Foundations of Mathematics and Physics One Century After Hilbert: New Perspectives Edited by Joseph Kouneiher
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Full Program, with Speakers
Frontiers of Fundamental Physics 14 Marseille, July 15–18, 2014 Program and Speakers Updated on January 8, 2015 1 Program, July, 15 08h00 – 08h45 Conference Registration, Room “Salle de Conférences” 08h45 – 10h30 Plenary session Plenary Session (broadcast) Chairman: Eric Kajfasz Amphi “Sciences Naturelles” 08h45 – 09h00 Roland Triay (CPT) Opening 09h00 – 09h30 Gabriele Veneziano (CdF) Personal reflections on two success stories 09h30 – 10h00 Paraskevas Sphicas (CERN and Athens) Status of HEP after the LHC Run 1 10h00 – 10h30 Subir Sarkar (UOXF & NBI) Program Discovering dark matter 10h30 – 11h00 Coffee break July, 15 11h00 – 12h30 Morning parallel plenary sessions Plenary Session 1 The visible universe (broadcast) Chairman: François Bouchet Amphi “Sciences Naturelles” 11h00 – 11h30 Enrique Gaztañaga (ICE, IEEC-CSIC) LSS with angular cross-correlations: Combining Spectroscopic and Photometric Surveys 11h30 – 12h00 Adi Nusser (IIT) Dynamics of the Cosmic Web 12h00 – 12h30 Pierre Astier (LPNHE) Distances to supernovae: an efficient probe of dark energy Plenary Session 2 New Geometries for Physics Chairman: Fedele Lizzi Amphi “Massiani” 11h00 – 11h45 Ali Chamseddine (AUB and IHES) Geometric Unification 11h45 – 12h30 Pierre Bieliavsky (UCLouvain) Geometrical aspects of deformation quantization Plenary Session 3 Gravitation and the Quantum Chairman: Jerzy Lewandowski Amphi “Charve” 11h00 – 11h45 Walter Greiner (FIAS) There are no black holes: Pseudo-Complex General Relativity From Einstein to Zweistein 11h45 – 12h30 Eugenio Bianchi (Penn State) -
Detailing Coherent, Minimum Uncertainty States of Gravitons, As
Journal of Modern Physics, 2011, 2, 730-751 doi:10.4236/jmp.2011.27086 Published Online July 2011 (http://www.SciRP.org/journal/jmp) Detailing Coherent, Minimum Uncertainty States of Gravitons, as Semi Classical Components of Gravity Waves, and How Squeezed States Affect Upper Limits to Graviton Mass Andrew Beckwith1 Department of Physics, Chongqing University, Chongqing, China E-mail: [email protected] Received April 12, 2011; revised June 1, 2011; accepted June 13, 2011 Abstract We present what is relevant to squeezed states of initial space time and how that affects both the composition of relic GW, and also gravitons. A side issue to consider is if gravitons can be configured as semi classical “particles”, which is akin to the Pilot model of Quantum Mechanics as embedded in a larger non linear “de- terministic” background. Keywords: Squeezed State, Graviton, GW, Pilot Model 1. Introduction condensed matter application. The string theory metho- dology is merely extending much the same thinking up to Gravitons may be de composed via an instanton-anti higher than four dimensional situations. instanton structure. i.e. that the structure of SO(4) gauge 1) Modeling of entropy, generally, as kink-anti-kinks theory is initially broken due to the introduction of pairs with N the number of the kink-anti-kink pairs. vacuum energy [1], so after a second-order phase tran- This number, N is, initially in tandem with entropy sition, the instanton-anti-instanton structure of relic production, as will be explained later, gravitons is reconstituted. This will be crucial to link 2) The tie in with entropy and gravitons is this: the two graviton production with entropy, provided we have structures are related to each other in terms of kinks and sufficiently HFGW at the origin of the big bang. -
Coll055-Endmatter.Pdf
http://dx.doi.org/10.1090/coll/055 America n Mathematica l Societ y Colloquiu m Publication s Volum e 55 Noncommutativ e Geometry , Quantu m Field s an d Motive s Alai n Conne s Matild e Marcoll i »AMS AMERICAN MATHEMATICA L SOCIET Y öUöi HINDUSTA N SJU BOOKAGENC Y Editorial Boar d Paul J . Sally , Jr., Chai r Yuri Mani n Peter Sarna k 2000 Mathematics Subject Classification. Primar y 58B34 , 11G35 , 11M06 , 11M26 , 11G09 , 81T15, 14G35 , 14F42 , 34M50 , 81V25 . This editio n i s published b y th e America n Mathematica l Societ y under licens e fro m Hindusta n Boo k Agency . For additiona l informatio n an d Update s o n thi s book , visi t www.ams.org/bookpages/coll-55 Library o f Congres s Cataloging-in-Publicatio n Dat a Connes, Alain . Noncommutative geometry , quantu m fields an d motive s / Alai n Connes , Matild e Marcolli , p. cm . — (Colloquiu m publication s (America n Mathematica l Society) , ISS N 0065-925 8 ; v. 55 ) Includes bibliographica l reference s an d index . ISBN 978-0-8218-4210- 2 (alk . paper ) 1. Noncommutativ e differentia l geometry . 2 . Quantu m field theory , I . Marcolli , Matilde . IL Title . QC20.7.D52C66 200 7 512/.55—dc22 200706084 3 Copying an d reprinting . Individua l reader s o f thi s publication , an d nonprofi t librarie s acting fo r them , ar e permitted t o mak e fai r us e o f the material , suc h a s to cop y a chapte r fo r us e in teachin g o r research . -
