The Mathematical Work of David A. Vogan, Jr
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Program of the Sessions San Diego, California, January 9–12, 2013
Program of the Sessions San Diego, California, January 9–12, 2013 AMS Short Course on Random Matrices, Part Monday, January 7 I MAA Short Course on Conceptual Climate Models, Part I 9:00 AM –3:45PM Room 4, Upper Level, San Diego Convention Center 8:30 AM –5:30PM Room 5B, Upper Level, San Diego Convention Center Organizer: Van Vu,YaleUniversity Organizers: Esther Widiasih,University of Arizona 8:00AM Registration outside Room 5A, SDCC Mary Lou Zeeman,Bowdoin upper level. College 9:00AM Random Matrices: The Universality James Walsh, Oberlin (5) phenomenon for Wigner ensemble. College Preliminary report. 7:30AM Registration outside Room 5A, SDCC Terence Tao, University of California Los upper level. Angles 8:30AM Zero-dimensional energy balance models. 10:45AM Universality of random matrices and (1) Hans Kaper, Georgetown University (6) Dyson Brownian Motion. Preliminary 10:30AM Hands-on Session: Dynamics of energy report. (2) balance models, I. Laszlo Erdos, LMU, Munich Anna Barry*, Institute for Math and Its Applications, and Samantha 2:30PM Free probability and Random matrices. Oestreicher*, University of Minnesota (7) Preliminary report. Alice Guionnet, Massachusetts Institute 2:00PM One-dimensional energy balance models. of Technology (3) Hans Kaper, Georgetown University 4:00PM Hands-on Session: Dynamics of energy NSF-EHR Grant Proposal Writing Workshop (4) balance models, II. Anna Barry*, Institute for Math and Its Applications, and Samantha 3:00 PM –6:00PM Marina Ballroom Oestreicher*, University of Minnesota F, 3rd Floor, Marriott The time limit for each AMS contributed paper in the sessions meeting will be found in Volume 34, Issue 1 of Abstracts is ten minutes. -
Orbital Varieties and Unipotent Representations of Classical
Orbital Varieties and Unipotent Representations of Classical Semisimple Lie Groups by Thomas Pietraho M.S., University of Chicago, 1996 B.A., University of Chicago, 1996 Submitted to the Department of Mathematics in partial fulfillment of the requirements for the degree of Doctor of Philosophy at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY June 2001 °c Thomas Pietraho, MMI. All rights reserved. The author hereby grants to MIT permission to reproduce and to distribute publicly paper and electronic copies of this thesis document in whole or in part and to grant others the right to do so. Author ::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: Department of Mathematics April 25, 2001 Certified by :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: David A. Vogan Professor of Mathematics Thesis Supervisor Accepted by :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: Tomasz Mrowka Chairman, Department Committee on Graduate Students 2 Orbital Varieties and Unipotent Representations of Classical Semisimple Lie Groups by Thomas Pietraho Submitted to the Department of Mathematics on April 25, 2001, in partial fulfillment of the requirements for the degree of Doctor of Philosophy Abstract Let G be a complex semi-simple and classical Lie group. The notion of a Lagrangian covering can be used to extend the method of polarizing a nilpotent coadjoint orbit to obtain a unitary representation of G. W. Graham and D. Vogan propose such a construction, relying on the notions of orbital varieties and admissible orbit data. The first part of the thesis seeks to understand the set of orbital varieties contained in a given nipotent orbit. Starting from N. Spaltenstein’s parameterization of the irreducible components of the variety of flags fixed by a unipotent, we produce a parameterization of the orbital varieties lying in the corresponding fiber of the Steinberg map. -
C*-Algebras and Kirillov's Coadjoint Orbit Method
C∗-ALGEBRAS AND KIRILLOV'S COADJOINT ORBIT METHOD DAVID SCHWEIN One of the main goals of representation theory is to understand the unitary dual of a topological group, that is, the set of irreducible unitary representations. Much of modern number theory, for instance, is concerned with describing the unitary duals of various reduc- tive groups over a local field or the adeles, and here our understanding of the representation theory is far from complete. For a different class of groups, the nilpotent Lie groups, A. A. Kirillov gave in the mid- nineteenth century [Kir62] a simple and transparent description of the unitary dual: it is the orbit space under the coadjoint action of the Lie group on the dual of its Lie algebra. The goal of this article, notes for a talk, is to explain Kirillov's result and illustrate it with the Heisenberg group, following Kirillov's excellent and approachable book on the subject [Kir04]. We begin with an introductory section on the unitary dual of a C∗-algebra, the proper setting (currently) for unitary representations of locally compact groups, following Dixmier's exhaustive monograph on C∗-algebras [Dix77]. 1. C∗-algebras and the unitary dual The theory of unitary representations of locally compact topological groups, for instance, reductive p-adic groups, is a special case of the more general theory of representations of C∗-algebras. In this section we review the representation theory of C∗-algebras and see how it specializes to that of topological groups. 1.1. Definitions and examples. A Banach algebra is a Banach space A equipped with an algebra structure with respect to which the norm is sub-multiplicative: ka · bk ≤ kak · kbk; a; b 2 A: We do note require Banach algebras to be unital, and in fact, we will see shortly that there are many natural examples that are not unital. -
