2 → → dw : T(y,x)W Tw(y,x)R . in dimension two) made the problem of extension easily solv- R → able. For instance, focusing on n = 2 to make drawings possi- The word regularisation translates the fact that the rank of ble, every immersion S 1 R2 extends to a folded immersion dw is maximal on all fibres of the tangent space TW. This → R of the disc to the plane as in Figure 3. In this example, without model extends to a wrinkle w with source and target of di- mension q, simply by taking y Rq 1 and rotating the 2- any fold line, there is no immersion of the disc extending the ∈ − given immersion. Indeed, the immersion of the disc if it ex- dimensional model about the axis y = 0. Then, ists must enter the unbounded component of the complement w(y, x) = (y, f y (x)) of the given immersed boundary line. But the disc is com- | | pact and any point of its image lying at a maximal distance and the regularised differential still exists. Finally, one can from the origin should be a critical point of the map, which is obtain a non-equidimensional model by enlarging the source therefore not an immersion. with an (n q)-ball (with coordinate z) and taking the map − This result translates a sort of flexibility in a sense pre- w(y, x, z) = y, f y (x) + Q(z) , cisely defined by M. Gromov in his seminal book [8]. The | | fold lines that Poenaru introduces lie parallel to the bound- where Q is a non-degenerate quadratic form. ary in a collar neighbourhood in the source disc. Thus, a pair With these models at hand, a wrinkled map g : Mn → of consecutive such fold lines may be thought of as a one- Nq, n q, between (possibly closed) manifolds is a smooth ≥ parameter family of primitive wrinkles. In the example shown map that coincides with wrinkle models in finitely many dis- in Figure 3, this family is made of folded diameters; one of the joint balls in Mn and has maximal rank elsewhere. Eliashberg diameters is shown. & Mishachev [2] state the flexibility of wrinkled maps, in that an h-principle in the sense of Gromov holds true for them. Wrinkles and the h-principle To make this more precise, denote by TM and TN the re- spective tangent spaces and consider the set W(M,N), formed The efficiency of what have been called primitive wrinkles by the collection of wrinkled maps and completed by maps above – mostly used in families – is already remarkable when with so-called embryos or unborn wrinkles. This set embeds applied to immersions (see W. Thurston’s corrugations [16]). into the space of bundle epimorphisms Epi(TM, TN) by the Of course, if one aims to apply wrinkles to very general regularised differential operator d and this embedding is a R classes of smooth mappings of manifolds, a more elaborate homotopy equivalence. model of wrinkles has to be used. Fortunately, this model, which is global in essence, still involves the two local stable Applications and novelties singularities of mappings from plane to plane only, namely the fold and the so-called cusp. A spectacular application to pseudo-isotopy theory [3] is a If the source and target are two-dimensional, a wrinkle strong generalisation of a theorem by K. Igusa (1984) [7], W consists, as in Figure 4, of a neighbourhood of a disc D with no restriction on dimension. Namely, any family of in the source, fibred in intervals over an interval I, with two smooth functions fu : M ([0, 1], 0, 1) ([0, 1], 0, 1) u S k { × → } ∈ fibres tangent to the boundary ∂D at points c1 and c2, and a contracts in the space of Morse functions with the same smooth map w : W R2. This map is fibred over an interval; boundary condition, completed by the embryos (functions → its singular locus consists of two cusps in c1 and c2 and of with one cubic singularity). 16 EMS Newsletter September 2016 Feature More recently, Eliashberg & Mishachev with S. Galatius [5] Eliashberg Y., Galatius S. & Mishachev N., Madsen–Weiss for [5] have shown that wrinkles apply in an area usually reserved geometrically minded topologists, Geometry & Topology, 15 to homotopy theorists. The question is to compute the stable2 (2011), 411–472. [6] Francis G. & Morin B., Arnold Shapiro’s eversion of the homology of the mapping class group of a Riemann surface. sphere, Math. Intelligencer 2 (1979), 200–203. Last but not least, thanks to the flexibility of a slightly [7] Igusa K., Higher singularities are unnecessary, Annals of different object called a wrinkled embedding [4], we wit- Math. 119 (1984), 1-58. nessed an exceptional event: E. Murphy’s breakthrough in [8] Gromov M., Partial Differential Relations, Springer, 1986. high-dimensional contact topology [10]. Thanks to wrinkling [9] Levy S., Making waves, A guide to the ideas behind Outside techniques (large zig-zags in front projections3), she discov- In, (text and video), AK Peters, Wellesley (MA), 1995. ered the loose Legendrian embeddings into contact manifolds. [10] Murphy E., Loose Legendrian embeddings in high dimen- sional contact manifolds, arXiv: 1201.2245. Such an embedding makes the ambient contact structure flex- [11] Phillips A., Turning a surface inside out, Scientific American ible. The wrinkle story is clearly far from over. 214 (May 1966), 112–120. [12] Poenaru V., Extension des immersions en codimension 1 Acknowledgement (d’après S. Blank), exposé n◦ 342, p. 473–505 in: Séminaire I am very indebted to Frank Morgan who gave me many sug- N. Bourbaki, vol. 10, 1966–1968, Soc. Math. de France, 1995; gestions for writing in a simpler language for addressing a https://eudml.org/doc/109745. large audience. I also feel very grateful to Allyn Jackson for [13] Poenaru V., On regular homotopy in codimension 1, Ann. of Math. 83 (2) (1966), 257–265. her help in some delicate situations. I express my thanks to [14] Smale S., A classification of immersions of the two-sphere, Anthony Phillips who offered me a copy of one of his beauti- Trans. Amer. Math. Soc. 90 (1958), 281–290. ful drawings and to Vincent Borrelli for his careful reading of [15] Thom R., Structural Stability and Morphogenesis, Addison- this note. Wesley, 2nd ed., 1994. [16] Thurston W., Making waves: The theory of corrugations, in: [9]. References [1] Cerf J., La stratification naturelle des espaces de fonctions