Arthur Strong Wightman (1922–2013)
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The Physical Basis of the Direction of Time (The Frontiers Collection), 5Th
the frontiers collection the frontiers collection Series Editors: A.C. Elitzur M.P. Silverman J. Tuszynski R. Vaas H.D. Zeh The books in this collection are devoted to challenging and open problems at the forefront of modern science, including related philosophical debates. In contrast to typical research monographs, however, they strive to present their topics in a manner accessible also to scientifically literate non-specialists wishing to gain insight into the deeper implications and fascinating questions involved. Taken as a whole, the series reflects the need for a fundamental and interdisciplinary approach to modern science. Furthermore, it is intended to encourage active scientists in all areas to ponder over important and perhaps controversial issues beyond their own speciality. Extending from quantum physics and relativity to entropy, consciousness and complex systems – the Frontiers Collection will inspire readers to push back the frontiers of their own knowledge. InformationandItsRoleinNature The Thermodynamic By J. G. Roederer Machinery of Life By M. Kurzynski Relativity and the Nature of Spacetime By V. Petkov The Emerging Physics of Consciousness Quo Vadis Quantum Mechanics? Edited by J. A. Tuszynski Edited by A. C. Elitzur, S. Dolev, N. Kolenda Weak Links Life – As a Matter of Fat Stabilizers of Complex Systems The Emerging Science of Lipidomics from Proteins to Social Networks By O. G. Mouritsen By P. Csermely Quantum–Classical Analogies Mind, Matter and the Implicate Order By D. Dragoman and M. Dragoman By P.T.I. Pylkkänen Knowledge and the World Quantum Mechanics at the Crossroads Challenges Beyond the Science Wars New Perspectives from History, Edited by M. -
Two Arrows of Time in Nonlocal Particle Dynamics
Two Arrows of Time in Nonlocal Particle Dynamics Roderich Tumulka∗ July 21, 2007 Abstract Considering what the world would be like if backwards causation were possible is usually mind-bending. Here I discuss something that is easier to study: a toy model that incorporates a very restricted sort of backwards causation. It defines particle world lines by means of a kind of differential delay equation with negative delay. The model pre- sumably prohibits signalling to the past and superluminal signalling, but allows nonlocality while being fully covariant. And that is what constitutes the model’s value: it is an explicit example of the possi- bility of Lorentz invariant nonlocality. That is surprising in so far as many authors thought that nonlocality, in particular nonlocal laws for particle world lines, must conflict with relativity. The development of this model was inspired by the search for a fully covariant version of Bohmian mechanics. arXiv:quant-ph/0210207v2 18 Sep 2008 In this paper I will introduce to you a dynamical system—a law of mo- tion for point particles—that has been invented [5] as a toy model based on Bohmian mechanics. Bohmian mechanics is a version of quantum mechanics with particle trajectories; see [4] for an introduction and overview. What makes this toy model remarkable is that it has two arrows of time, and that precisely its having two arrows of time is what allows it to perform what it was designed for: to have effects travel faster than light from their causes (in short, nonlocality) without breaking Lorentz invariance. Why should anyone ∗Department of Mathematics, Rutgers University, 110 Frelinghuysen Road, Piscataway, NJ 08854-8019, USA. -
Defining Physics at Imaginary Time: Reflection Positivity for Certain
Defining physics at imaginary time: reflection positivity for certain Riemannian manifolds A thesis presented by Christian Coolidge Anderson [email protected] (978) 204-7656 to the Department of Mathematics in partial fulfillment of the requirements for an honors degree. Advised by Professor Arthur Jaffe. Harvard University Cambridge, Massachusetts March 2013 Contents 1 Introduction 1 2 Axiomatic quantum field theory 2 3 Definition of reflection positivity 4 4 Reflection positivity on a Riemannian manifold M 7 4.1 Function space E over M ..................... 7 4.2 Reflection on M .......................... 10 4.3 Reflection positive inner product on E+ ⊂ E . 11 5 The Osterwalder-Schrader construction 12 5.1 Quantization of operators . 