Lectures on the Orbit Method, by AA
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 42, Number 4, Pages 535–544 S 0273-0979(05)01065-7 Article electronically published on April 6, 2005 Lectures on the orbit method, by A. A. Kirillov, Graduate Studies in Mathemat- ics, vol. 64, American Mathematical Society, Providence, RI, 2004, xx+408 pp., $65.00, ISBN 0-8218-3530-0 1. Introduction without formulas This book is about a wonderfully successful example of (if you will forgive some geometric language) circular reasoning. Here is the short version. Everywhere in mathematics, we find geometric objects M (like manifolds) that are too complicated for us to understand. One way to make progress is to introduce a vector space V of functions on M.ThespaceV may be infinite-dimensional, but linear algebra is such a powerful tool that we can still say more about the function space V than about the original geometric space M. (With a liberal interpretation of “vector space of functions”, one can include things like the de Rham cohomology of M in this class of ideas.) Often M comes equipped with a group G of symmetries, but G and M may be even less comprehensible together than separately. Nevertheless, G will act on our function space V by change of variables (giving linear transformations), and so we get a representation of G on V . Our original (and impossible) problem of understanding all actions of G on geometric spaces M is therefore at least related to the problem of understanding all representations of G. Because this is a problem about vector spaces, it sounds a bit less daunting. -
1. David Vogan, Massachusetts Institute of Technology Could You
1. David Vogan, Massachusetts Institute of Technology Could you start by giving a biographical sketch? I was born in 1954 in a small town in Pennsylvania, and lived in that state until I went to the University of Chicago. My time at the University of Chicago was mathematically important because it was there that I met Paul Sally, who ended up directing my mathematical career. He did representation theory. he is the reason that I do that too! After getting my undergraduate degree I did what he told me to, which was to go to MIT for graduate school. Lots of people at that time thought that MIT was the place to go for representation theory. I guess it was in 1974 that I went to MIT to work with Kostant. Graduate school is never exactly the way you expected it was going to be. Things went as expected in the sense that I did in fact work with Kostant. However, after less than two years Kostant asked me if I wanted a job. I had been expecting to spend another couple of years in graduate school. I was very happy with this possibility and I had to work a lot faster and harder than I thought I was going to have to work but somehow managed to finish. After that I became an instructor at MIT, only, as it turned out, for one year. Then I spent a couple of years at the Institute for Advanced Study in Princeton. I learned a lot at Princeton. Especially from Greg Zuckerman, who was visiting there and from Armand Borel. -
Sdiff(S ) and the Orbit Method Arxiv:1806.05235V2 [Hep-Th]
SDiff(S2) and the orbit method Robert Penna Institute for Advanced Study, Princeton, NJ 08540, USA E-mail: [email protected] Abstract: The group of area preserving diffeomorphisms of the two sphere, SDiff(S2), is one of the simplest examples of an infinite dimensional Lie group. It plays a key role in incompressible hydrodynamics and it recently appeared in general relativity as a subgroup of two closely related, newly defined symmetry groups. We investi- gate its representation theory using the method of coadjoint orbits. We describe the Casimir functions and the Cartan algebra. Then we evaluate the trace of a simple SDiff(S2) operator using the Atiyah-Bott fixed point formula. The trace is divergent but we show that it has well-defined truncations related to the structure of SDiff(S2). Finally, we relate our results back to the recent appearances of SDiff(S2) in black hole physics. arXiv:1806.05235v2 [hep-th] 27 Nov 2019 Contents 1 Introduction1 2 Labeling the states2 2.1 Coadjoint orbits and Casimir functions3 2.2 SO(3) revisited5 2.3 Cartan algebra6 3 Traces8 3.1 SDiff(S2) 10 3.2 Fixed points 11 3.3 Complex coordinates 11 3.4 Result and discussion 12 4 Discussion 13 1 Introduction The set of area preserving diffeomorphisms of the two-sphere, SDiff(S2), is a basic example of an infinite dimensional Lie group. It is the configuration space and the symmetry group of the incompressible Euler equations for fluid flow on the sphere [1–5]. It may have a role to play in black hole physics, where it is a subgroup of two recently introduced symmetry groups. -