dif- François Laudenbach [francois.laudenbach férentiables réelles et le théorème de la pseudo-isotopie, Inst. @univ-nantes.fr] is a topologist (explor- Hautes Études Sci. Publ. Math. 39 (1970), 5–173. ing topics such as pseudo-isotopy, Morse [2] Eliashberg Y. & Mishachev N., Wrinkling of smooth mappings functions, 2-spheres in 3-manifolds, closed and its applications I, Invent. Math. 130 (1997), 345–369. differential forms of degree one, generat- [3] , Wrinkling of smooth mappings-II Wrinkling of embed- ing functions in symplectic topology and dings and K. Igusa’s theorem, Topology 39 (2000), 711–732. Morse-Novikov theory). He has had posi- Wrinkled embeddings [4] , , Contemporary Mathematics 498 tions as professor at various places including the University (2009), 207–232; http://dx.doi.org/10.1090/conm/498/09753. Paris-sud (Orsay) from 1974 to 1989 and then successively the École Normale Supérieure de Lyon, the École polytech- 2 Quoted from [5, p. 412]: “stabilization with respect to the genus”. nique and the Université de Nantes, where he retired as a professor emeritus. He has been Editor-in-Chief of Astérisque 3 Near a Legendrian submanifold, the local model of a contact structure is given by the one-jet space J1(Rn, R) equipped with the 2n-plane field and of the Bulletin SMF at different periods. He directed the whose equation reads dz p dqi = 0 in canonical coordinates. The Centre de Mathématiques of the École polytechnique from − i front projection is the projection onto the 0-jet space (q, p, z) (q, z). → 1994 to 2000. European Mathematical Society Publishing House Seminar for Applied Mathematics ETH-Zentrum SEW A27, CH-8092 Zürich, Switzerland [email protected] / www.ems-ph.org Geometry, Analysis and Dynamics on sub-Riemannian Manifolds, Volume I and Volume II (EMS Series of Lectures in Mathematics) Davide Barilari (Université Paris 7 Denis Diderot, Paris, France), Ugo Boscain (École Polytechnique, Palaiseau, France) and Mario Sigalotti (École Polytechnique, Palaiseau, France), Editors Vol. I: ISBN 978-3-03719-162-0. 2016. 332 pages. Softcover. 17 x 24 cm. 44.00 Euro Vol. II ISBN 978-3-03719-163-7. 2016. Approx. 306 pages. Softcover. 17 x 24 cm. 44 Euro Sub-Riemannian manifolds model media with constrained dynamics: motion at any point is only allowed along a limited set of directions, which are prescribed by the physical problem. From the theoretical point of view, sub-Riemannian geometry is the geometry underlying the theory of hypoelliptic operators and degenerate diffusions on manifolds. In the last twenty years, sub-Riemannian geometry has emerged as an independent research domain, with extremely rich motivations and ramifications in several parts of pure and applied mathematics, such as geometric analysis, geometric meas- ure theory, stochastic calculus and evolution equations together with applications in mechanics, optimal control and biology. The aim of the lectures collected here is to present sub-Riemannian structures for the use of both researchers and graduate students. EMS Newsletter September 2016 17 Feature Kardar–Parisi–Zhang Universality universality Ivan Corwin (Columbia University, New York, USA) Ivan Corwin (Columbia University, New York, USA) 1 Universality in random systems area of study. To even provide a representative cross-section of references is beyond this scope. Additionally, even though Universality in complex random systems is a striking con- we will discuss integrable examples, we will not describe cept that has played a central role in the direction of re- the algebraic structures and methods of asymptotic analy- search within probability, mathematical physics and statisti- sis behind them (despite their obvious importance and inter- cal mechanics. In this article, we will describe how a vari- est). Some recent references that review some of these struc- ety of physical systems and mathematical models, including tures include [2, 4, 8] and references therein. On the more randomly growing interfaces, certain stochastic PDEs, traf- physics-oriented side, the collection of reviews and books fic models, paths in random environments and random matri- [1, 3, 5, 6, 7, 8, 9, 10] provides some idea of the scope of ces, all demonstrate the same universal statistical behaviours the study of the KPZ universality class and the diverse areas in their long-time/large-scale limit. These systems are said upon which it touches. to lie in the Kardar–Parisi–Zhang (KPZ) universality class. We start now by providing an overview of the general no- Proof of universality within these classes of systems (except tion of universality in the context of the simplest and histori- for random matrices) has remained mostly elusive. Extensive cally first example – fair coin flipping and the Gaussian uni- computer simulations, non-rigorous physical arguments and versality class. heuristics, some laboratory experiments and limited mathe- matically rigorous results provide important evidence for this 2 Gaussian universality class belief. The last 15 years have seen a number of breakthroughs Flip a fair coin N times. Each string of outcomes (e.g., head, N in the discovery and analysis of a handful of special inte- tail, tail, tail, head) has an equal probability 2− . Call H the grable probability systems, which, due to enhanced algebraic (random) number of heads and let P denote the probability structure, admit many exact computations and, ultimately, distribution for this sequence of coin flips. Counting shows asymptotic analysis revealing the purportedly universal prop- that erties of the KPZ class. The structures present in these sys- N N P H = n = 2− . tems generally originate in representation theory (e.g., sym- n metric functions), quantum integrable systems (e.g. Bethe Since each flip is independent, the expected number of heads ansatz) and algebraic combinatorics (e.g., RSK correspon- is N/2. Bernoulli (1713) proved that H/N converges to 1/2 as dence) and the techniques in their asymptotic analysis gen- N goes to infinity. This was the first example of a law of large erally involve Laplace’s method, Fredholm determinants or numbers. Of course, this does not mean that if you flip the Riemann-Hilbert problem