13 5.2 Examples of quantizable operators . 14 5.3 Quantization domains . 16 5.4 The Hamiltonian . 17 6 Reflection positivity on the level of group representations 17 6.1 Weakened quantization condition . 18 6.2 Symmetric local semigroups . 19 6.3 A unitary representation for Glor . 20 7 Construction of reflection positive measures 22 7.1 Nuclear spaces . 23 7.2 Construction of nuclear space over M . 24 7.3 Gaussian measures . 27 7.4 Construction of Gaussian measure . 28 7.5 OS axioms for the Gaussian measure . 30 8 Reflection positivity for the Laplacian covariance 31 9 Reflection positivity for the Dirac covariance 34 9.1 Introduction to the Dirac operator . 35 9.2 Proof of reflection positivity . 38 10 Conclusion 40 11 Appendix A: Cited theorems 40 12 Acknowledgments 41 1 Introduction Two concepts dominate contemporary physics: relativity and quantum me- chanics. They unite to describe the physics of interacting particles, which live in relativistic spacetime while exhibiting quantum behavior. -
April 2010 Contents
International Association of Mathematical Physics News Bulletin April 2010 Contents International Association of Mathematical Physics News Bulletin, April 2010 Contents Reflections on the IAMP Geography 3 Aharonov-Bohm & Berry Phase Anniversaries 50/25 5 The 25th anniversary of the founding of HARL 8 An interview with Huzihiro Araki 10 Shing-Tung Yau the Wolf Prize laureate 2010 in Mathematics 14 News from the IAMP Executive Committee 22 A new associated member: PIMS 26 Bulletin editor Valentin Zagrebnov Editorial board Evans Harrell, Masao Hirokawa, David Krejˇciˇr´ık, Jan Philip Solovej Contacts [email protected] http://www.iamp.org Cover photo (courtesy of Professor A.Tonomura): From double-slit experiment to the Aharonov-Bohm effect. See a comment at the end of the page 7. The views expressed in this IAMP News Bulletin are those of the authors and do not necessary represent those of the IAMP Executive Committee, Editor or Editorial board. Any complete or partial performance or reproduction made without the consent of the author or of his successors in title or assigns shall be unlawful. All reproduction rights are henceforth reserved, mention of the IAMP News Bulletin is obligatory in the reference. (Art.L.122-4 of the Code of Intellectual Property). 2 IAMP News Bulletin, April 2010 Editorial Reflections on the IAMP Geography by Pavel Exner (IAMP President) The topic of today’s meditation was inspired by complaints of American colleagues about the shaky position our discipline enjoys in the U.S. True, such woes are ubiquitous since com- petition for resources in science was and will always be tough. -
Mathematisches Forschungsinstitut Oberwolfach Reflection Positivity
Mathematisches Forschungsinstitut Oberwolfach Report No. 55/2017 DOI: 10.4171/OWR/2017/55 Reflection Positivity Organised by Arthur Jaffe, Harvard Karl-Hermann Neeb, Erlangen Gestur Olafsson, Baton Rouge Benjamin Schlein, Z¨urich 26 November – 2 December 2017 Abstract. The main theme of the workshop was reflection positivity and its occurences in various areas of mathematics and physics, such as Representa- tion Theory, Quantum Field Theory, Noncommutative Geometry, Dynamical Systems, Analysis and Statistical Mechanics. Accordingly, the program was intrinsically interdisciplinary and included talks covering different aspects of reflection positivity. Mathematics Subject Classification (2010): 17B10, 22E65, 22E70, 81T08. Introduction by the Organisers The workshop on Reflection Positivity was organized by Arthur Jaffe (Cambridge, MA), Karl-Hermann Neeb (Erlangen), Gestur Olafsson´ (Baton Rouge) and Ben- jamin Schlein (Z¨urich) during the week November 27 to December 1, 2017. The meeting was attended by 53 participants from all over the world. It was organized around 24 lectures each of 50 minutes duration representing major recent advances or introducing to a specific aspect or application of reflection positivity. The meeting was exciting and highly successful. The quality of the lectures was outstanding. The exceptional atmosphere of the Oberwolfach Institute provided the optimal environment for bringing people from different areas together and to create an atmosphere of scientific interaction and cross-fertilization. In particular, people from different subcommunities exchanged ideas and this lead to new col- laborations that will probably stimulate progress in unexpected directions. 3264 Oberwolfach Report 55/2017 Reflection positivity (RP) emerged in the early 1970s in the work of Osterwalder and Schrader as one of their axioms for constructive quantum field theory ensuring the equivalence of their euclidean setup with Wightman fields. -