View Front and Back Matter from the Print Issue
Bulletin (New Series) of the American Mathematical Society This journal is devoted to articles of the following types: Research-Expository Surveys These are, by definition, papers that present a clear and insightful exposition of signif- icant aspects of contemporary mathematical research. Gibbs lectures, Progress in Math- ematics lectures, and retiring presidential addresses will be included in this section. Research Reports These are brief, timely reports on important mathematical developments. They are normally solicited and often written by a disinterested expert. Book Reviews Book Reviews are accepted for publication by invitation only. Unsolicited manuscripts will not be considered. Submission information. See Information for Authors at the end of this issue. Publisher Item Identifier. The Publisher Item Identifier (PII) appears at the top of the first page of each article published in this journal. This alphanumeric string of characters uniquely identifies each article and can be used for future cataloging, searching, and electronic retrieval. Subscription information. Bulletin (New Series) of the American Mathematical Society is published quarterly. The Bulletin is also accessible electronically, starting with the January 1992 issue, from e-MATH via the World Wide Web at the URL http : //www.ams.org/publications/. For paper delivery, subscription prices for Vol- ume 36 (1999) are $288 list, $230 institutional member, $173 individual member. The subscription price for members is included in the annual dues. A late charge of 10% of the subscription price will be imposed upon orders received from nonmembers after January 1 of the subscription year. Subscribers outside the United States and India must pay a postage surcharge of $8.00; subscribers in India must pay a postage surcharge of $13.00. -
Quantization, the Orbit Method, and Unitary Representations
Quantization, the orbit method, and unitary representations David Vogan Quantization, the orbit method, and Physics Representations unitary representations Orbit method Hyperbolic orbits Elliptic orbits David Vogan Department of Mathematics Massachusetts Institute of Technology Representation Theory, Geometry, and Quantization: May 28–June 1 2018 Quantization, the Outline orbit method, and unitary representations David Vogan Physics: a view from a neighboring galaxy Physics Representations Orbit method Classical representation theory Hyperbolic orbits Elliptic orbits History of the orbit method in two slides Hyperbolic coadjoint orbits for reductive groups Elliptic coadjoint orbits for reductive groups Quantization, the Quantum mechanics orbit method, and unitary representations David Vogan ! H Physical system complex Hilbert space Physics States ! lines in H Representations Orbit method Observables ! linear operators fAj g on H Hyperbolic orbits Elliptic orbits Expected value of obs A !h Av; vi Energy ! special skew-adjoint operator A0 Time evolution ! unitary group t 7! exp(tA0) Observable A conserved ! [A0; A] = 0 Moral of the story: quantum mechanics is about Hilbert spaces and Lie algebras. Quantization, the Quantum mechanics orbit method, and unitary representations David Vogan ! H Physical system complex Hilbert space Physics States ! lines in H Representations Orbit method Observables ! linear operators fAj g on H Hyperbolic orbits Elliptic orbits Expected value of obs A !h Av; vi Energy ! special skew-adjoint operator A0 Time -
Notes on the Orbit Method and Quantization
Notes on the Orbit Metho d and Quantization Reyer Sjamaar Les Diablerets March 1 Contents Orbit metho d and quantization Index theorem in symplectic geometry 2 Orbit metho d and quantization A A Kirillov G Lie group innitedimensional group quan tum group Category of unitary representations of G Objects continuous homomorphisms T G UH H a Hilb ert space Morphism intertwining op erator from T to T continuous linear A H H A H H T g T g 2 1 A H H 3 Example X Gmanifold with Ginvariant mea sure Unitary representation on L X T g f x f g x Map F X X induces intertwining map F L X L X if is absolutely continuous wrt F T is indecomp osable if T T T for nonzero T and T T is irreducible if do es not have nontrivial invariant subspaces For unitary representation irreducible in decomp osable Unirrep unitary irreducible representation 4 Main problems of representation theory Describ e unitary dual G funirreps of Ggequivalence Decomp ose any T into unirreps Z T g T g dy y Y Sp ecial cases for H G closed littl e group G T a for T G decomp ose restriction Res H G S b for S H decomp ose induction Ind H Compute character of T G 5 Ad b let S H UH Supp ose GH has G G invariant measure Ind S L sections of H H G H Obtained by taking space of functions f G H satisfying f g h S hf g and completing wrt inner product Z hf f i hf x f xi dx H GH Ad let C G Put Z T g T g dg G With luck T H H is of trace class and Tr T is a distribution on G the charac -