asymptotics. coin 1000 times, you will see exactly 500 heads. Indeed, in N This article will focus on the phenomena associated with coin flips one expects the number of heads to vary randomly the KPZ universality class [3] and highlight how certain in- around the value N/2 in the scale √N. Moreover, for all x tegrable examples expand the scope of and refine the notion ∈ R, of universality. We start by providing a brief introduction to x y2/2 e− the Gaussian universality class and the integrable probabilis- lim P H < 1 N + 1 √Nx = dy. N 2 2 √ tic example of random coin flipping, as well as the random →∞ 2π deposition model. A small perturbation to the random depo- −∞ sition model leads us to the ballistic deposition model and the De Moivre (1738), Gauss (1809), Adrain (1809), and Laplace KPZ universality class. The ballistic deposition model fails to (1812) all participated in the proof of this result. The limiting be integrable; thus, to gain an understanding of its long-time distribution is known as the Gaussian (or sometimes normal behaviour and that of the entire KPZ class, we turn to the cor- or bell curve) distribution. ner growth model. The rest of the article focuses on various A proof of this follows from asymptotics of n!, as derived sides of this rich model: its role as a random growth process, by de Moivre (1721) and named after Stirling (1729). Write its relation to the KPZ stochastic PDE, its interpretation in ∞ ∞ t n n+1 nf(z) terms of interacting particle systems and its relation to opti- n! =Γ(n + 1) = e− t dt = n e dz, misation problems involving paths in random environments. 0 0 Along the way, we include some other generalisations of this where f (z) = log z z and the last equality is from the change − process whose integrability springs from the same sources. of variables t = nz. The integral is dominated, as n grows, by We close the article by reflecting upon some open problems. the maximal value of f (z) on the interval [0, ). This occurs A survey of the KPZ universality class and all of the as- (z 1)2 ∞ at z = 1; thus, expanding f (z) 1 − and plugging this sociated phenomena and methods developed or utilised in its ≈− − 2 into the integral yields the final expansion study is far too vast to be provided here. This article presents n+1 n only one of many stories and perspectives regarding this rich n! n e− 2π/n. ≈ EMS Newsletter September 2016 19 Feature This general route of writing exact formulas for probabilities in terms of integrals and then performing asymptotics is quite common to the analysis of integrable models in the KPZ uni- versality class – though those formulas and analyses are con- siderably more involved. The universality of the Gaussian distribution was not broadly demonstrated until work of Chebyshev, Markov and Lyapunov around 1900. The central limit theorem (CLT) (a) (b) showed that the exact nature of coin flipping is immaterial – any sum of independent, identically distributed (iid) random variables with finite mean and variance will demonstrate the same limiting behaviour. Theorem 2.1. Let X1, X2,...be iid random variables of finite mean m and variance v. Then, for all x R, ∈ x N y2/2 e− lim P Xi < mN + v √Nx = dy. N √ π →∞ i=1 2 (c) (d) −∞ Proofs of this result use different tools than the exact anal- Figure 1. (A) and (B) illustrate the random deposition model and (C) ysis of coin flipping and much of probability theory deals and (D) illustrate the ballistic deposition model. In both cases, blocks fall from above each site with independent, exponentially distributed wait- with the study of Gaussian processes that arise through var- ing times. In the first model, they land at the top of each column whereas ious generalisations of the CLT. The Gaussian distribution is in the second model they stick to the first edge to which they become ubiquitous and, as it is the basis for much of classical statistics incident. and thermodynamics, it has had immense societal impact. While the Gaussian behaviour of this model is resilient 3 Random versus ballistic deposition against changes in the distribution of the wx,i (owing to the The random deposition model is one of the simplest (and least CLT), generic changes in the nature of the growth rules shat- realistic) models for a randomly growing one-dimensional in- ter the Gaussian behaviour. The ballistic deposition (or sticky terface. Unit blocks fall independently and in parallel from block) model was introduced by Vold (1959) and, as one ex- the sky above each site of Z according to exponentially dis- pects in real growing interfaces, displays spatial correlation. tributed waiting times (see Figure 1). Recall that a random As before, blocks fall according to iid exponential waiting variable X has an exponential distribution of rate λ>0 (or times; however, a block will now stick to the first edge against λx which it becomes incident. This mechanism is illustrated in mean 1/λ) if P(X > x) = e− . Such random variables are characterised by the memoryless property – conditioned on Figure 1. This creates overhangs and we define the height the event that X > x, X x still has the exponential distri- function h(t, x) as the maximal height above x that is occu- − bution of the same rate. Consequently, the random deposition pied by a box. How does this microscopic change manifest model is Markov – its future evolution only depends on the itself over time? present state (and not on its history). It turns out that sticky blocks radically change the limit- The random deposition model is quite simple to analyse ing behaviour of this growth process. The bottom of Figure since each column grows independently. Let h(t, x) record the 2 records one simulation of the process. Seppäläinen (1999) height above site x at time t and assume h(0, x) 0. Define gave a proof that there is still an overall linear growth rate. ≡ Moreover, by considering a lower bound by a width two sys- random waiting times wx,i to be the time for the i-th block in column x to fall. For any n, the event h(t, x) < n is equivalent tem, one can see that this velocity exceeds that of the random n deposition model. The exact value of this rate, however, re- to i=1 wx,i > t. Since the wx,i are iid, the law of large numbers and central limit theory apply here. Assuming λ = 1, mains unknown. The simulation in Figure 2 (as well as the longer time re- h(t, x) h(t, x) t lim = 1, and lim − N(x) sults displayed in Figure 3) also shows that the scale of fluc- t t 1/2 →∞ t →∞ t ⇒ tuations of h(t, x) is smaller than in random deposition and jointly over x Z, where N(x) is a collection of iid stan- that the height function remains correlated transversally over ∈ x Z dard Gaussian random variables.