Partial Differential Equations
CALENDAR OF AMS MEETINGS THIS CALENDAR lists all meetings which have been approved by the Council pnor to the date this issue of the Nouces was sent to press. The summer and annual meetings are joint meetings of the Mathematical Association of America and the Ameri· can Mathematical Society. The meeting dates which fall rather far in the future are subject to change; this is particularly true of meetings to which no numbers have yet been assigned. Programs of the meetings will appear in the issues indicated below. First and second announcements of the meetings will have appeared in earlier issues. ABSTRACTS OF PAPERS presented at a meeting of the Society are published in the journal Abstracts of papers presented to the American Mathematical Society in the issue corresponding to that of the Notices which contains the program of the meet ing. Abstracts should be submitted on special forms which are available in many departments of mathematics and from the office of the Society in Providence. Abstracts of papers to be presented at the meeting must be received at the headquarters of the Society in Providence, Rhode Island, on or before the deadline given below for the meeting. Note that the deadline for ab stracts submitted for consideration for presentation at special sessions is usually three weeks earlier than that specified below. For additional information consult the meeting announcement and the list of organizers of special sessions. MEETING ABSTRACT NUMBER DATE PLACE DEADLINE ISSUE 778 June 20-21, 1980 Ellensburg, Washington APRIL 21 June 1980 779 August 18-22, 1980 Ann Arbor, Michigan JUNE 3 August 1980 (84th Summer Meeting) October 17-18, 1980 Storrs, Connecticut October 31-November 1, 1980 Kenosha, Wisconsin January 7-11, 1981 San Francisco, California (87th Annual Meeting) January 13-17, 1982 Cincinnati, Ohio (88th Annual Meeting) Notices DEADLINES ISSUE NEWS ADVERTISING June 1980 April 18 April 29 August 1980 June 3 June 18 Deadlines for announcements intended for the Special Meetings section are the same as for News. -
6. L CPT Reversal
6. CPT reversal l Précis. On the representation view, there may be weak and strong arrows of time. A weak arrow exists. A strong arrow might too, but not in current physics due to CPT symmetry. There are many ways to reverse time besides the time reversal operator T. Writing P for spatial reflection or ‘parity’, and C for matter-antimatter exchange or ‘charge conjugation’, we find that PT, CT, and CPT are all time reversing transformations, when they exist. More generally, for any non-time-reversing (unitary) transformation U, we find that UT is time reversing. Are any of these transformations relevant for the arrow of time? Feynman (1949) captured many of our imaginations with the proposal that to understand the direction of time, we must actually consider the exchange of matter and antimatter as well.1 Writing about it years later, he said: “A backwards-moving electron when viewed with time moving forwards appears the same as an ordinary electron, except it’s attracted to normal electrons — we say it has positive charge. For this reason it’s called a ‘positron’. The positron is a sister to the electron, and it is an example of an ‘anti-particle’. This phenomenon is quite general. Every particle in Nature has an amplitude to move backwards in time, and therefore has an anti-particle.”(Feynman 1985, p.98) Philosophers Arntzenius and Greaves (2009, p.584) have defended Feynman’s proposal, 1In his Nobel prize speech, Feynman (1972, pg.163) attributes this idea to Wheeler in the development of their absorber theory (Wheeler and Feynman 1945). -
On the Geometry of the Spin-Statistics Connection in Quantum Mechanics