Noncommutative Geometry Models for Particle Physics and Cosmology, Lecture I
Noncommutative Geometry models for Particle Physics and Cosmology, Lecture I Matilde Marcolli Villa de Leyva school, July 2011 Matilde Marcolli NCG models for particles and cosmology, I Plan of lectures 1 Noncommutative geometry approach to elementary particle physics; Noncommutative Riemannian geometry; finite noncommutative geometries; moduli spaces; the finite geometry of the Standard Model 2 The product geometry; the spectral action functional and its asymptotic expansion; bosons and fermions; the Standard Model Lagrangian; renormalization group flow, geometric constraints and low energy limits 3 Parameters: relations at unification and running; running of the gravitational terms; the RGE flow with right handed neutrinos; cosmological timeline and the inflation epoch; effective gravitational and cosmological constants and models of inflation 4 The spectral action and the problem of cosmic topology; cosmic topology and the CMB; slow-roll inflation; Poisson summation formula and the nonperturbative spectral action; spherical and flat space forms Matilde Marcolli NCG models for particles and cosmology, I Geometrization of physics Kaluza-Klein theory: electromagnetism described by circle bundle over spacetime manifold, connection = EM potential; Yang{Mills gauge theories: bundle geometry over spacetime, connections = gauge potentials, sections = fermions; String theory: 6 extra dimensions (Calabi-Yau) over spacetime, strings vibrations = types of particles NCG models: extra dimensions are NC spaces, pure gravity on product space becomes gravity -
Dirac Operators: Yesterday and Today
Dirac Operators: Yesterday and Today Dirac Operators: Yesterday and Today Proceedings of the Summer School & Workshop Center for Advanced Mathematical Sciences American University of Beirut, Lebanon August 27 to September 7, 2001 edited by Jean-Pierre Bourguignon Thomas Branson Ali Chamseddine Oussama Hijazi Robert J. Stanton International Press www.intlpress.com Dirac Operators: Yesterday and Today Editors: Jean-Pierre Bourguignon Thomas Branson Ali Chamseddine Oussama Hijazi Robert J. Stanton Copyright © 2005, 2010 by International Press Somerville, Massachusetts, U.S.A. All rights reserved. Individual readers of this publication, and non-profit libraries acting for them, are permitted to make fair use of the material, such as to copy a chapter for use in teaching or research. Permission is granted to quote brief passages from this publication in reviews, provided the customary acknowledgement of the source is given. Republication, systematic copying, or mass reproduction of any material in this publication is permitted only under license from International Press. ISBN 978-1-57146-184-1 Paperback reissue 2010. Previously published in 2005 under ISBN 1-57146-175-2 (clothbound). Typeset using the LaTeX system. v Preface The Summer School ”Dirac Operators: Yesterday and Today” was an ambitious endeavour to show to a public of advanced students a tableau of modern mathematics. The idea was to make available a topic, of considerable importance for mathematics itself because of its deep impact on many mathematical questions, but also for its interactions with one of mathematics historic partners, physics. The Dirac operator was undoubtedly created by Paul Adrien Maurice Dirac to deal with an important physical question. -
JHEP08(2020)001 Springer July 7, 2020 May 29, 2020