∈ The top of Figure 2 shows a a long distance. There are exact conjectures for these fluctua- simulation of the random deposition model. The linear growth tions. They are supposed to grow like t1/3 and demonstrate a speed and lack of spatial correlation are quite evident. The non-trivial correlation structure in a transversal scale of t2/3. fluctuations of this model are said to be in the Gaussian uni- Additionally, precise predictions exist for the limiting dis- versality class since they grow like t1/2, with Gaussian limit tributions. Up to certain (presently undetermined) constants law and trivial transversal correlation length scale t0. In gen- c , c , the sequence of scaled heights c t 1/3 h(t, 0) c t 1 2 2 − − 1 eral, fluctuation and transversal correlation exponents, as well should converge to the so-called Gaussian Orthogonal En- as limiting distributions, constitute the description of a uni- semble (GOE) Tracy-Widom distributed random variable. The versality class and all models that match these limiting be- Tracy-Widom distributions can be thought of as modern-day haviours are said to lie in the same universality class. bell curves and their names GOE or GUE (for Gaussian 20 EMS Newsletter September 2016 Feature Figure 3. Simulation of random (left) versus ballistic (right) deposition models driven by the same process of falling blocks and run for a long time. The white and grey colours represent different epochs of time in the simulation. The sizes of the boxes in both figures are the same. 4 Corner growth model We come to the first example of an integrable probabilistic system in the KPZ universality class – the corner growth model. The randomly growing interface is modelled by a height function h(t, x) that is continuous, piecewise linear and composed of √2-length line increments of slope +1 or 1, − Figure 2. Simulation of random (top) versus ballistic (bottom) deposition changing value at integer x. The height function evolves ac- models driven by the same process of falling blocks. The ballistic model cording to the Markovian dynamics that each local minimum grows much faster and has a smoother, more spatially correlated top of h (looking like ) turns into a local maximum (looking interface. ∨ like ) according to an exponentially distributed waiting time. ∧ This happens independently for each minimum. This change in height function can also be thought of as adding boxes (ro- tated by 45◦). See Figures 4 and 5 for further illustration of Unitary Ensemble) come from the random matrix ensembles this model. Wedge initial data means that h(0, x) = x while flat initial in which these distributions were first observed by Tracy- | | Widom (1993, 1994). data (as considered for ballistic deposition) means that h(0, x) Ballistic deposition does not seem to be an integrable is given by a periodic saw-tooth function that goes between probabilistic system so where do these precise conjectures heights 0 and 1. We will focus on wedge initial data. Rost come from? The exact predictions come from the analysis of (1980) proved a law of large numbers for the growing inter- a few similar growth processes that just happen to be inte- face when time, space and the height function are scaled by grable! Ballistic deposition shares certain features with these the same large parameter L. models that are believed to be key for membership in the KPZ class: • Locality: height function change depends only on neigh- bouring heights. • Smoothing: large valleys are quickly filled in. (a) (b) • Non-linear slope dependence: vertical effective growth rate depends non-linearly on local slope. • Space-time independent noise: growth is driven by noise, which quickly decorrelates in space and time and does not display heavy tails. It should be made clear that a proof of the KPZ class be- haviour for the ballistic deposition model is far beyond what (c) (d) can be done mathematically (though simulations strongly Figure 4. Various possible ways that a local minimum can grow into a suggest that the above conjecture is true). local maximum. EMS Newsletter September 2016 21 Feature (a) (b) (c) (d) Figure 6. Simulation of the corner growth model. The top shows the model after a medium amount of time and the bottom shows it after a longer amount of time. The rough interface is the simulation while the smooth curve is the limiting parabolic shape. The simulation curve has vertical fluctuations of order t1/3 and decorrelates spatially on distances (e) (f) of order t2/3. This equation actually governs the evolution of the law of large numbers from arbitrary initial data. The fluctuations of this model around the law of large numbers are what is believed to be universal. Figure 6 shows that the interface fluctuates around its limiting shape on a fairly small scale, with transversal correlation on a larger scale. For >0, define the scaled and centred height func- tion (g) (h) 1 b z 1 − t Figure 5. The corner growth model starts with an empty corner, as in (A). h (t, x):= h(− t,− x) , There is only one local minimum (the large dot) and after an exponen- − 2 tially distributed waiting time, this turns into a local maximum by filling where the dynamic scaling exponent z = 3/2 and the fluctu- in the site above it with a block, as in (B). In (B), there are now two pos- ation exponent b = 1/2. These exponents are easily remem- sible locations for growth (the two dots). Each one has an exponentially distributed waiting time. (C) corresponds to the case when the left local bered since they correspond with scaling time : space : fluctu- minimum grows before the right one. By the memoryless property of ex- ations like 3 : 2 : 1. These are the characteristic exponents for ponential