Interaction Between Lie Theory and Algebraic Geometry
INTERACTIONS BETWEEN LIE THEORY AND ALGEBRAIC GEOMETRY SHILIN YU 1. Introduction My primary research interests lie in the interactions of complex/algebraic geometry with Lie the- ory and representation theory in the spirit of noncommutative geometry, derived algebraic geometry and mathematical physics. Both Lie theory and algebraic geometry have been at the center of the 20th-century mathematical studies. Entering the 21th century, the two subjects came across each other in a surprising way, due to the phenomenal work of Kontsevich on deformation quantization of Poisson manifolds ([45]) and the birth of derived algebraic geometry ([46]). We start from the following observation: in algebraic geometry, the well-known Grothendieck- Riemann-Roch (GRR) theorem involves the Todd class, which is a characteristic class defined by a certain formal power series. The same type of class also appears in the Atiyah-Singer index theorem, which is a generalization of the Riemann-Roch theorem and one of the most important theorems of the 20th century. On the other hand, the exact same power series also shows up in Lie theory in a fundamental way, long before the GRR theorem was formulated. Namely, it appears in in the differential of the exponential map of a Lie group the Baker-Campbell-Hausdorff (BCH) formula in Lie theory. It (or its inverse) also plays an essential role in the Duflo-Kirillov isomorphism ([28]). Due to the work of many people, including but not limited to Kapranov [40], Kontsevich [45], Markarian [48], and Ramadoss [53], it is now clear that the same power series appearing in the two seemly unrelated cases is not a coincidence. -
Review of “Lectures on the Orbit Method,” by Aa Kirillov
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 00, Number 0, 1997 REVIEW OF \LECTURES ON THE ORBIT METHOD," BY A. A. KIRILLOV DAVID A. VOGAN, JR. Contents 1. Introduction without formulas 2. Introduction with formulas 3. Which orbits count? 4. Kirillov's book 1. Introduction without formulas This book is about a wonderfully successful example of (if you will forgive some geometric language) circular reasoning. Here is the short version. Everywhere in mathematics, we find geometric objects M (like manifolds) that are too complicated for us to understand. One way to make progress is to introduce a vector space V of functions on M. The space V may be infinite-dimensional, but linear algebra is such a powerful tool that we can still say more about the function space V than about the original geometric space M. (With a liberal interpretation of \vector space of functions," one can include things like the de Rham cohomology of M in this class of ideas.) Often M comes equipped with a group G of symmetries, but G and M may be even less comprehensible together than separately. Nevertheless, G will act on our function space V by change of variables (giving linear transformations), and so we get a representation of G on V . Our original (and impossible) problem of understanding all actions of G on geometric spaces M is therefore at least related to the problem of understanding all representations of G. Because this is a problem about vector spaces, it sounds a bit less daunting. The goal of the orbit method is to say something about all representations of a Lie group G. -
P-Mechanics As a Physical Theory: an Introduction
This is a repository copy of p-mechanics as a physical theory: an introduction. White Rose Research Online URL for this paper: http://eprints.whiterose.ac.uk/111528/ Version: Accepted Version Article: Kisil, VV orcid.org/0000-0002-6593-6147 (2004) p-mechanics as a physical theory: an introduction. Journal of Physics A: Mathematical and General, 37 (1). pp. 183-204. ISSN 0305-4470 https://doi.org/10.1088/0305-4470/37/1/013 © 2004 IOP Publishing Ltd. This is an author produced version of an article published in Journal of Physics A: Mathematical and General. Uploaded in accordance with the publisher's self-archiving policy. Reuse Items deposited in White Rose Research Online are protected by copyright, with all rights reserved unless indicated otherwise. They may be downloaded and/or printed for private study, or other acts as permitted by national copyright laws. The publisher or other rights holders may allow further reproduction and re-use of the full text version. This is indicated by the licence information on the White Rose Research Online record for the item. Takedown If you consider content in White Rose Research Online to be in breach of UK law, please notify us by emailing [email protected] including the URL of the record and the reason for the withdrawal request. [email protected] https://eprints.whiterose.ac.uk/ LEEDS-PURE-MATH-200 2 -31, 200 2 arXiv:quant-ph/0212101 p-MECHANICS AS A PHYSICAL THEORY. AN INTRODUCTION VLADIMIR V. KISIL Abstract. The paper provides an introduction into p-mechanics, which is a consistent physical theory suitable for a simultaneous description of classical and quantum mechanics.