On the Geometry of the Spin-Statistics Connection in Quantum Mechanics Dissertation zur Erlangung des Grades ,,Doktor der Naturwissenschaften“ am Fachbereich Physik der Johannes Gutenberg-Universit¨at Mainz vorgelegt von Andr´es Reyes geb. in Bogot´a Mainz 2006 Zusammenfassung Das Spin-Statistik-Theorem besagt, dass das statistische Verhalten eines Systems von identischen Teilchen durch deren Spin bestimmt ist: Teilchen mit ganzzahligem Spin sind Bosonen (gehorchen also der Bose-Einstein-Statistik), Teilchen mit halbzahligem Spin hingegen sind Fermionen (gehorchen also der Fermi-Dirac-Statistik). Seit dem urspr¨unglichen Beweis von Fierz und Pauli wissen wir, dass der Zusammenhang zwi- schen Spin und Statistik aus den allgemeinen Prinzipien der relativistischen Quanten- feldtheorie folgt. Man kann nun die Frage stellen, ob das Theorem auch dann noch g¨ultig bleibt, wenn man schw¨achere Annahmen macht als die allgemein ¨ublichen (z.B. Lorentz- Kovarianz). Es gibt die verschiedensten Ans¨atze, die sich mit der Suche nach solchen schw¨acheren Annahmen besch¨aftigen. Neben dieser Suche wurden ¨uber viele Jahre hinweg Versuche unternommen einen geometrischen Beweis f¨ur den Zusammenhang zwischen Spin und Statistik zu finden. Solche Ans¨atze werden haupt- s¨achlich, durch den tieferen Zusammenhang zwischen der Ununterscheidbarkeit von identischen Teilchen und der Geometrie des Konfigurationsraumes, wie man ihn beispielsweise an dem Gibbs’schen Paradoxon sehr deutlich sieht, motiviert. Ein Ver- such der diesen tieferen Zusammenhang ausnutzt, um ein geometrisches Spin- Statistik-Theorem zu beweisen, ist die Konstruktion von Berry und Robbins (BR). Diese Konstruktion basiert auf einer Eindeutigkeitsbedingung der Wellenfunktion, die Aus- gangspunkt erneuerten Interesses an diesem Thema war. Die vorliegende Arbeit betrachtet das Problem identischer Teilchen in der Quanten- mechanik von einem geometrisch-algebraischen Standpunkt. -
1995 Steele Prizes
steele.qxp 4/27/98 3:29 PM Page 1288 1995 Steele Prizes Three Leroy P. Steele Prizes were presented at The text that follows contains, for each award, the awards banquet during the Summer Math- the committee’s citation, the recipient’s response fest in Burlington, Vermont, in early August. upon receiving the award, and a brief bio- These prizes were established in 1970 in honor graphical sketch of the recipient. of George David Birkhoff, William Fogg Osgood, and William Caspar Graustein Edward Nelson: 1995 Steele Prize for and are endowed under the Seminal Contribution to Research terms of a bequest from The 1995 Leroy P. Steele award for research of Leroy P. Steele. seminal importance goes to Professor Edward The Steele Prizes are Nelson of Princeton University for the following ...for a research awarded in three categories: two papers in mathematical physics character- for a research paper of fun- ized by leaders of the field as extremely innov- paper of damental and lasting impor- ative: tance, for expository writing, 1. “A quartic interaction in two dimensions” in fundamental and for cumulative influence Mathematical Theory of Elementary Particles, and lasting extending over a career, in- MIT Press, 1966, pages 69–73; cluding the education of doc- 2. “Construction of quantum fields from Markoff importance, toral students. The current fields” in Journal of Functional Analysis 12 award is $4,000 in each cate- (1973), 97–112. for expository gory. In these papers he showed for the first time The recipients of the 1995 how to use the powerful tools of probability writing, and for Steele Prizes are Edward Nel- theory to attack the hard analytic questions of son for seminal contribution constructive quantum field theory, controlling cumulative to research, Jean-Pierre Serre renormalizations with Lp estimates in the first influence for mathematical exposition, paper and, in the second, turning Euclidean and John T. -
Solutions in Constructive Field Theory
Solutions in Constructive Field Theory Leif Hancox-Li ∗ [email protected] June 7, 2016 Abstract Constructive field theory aims to rigorously construct concrete, non-trivial solutions to Lagrangians used in particle physics, where the solutions satisfy some relevant set of axioms. I examine the relationship of solutions in constructive field theory to both axiomatic and Lagrangian quantum field theory (QFT). I argue that Lagrangian QFT provides conditions for what counts as a successful constructive solution, and that it provides other information that guides constructive field theorists to solutions. Solutions matter because they describe the behavior of QFT systems, and thus what QFT says the world is like. Constructive field theory, in incorporating ingredients from both axiomatic and Lagrangian QFT, clarifies existing disputes about which parts of QFT are philosophically relevant and how rigor relates to these disputes. ∗I thank Bob