random variables, once in state (C), we can think of choosing the KPZ universality class. Johansson (1999) proved that for new exponentially distributed waiting times for the possible growth des- fixed t, as 0, the random variable h (t, 0) converges to tinations. Continuing in a similar manner, we arrive at the evolution in → (D) through (H). a GUE Tracy-Widom distributed random variable (see Figure 7). Results for the related model of the longest increasing sub- sequence in a random permutation were provided around the Theorem 4.1. For wedge initial data, same time by Baik-Deift-Johansson (1999). For that related 1 (x/t)2 model, two years later, Prähofer-Spohn (2001) computed the h(Lt, Lx) t − x < t, lim = h(t, x):= 2 | | analogue to the joint distribution of h (t, x) for fixed t and L →∞ L x x t. varying x. | |||≥ The entire scaled growth process h ( , ) should have a Figure 6 displays the result of a computer simulation · · limit as 0 that would necessarily be a fixed point under wherein the limiting parabolic shape is evident. The function → 3 : 2 : 1 scaling. The existence of this limit (often called the h is the unique viscosity solution to the Hamilton-Jacobi equa- KPZ fixed point) remains conjectural. Still, much is known tion ∂ 1 ∂ about the properties this limit should enjoy. It should be a h(t, x) = 1 h(t, x) 2 . ∂t 2 − ∂x stochastic process whose evolution depends on the limit of 22 EMS Newsletter September 2016 Feature cal minima into local maxima at rate p, and turn local maxima into local minima at rate q (all waiting times are independent and exponentially distributed, and p + q = 1). See 8 for an illustration of this partially asymmetric corner growth model. Tracy-Widom (2007-2009) showed that so long as p > q, the same law of large numbers and fluctuation limit theorem holds for the partially asymmetric model, provided that t is replaced by t/(p q). Since p q represents the growth drift, − − one simply has to speed up to compensate for this drift being smaller. Clearly, for p q, something different must occur than ≤ for p > q. For p = q, the law of large numbers and fluctua- tions change nature. The scaling of time : space : fluctuations becomes 4 : 2 : 1 and the limiting process under these scal- ings becomes the stochastic heat equation with additive white noise. This is the Edwards-Wilkinson (EW) universality class, 5 4 3 2 1 01 which is described by the stochastic heat equation with ad- − − − − − ditive noise. For p < q, the process approaches a stationary distribution where the probability of having k boxes added to the empty wedge is proportional to (p/q)k. 40 0 40 80 120 160 200 So, we have observed that for any positive asymmetry the − growth model lies in the KPZ universality class while for zero asymmetry it lies in the EW universality class. It is natural to wonder whether by critically scaling parameters (i.e. p q 1000 − → − 0), one might encounter a crossover regime between these two universality classes. Indeed, this is the case and the crossover 2000 − is achieved by the KPZ equation that we now discuss. 3000 5 The KPZ equation − The KPZ equation is written as 4000 − ∂h ∂2h ∂h 2 (t, x) = ν (t, x) + 1 λ (t, x) + √Dξ(t, x), ∂t ∂x2 2 ∂x 5000 − where ξ(t, x) is Gaussian space-time white noise, λ, ν R, ∈ Figure 7. The density (top) and log of the density (bottom) of the GUE D > 0 and h(t, x) is a continuous function of time t R ∈ + Tracy-Widom distribution. Though the density appears to look like a and space x R, taking values in R. Due to the white noise, ∈ bell-curve (or Gaussian), this comparison is misleading. The mean and one expects x h(t, x) to be only as regular as in Brownian variance of the distribution are approximately 1.77 and 0.81. The − → tails of the density (as shown in terms of the log of the density in the motion. Hence, the non-linearity does not a priori make any 3 / c x c+ x3 2 bottom plot) decay like e − for x 0 and like e− for x 0, sense (the derivative of Brownian motion has negative Hölder − | | for certain positive constants c and c+. The Gaussian density decays − regularity). Bertini-Cancrini (1995) provided the physically cx2 like e− in both tails, with the constant c related to the variance. relevant notion of solution (called the Hopf–Cole solution) and showed how it arises from regularising the noise, solving the (now well-posed) equation and then removing the noise the initial data under the same scaling. The one-point distri- and subtracting a divergence. bution for general initial data, the multi-point and multi-time The equation contains the four key features mentioned distribution for wedge initial data and various aspects of its earlier – the growth is local, depending on the Laplacian continuity are all understood. Besides the existence of this (smoothing), the square of the gradient (non-linear slope de- limit, what is missing is a useful characterisation of the KPZ pendent growth) and white noise (space-time uncorrelated fixed point. Since the KPZ fixed point is believed to be the noise). Kardar, Parisi and Zhang introduced their eponymous universal scaling limit of all models in the KPZ universality equation and 3:2:1 scaling prediction in 1986 in an attempt class and since corner growth enjoys the same key properties to understand the scaling behaviours of random interface as ballistic deposition, one is also led to the conjecture that growth. ballistic deposition scales to the same fixed point and hence How might one see the 3:2:1 scaling from the KPZ equa- b z 1 enjoys the same scalings and limiting distributions. The rea- tion? Define h (t, x) = h(− t,− x); then, h satisfies the 2 z 2 z b 1 son why the GOE Tracy-Widom distribution came up in our KPZ equation with scaled coefficients − ν, − − 2 λ and b z + 1 earlier discussion is that we were dealing with flat rather than − 2 2 √D. It turns out that two-sided Brownian motion is wedge initial data. stationary for the KPZ equation; hence, any non-trivial scal- One test of the universality belief is to introduce partial ing must respect the Brownian scaling of the initial data and asymmetry into the corner growth model. Now we change lo- thus have b = 1/2. Plugging this in, the only way to have EMS Newsletter September 2016 23 Feature no coefficient blow up to infinity and not to have every term shrink to zero (as 0) is to choose z = 3/2. This suggests → the plausibility of the 3:2:1 scaling. While this heuristic gives the right scaling, it does not provide for the scaling limit. The limit as 0 of the equation (the inviscid Burgers equa- → tion where only the non-linearity survives) certainly does not govern the limit of the solutions. It remains something of a mystery as to exactly how to describe this limiting KPZ fixed (a) point. The above heuristic says nothing of the limiting distri- bution of the solution to the KPZ equation and there does not currently exist a simple way to see what this should be. It took just under 25 years until Amir-Corwin-Quastel (2010) rigorously proved that the KPZ equation is in the KPZ universality class. That work also computed an exact formula for the probability distribution of the solution to the KPZ equation – marking the first instance of a non-linear stochas- tic PDE for which this was accomplished. Tracy-Widom’s work on the partially asymmetric corner growth model and (b) the work of Bertini-Giacomin (1997) relating that model to Figure 8. Mapping the partially asymmetric corner growth model to the the KPZ equation were the two main inputs in this develop- partially asymmetric simple exclusion process. In (A), the local minimum grows into a local maximum. In terms of the particle process beneath it, ment. See [3] for further details regarding this, as well as the the minimum corresponds to a particle followed by a hole and the growth simultaneous exact but non-rigorous steepest descent work of corresponds to said particle jumping into the hole to its right. In (B), the Sasamoto-Spohn (2010), and non-rigorous replica approach opposite is shown as the local maximum shrinks into a local minimum. work of Calabrese-Le Doussal-Rosso (2010) and Dotsenko Correspondingly, there is a hole followed by a particle and the shrinking results in the particle moving into the hole to its left. (2010). The proof that the KPZ equation is in the KPZ universal- ity class was part of an ongoing flurry of activity surrounding sity. ASEP was introduced in biology literature in 1968 by the KPZ universality class from a number of directions such MacDonald-Gibbs-Pipkin as a model for RNA’s movement as integrable probability [4], experimental physics [10] and during transcription. Soon after, it was independently intro- stochastic PDEs. For instance, Bertini-Cancrini’s Hopf–Cole duced within the probability literature in 1970 by Spitzer. solution relies upon a trick (the Hopf–Cole transform) that The earlier quoted results regarding corner growth imme- linearises the KPZ equation. Hairer (2011), who had been diately imply that the number of particles to cross the origin developing methods to make sense of classically ill-posed after a long time t demonstrates KPZ class fluctuation be- stochastic PDEs, focused on the KPZ equation and developed haviour. KPZ universality would have that generic changes a direct notion of solution that agreed with the Hopf–Cole one to this model should not change the KPZ class fluctuations. but did not require use of the Hopf–Cole transform trick. Still, Unfortunately, such generic changes destroy the model’s in- this does not say anything about the distribution of solutions tegrable structure. There are a few integrable generalisations or their long-time scaling behaviours. Hairer’s KPZ work set discovered over the past five years that demonstrate some of the stage for his development of regularity structures in 2013 the resilience of the KPZ universality class against perturba- – an approach to construction solutions of certain types of ill- tions. posed stochastic PDEs – work for which he was awarded a TASEP (the totally asymmetric version of ASEP) is a very Fields Medal. basic model for traffic on a one-lane road in which cars (par- ticles) move forward after exponential rate one waiting times, 6 Interacting particle systems provided the site is unoccupied. A more realistic model would account for the fact that cars slow down as they approach There is a direct mapping (see Figure 8) between the partially the one in front. The model of q-TASEP does just that (Fig- asymmetric corner growth model and the partially asymmet- ure 9). Particles jump right according to independent expo- ric simple exclusion process (generally abbreviated ASEP). nential waiting times of rate 1 qgap, where gap is the num- One can associate to every 1 slope line increment a particle − − ber of empty spaces to the next particle to the right. Here on the site of Z above which the increment sits, and to every q [0, 1) is a different parameter than in the ASEP, though ∈ +1 slope line increment an empty site. The height function when q goes to zero, these dynamics become those of TASEP. then maps onto a configuration of particles and holes on Z, Another feature one might include in a more realistic traf- with at most one particle per site. When a minimum of the height function becomes a maximum, it corresponds to a par- ticle jumping right by one into an empty site and, likewise, when a maximum becomes a minimum, a particle jumps left rate = 1 qgap − by one into an empty site. Wedge initial data for corner growth corresponds to having all sites to the left of the origin initially gap = 4 occupied and all to the right empty – this is often called step Figure 9. The q-TASEP, whereby each particle jumps one to the right initial data due to the step function in terms of particle den- after an exponentially distributed waiting time with rate given by 1 qgap. − 24 EMS Newsletter September 2016 Feature rate = L rate = 1 qgap − w4,2 w5,1 w1,4 w2,3 w3,2 w4,1 (a) w1,3 w2,2 w3,1 q2 q4 w1,2 w2,1 w1,1 (b) Figure 10. The q-pushASEP. As shown in (A), particles jump right ac- cording to the q-TASEP rates and left according to independent expo- Figure 11. The relation between the corner growth model and last pas- nentially distributed waiting times of rate L. When a left jump occurs, sage percolation with exponential weights. wi, j are the waiting times be- it may trigger a cascade of left jumps. As shown in (B), the