Batterman and Michael Miller for comments and encouragement. Several anonymous referees also contribued valuable comments. Copyright Philosophy of Science 2016 Preprint (not copyedited or formatted) Please use DOI when citing or quoting 1 Introduction To date, philosophers of quantum field theory (QFT) have paid much attention to roughly two kinds of QFT: axiomatic approaches to algebraic QFT (Halvorson and Muger,¨ 2006), and Lagrangian-based QFT as used by particle physicists (Wallace, 2006). Comparatively less attention, however, has been paid to constructive QFT, an approach that aims to rigorously construct non-trivial solutions of QFT for Lagrangians and Hamiltonians that are important in particle physics, ensuring that such solutions satisfy certain axioms. In doing so, constructive QFT mediates between axiomatic approaches to QFT and physicists’ Lagrangian-based QFT. -
Finite Dimensional Systems of Free Fermions and Diffusion Processes
Finite dimensional systems of free Fermions and diffusion processes on Spin groups Luigi M. Borasi Hausdorff Center of Mathematics & Institute of Applied Mathematics University of Bonn, Germany [email protected] February 2, 2021 Abstract In this article we are concerned with “finite dimensional Fermions”, by which we mean vectors in a finite dimensional complex space embedded in the exterior algebra over itself. These Fermions are spinless but possess the characterizing anticommutativity property. We associate invariant com- plex vector fields on the Lie group Spin(2n + 1) to the Fermionic creation and annihilation operators. These vector fields are elements of the com- plexification of the regular representation of the Lie algebra so(2n + 1). As such, they do not satisfy the canonical anticommutation relations, however, once they have been projected onto an appropriate subspace of L2(Spin(2n + 1)), these relations are satisfied. We define a free time evo- lution of this system of Fermions in terms of a symmetric positive-definite quadratic form in the creation-annihilation operators. The realization of Fermionic creation and annihilation operators brought by the (invariant) vector fields allows us to interpret this time evolution in terms of a pos- itive selfadjoint operator which is the sum of a second order operator, which generates a stochastic diffusion process, and a first order complex operator, which strongly commutes with the second order operator. A probabilistic interpretation is given in terms of a Feynman-Kac like for- mula with respect to the diffusion process associated with the second order operator. arXiv:2102.01000v1 [math-ph] 1 Feb 2021 1 Introduction Probabilistic methods in Quantum Field Theory have proved to be particu- larly fruitful (cf. -
William A. Hiscock Michio Kaku Gordon Kane J-M Wersinger
WILLIAM A. HISCOCK From Wormholes to the Warp Drive: Using Theoretical Physics to Place Ultimate Bounds on Technology MICHIO KAKU M-Theory: Mother of All Superstrings GORDON KANE Anthropic Questions Peering into the Universe: Images from the Hubble Space Telescope J-M WERSINGER The National Space Grant Student Satellite Program: Crawl, Walk, Run, Fly! The Honor Society of Phi Kappa Phi was founded in 1897 and became a national organization Board of Directors through the efforts of the presidents of three state Wendell H. McKenzie, PhD universities. Its primary objective has been from National President the first the recognition and encouragement of Dept. of Genetics superior scholarship in all fields of study. Good Box 7614 NCSU character is an essential supporting attribute for Raleigh, NC 27695 those elected to membership. The motto of the Paul J. Ferlazzo, PhD Society is philosophia krateit¯oph¯ot¯on, which is National President-Elect freely translated as “Let the love of learning rule Northern Arizona University Phi Kappa Phi Forum Staff humanity.” Dept. of English, Bx 6032 Flagstaff, AZ 86011 Editor: JAMES P. KAETZ Donna Clark Schubert National Vice President Associate Editors: Troy State University Phi Kappa Phi encourages and recognizes aca- 101 C Wallace Hall STEPHANIE J. BOND demic excellence through several national pro- Troy, AL 36082 LAURA J. KLOBERG grams. Its flagship National Fellowship Program now awards more than $460,000 each year to Neil R. Luebke, PhD Copy Editor: student members for the first year of graduate Past President 616 W. Harned Ave. AMES ARRS study. In addition, the Society funds Study J T.