right-most tween when a box can grow and when it does grow. L(x, y) is the time particle has just jumped left by one. The next particle (to its left) instan- when box (x, y) grows. taneously jumps left by one with probability given by qgap, where gap is the number of empty sites between the two particles before the left jumps occurred (in this case gap =4). If that next left jump is realised, the cascade continues to the next-left particle according to the same rule, demonstrates KPZ class fluctuations. A very compelling and otherwise it stops and no other particles jump left in that instant of time. entirely open problem is to show that this type of behaviour persists when the distribution of wi, j is no longer exponential. The only other solvable case is that of geometric weights. A fic model is the cascade effect of braking. The q-pushASEP certain limit of the geometric weights leads to maximising includes this (Figure 10). Particles still jump right according the number of Poisson points along directed paths. Fixing the to q-TASEP rules; however, particles may now also jump left total number of points, this becomes equivalent to finding the after exponential rate L waiting times. When such a jump oc- longest increasing subsequence of a random permutation. The curs, it prompts the next particle to the left to likewise jump KPZ class behaviour for this version of last passage percola- gap left, with a probability given by q , where gap is the num- tion was shown by Baik-Deift-Johansson (1999). ber of empty spaces between the original particle and its left There is another related integrable model that can be neighbour. If that jump occurs, it may likewise prompt the thought of as describing the optimal way to cross a large grid next left particle to jump, and so on. Of course, braking is not with stop lights at intersections. Consider the first quadrant of the same as jumping backwards; however, if one goes into a Z2 and to every vertex (x, y) assign waiting times to the edges moving frame, this left jump is like a deceleration. It turns leaving the vertex rightwards and upwards. With a probabil- out that both of these models are solvable via the methods ity of 1/2, the rightward edge has waiting time zero, while of Macdonald processes as well as stochastic quantum inte- the upward edge has waiting time given by exponential rate 1 grable systems and it has thus been proved that, just as for random variables; otherwise, reverse the situation. The edge ASEP, they demonstrate KPZ class fluctuation behaviour (see waiting time represents the time needed to cross an intersec- the review [4]). tion in the given direction (the walking time between lights has been subtracted). The minimal passage time from (1, 1) 7 Paths in a random environment to (x, y) is given by P(x, y) = min we, There is yet another class of probabilistic systems related π e π to the corner growth model. Consider the totally asymmet- ∈ ric version of this model, starting from wedge initial data. where π goes right or up in each step and ends on the vertical line above (x, y) and w is the waiting time for edge e π. An alternative way to track the evolving height function is e ∈ to record the time when a given box is grown. Using the la- From the origin, there will always be a path of zero waiting belling shown in Figure 11, let us call L(x, y) this time, for time, whose spatial distribution is that of the graph of a sim- x, y positive integers. A box (x, y) may grow once its parent ple symmetric random walk. Just following this path, one can blocks (x 1, y) and (x, y 1) have both grown – though even get very close to the diagonal x = y without waiting. On the − − other hand, for x y, getting to xt , yt for large t re- then it must wait for an independent exponential waiting time that we denote by wx,y. Thus, L(x, y) satisfies the recursion quires some amount of waiting. Barraquand-Corwin (2015) demonstrated that as long as x y, P xt , yt demonstrates L(x, y) = max L(x 1, y), L(x, y 1) + w , − − x,y KPZ class fluctuations. This should be true when π is re- subject to boundary conditions L(x, 0) 0 and L(0, y) 0. stricted to hit exactly (x, y), though that result has not yet been ≡ ≡ Iterating yields proved. Achieving this optimal passage time requires some level of omnipotence as you must be able to look forward be- L(x, y) = max wi, j, π fore choosing your route. As such, it could be considered as a (i, j) π ∈ benchmark against which to test various routing algorithms. where the maximum is over all up-right and up-left lattice In addition to maximising or minimising path problems, paths between box (1, 1) and (x, y). This model is called the KPZ universality class describes fluctuations of ‘positive last passage percolation with exponential weights. Follow- temperature’ versions of these models in which energetic or ing from the earlier corner growth model results, one readily probabilistic favouritism is assigned to paths based on the sum sees that for any positive real (x, y), for large t, L xt , yt of space-time random weights along its graph. One such sys- EMS Newsletter September 2016 25 Feature 8 Big problems It took almost 200 years from the discovery of the Gaussian distribution to the first proof of its universality (the central limit theorem). So far, KPZ universality has withstood proof for almost three decades and shows no signs of yielding. Besides universality, there remain a number of other big problems for which little to no progress has been made. All of the systems and results discussed herein have been 1 + 1 dimensional, meaning that there is one time dimension and one space dimension. In the context of random growth, it makes perfect sense (and is quite important) to study surface growth, i.e. 1 + 2 dimensional. In the isotropic case (where the underlying growth mechanism is roughly symmetric with respect to the two spatial dimensions), there are effectively no mathematical results though numerical simulations sug- gest that the 1/3 exponent in the t1/3 scaling for corner growth should be replaced by an exponent of roughly 0.24. In the anisotropic case there have been a few integrable examples discovered that suggest very different (logarithmic scale) fluc- Figure 12. The random walk in a space-time random environment. For tuations such as observed by Borodin-Ferrari (2008). each pair of up-left and up-right pointing edges leaving a vertex (y,s), the width of the edges is given by u , and 1 u , , where u , are inde- Finally, despite the tremendous success in employing y s − y s y s pendent uniform random variables on the interval [0, 1]. A walker (the methods of integrable probability to expand and refine the grey highlighted path) then performs a random walk in this environ- KPZ universality class, there still seems to be quite a lot of ment, jumping up-left or up-right from a vertex with probability equal room to grow and new integrable structures to employ. Within to the width of the edges. the physics literature, there are a number of exciting new di- rections in which the KPZ class has been pushed, including out-of-equilibrium transform and energy transport with mul- tiple conservation laws, front propagation equations, quan- tem is called directed polymers in random environment and tum localisation with directed paths and biostatistics. What is is the detropicalisation of LPP where one replaces the opera- equally important is to understand what type of perturbations tions of (max, +) by (+, ) in the definition of L(x, y). Then, break out of the KPZ class. × the resulting (random) quantity is called the partition func- Given all of the rich mathematical predictions, one might tion for the model and its logarithm (the free energy) is con- hope that experiments would have revealed KPZ class be- haviour in nature. This is quite a challenge since determin- jectured for very general distributions on wi, j to show KPZ class fluctuations. There is one known integrable example of ing scaling exponents and limiting fluctuations require im- weights for which this has been proved – the inverse-gamma mense numbers of repetitions of experiments. However, there distribution, introduced by Seppäläinen (2009) and proved in have been a few startling experimental confirmations of these the work of Corwin-O’Connell-Seppäläinen-Zygouras (2011) behaviours in the context of liquid crystal growth, bacterial and Borodin-Corwin-Remenik (2012). colony growth, coffee stains and fire propagation (see [10] The stop light system discussed above also has a positive and references therein). Truly, the study of the KPZ universal- temperature lifting of which we will describe a special case ity class demonstrates the unity of mathematics and physics (see Figure 12 for an illustration). For each space-time ver- at its best. tex (y, s), choose a random variable uy,s distributed uniformly on the interval [0, 1]. Consider a random walk X(t) that starts Acknowledgements at (0, 0). If the random walk is in position y at time s then it The author appreciates comments on a draft of this article by jumps to position y 1 at time s + 1 with probability u and A. Borodin, P. Ferrari and H. Spohn. This text is loosely based − y,s to position y + 1 with probability 1 u . With respect to the on his “Mathematic Park” lecture entitled Universal phenom- − y,s same environment of u’s, consider N such random walks. The ena in random systems and delivered at the Institut Henri fact that the environment is fixed causes them to follow cer- Poincaré in May 2015. The author is partially supported by tain high probability channels. This type of system is called the NSF grant DMS-1208998, by a Clay Research Fellow- a random walk in a space-time random environment and the ship, by the Poincaré Chair and by a Packard Fellowship for behaviour of a single random walker is quite well understood. Science and Engineering. Let us, instead, consider the maximum of N walkers in the N (i) same environment M(t, N) = maxi=1 X (t). For a given envi- ronment, it is expected that M(t, N) will localise near a given References random environment dependent value. However, as the ran- [1] A. Barabasi, H. Stanley. Fractal concepts in surface growth. dom environment varies, this localisation value does as well Cambridge University Press (1995). in such a way that for r (0, 1) and large t, M(t, ert) displays ∈ [2] A. Borodin, V. Gorin. Lectures on integrable probability. KPZ class fluctuations. arXiv:1212.3351. 26 EMS Newsletter September 2016 Feature [3] I. Corwin. The Kardar-Parisi-Zhang equation and universality ability, mathematical physics and inte- class. Rand. Mat.: Theo. Appl. 1:1130001 (2012). grable systems, and is particularly known [4] I. Corwin. Macdonald processes, quantum integrable systems for his work on the Kardar–Parisi–Zhang and the Kardar–Parisi–Zhang universality class. Proceedings equation and universality class. He ob- of the ICM (2014). [5] T. Halpin-Healy, Y-C. Zhang. Kinetic roughening, stochastic tained his PhD at the Courant Institute growth, directed polymers and all that. Phys. Rep., 254:215– and was the first Schramm Memorial Post- 415 (1995). doctoral Fellow at Microsoft Research and [6] J. Krug. Origins of scale invariance in growth processes. Ad- MIT. He has also held a Clay Research Fel- vances in Physics, 46:139–282 (1997). lowship and the first Poincare Chair at the Institute Henri [7] P. Meakin. Fractals, scaling and growth far from equilibrium. Poincare, and currently holds a Packard Foundation Fellow- Cambridge University Press (1998). ship in Science and Engineering. He received the Young Sci- [8] J. Quastel, H. Spohn. The one-dimensional KPZ equation and its universality class. J. Stat. Phys., to appear. entist Prize, the Rollo Davidson Prize and was an invited [9] H. Spohn. Large scale dynamics of interacting particles. speaker at the 2014 ICM. Springer, Heidelberg (1991). [10] K. Takeuchi, T. Halpin-Healy. A KPZ cocktail – shaken, not This article has been reprinted with permission from the orig- stirred . . . J. Stat. Phys. Online First (2015). inal publication in Notices of the American Mathematical Society 63 (2016), 230–239. Figures by Ivan Corwin and Ivan Corwin [[email protected]] is a professor of math- William Casselman, reprinted by permission of the creators. ematics at Columbia University. He works in between prob- Picture of Ivan Corwin: Courtesy of Craig Tracy. Monograph Award