Published for SISSA by Springer Received: March 10, 2019 Revised: May 29, 2020 Accepted: July 7, 2020 Published: August 4, 2020 Four-dimensional gravity on a covariant noncommutative space JHEP08(2020)001 G. Manolakos,a P. Manousselisa and G. Zoupanosa;b;c;d aPhysics Department, National Technical University, Zografou Campus 9, Iroon Polytechniou str, GR-15780 Athens, Greece bInstitute of Theoretical Physics, D-69120 Heidelberg, Germany cMax-Planck Institut f¨urPhysik, Fohringer Ring 6, D-80805 Munich, Germany dLaboratoire d' Annecy de Physique Theorique, Annecy, France E-mail: [email protected], [email protected], [email protected] Abstract: We formulate a model of noncommutative four-dimensional gravity on a co- variant fuzzy space based on SO(1,4), that is the fuzzy version of the dS4. The latter requires the employment of a wider symmetry group, the SO(1,5), for reasons of covari- ance. Addressing along the lines of formulating four-dimensional gravity as a gauge theory of the Poincar´egroup, spontaneously broken to the Lorentz, we attempt to construct a four-dimensional gravitational model on the fuzzy de Sitter spacetime. In turn, first we consider the SO(1,4) subgroup of the SO(1,5) algebra, in which we were led to, as we want to gauge the isometry part of the full symmetry. Then, the construction of a gauge theory on such a noncommutative space directs us to use an extension of the gauge group, the SO(1,5)×U(1), and fix its representation. Moreover, a 2-form dynamic gauge field is included in the theory for reasons of covariance of the transformation of the field strength tensor. -
Curriculum Vitae
SEBASTIAN DE HARO Curriculum Vitae Assistant Professor in Philosophy of Science at the Institute for Logic, Language and Computation and the Institute of Physics of the University of Amsterdam 1. RESEARCH PROFILE Areas of specialisation: Philosophy of Science, History and Philosophy of Physics, Theoretical Physics Areas of competence: Epistemology, Metaphysics, Ethics, Philosophical and Social Aspects of Information, History of Science, History of Philosophy, Philosophy of Logic and Language, Philosophy of Mathematics 2. PREVIOUS POSITIONS • Lecturer (2009-2020), Amsterdam University College (AUC), University of Amsterdam. Tasks: teaching, curriculum development and evaluation, thesis supervision, member of the BSA committee. Between 2009-2015 I also had tutoring responsibilities. • Lecturer (2019-2020, fixed term), Department of Philosophy, Free University Amsterdam • Lecturer in theoretical physics (fixed term), Institute for Theoretical Physics, Faculty of Science, University of Amsterdam. Teaching, research, thesis supervision. 02/12 - 07/14. • Research associate. Managing editor of Foundations of Physics on behalf of Gerard ’t Hooft, Spinoza Institute/ITP, Utrecht University and Springer Verlag, 2008-2009. Research, managing editorial office, setting up new projects, contact Editorial Board. 3. PUBLICATIONS Total number of citations (all publications): 2,751. i10-index: 33. h-index: 22 Full list of publications and citation information via Google scholar profile: http://scholar.google.nl/citations?user=rmXDqN4AAAAJ&hl=nl&oi=ao Journal articles, book chapters, and book reviews General philosophy of science: journal articles (6) 1. ‘The Empirical Under-determination Argument Against Scientific Realism for Dual Theories’. Erkenntnis, 2021. https://link.springer.com/article/10.1007%2Fs10670-020-00342-0 2. ‘Science and Philosophy: A Love-Hate Relationship’. -
Foundations of Quantum Physics I. a Critique of the Tradition
Foundations of quantum physics I. A critique of the tradition Arnold Neumaier Fakult¨at f¨ur Mathematik, Universit¨at Wien Oskar-Morgenstern-Platz 1, A-1090 Wien, Austria email: [email protected] http://www.mat.univie.ac.at/~neum April 24, 2019 Abstract. This paper gives a thorough critique of the foundations of quantum physics in its mainstream interpretation (i.e., treating pure states and probability as primitives, without reference to hidden variables, and without modifications of the quantum laws). This is achieved by cleanly separating a concise version of the (universally accepted) for- mal core of quantum physics from the (controversial) interpretation issues. The latter are primarily related to measurement, but also to questions of existence and of the meaning of basic concepts like ’state’ and ’particle’. The requirements for good foundations of quantum physics are discussed. Main results: • Born’s rule cannot be valid universally, and must be considered as a scientific law with a restricted domain of validity. • If the state of every composite quantum system contains all information that can be known about this system, it cannot be a pure state in general. For the discussion of questions related to this paper, please use the discussion forum https://www.physicsoverflow.org. 1 Contents 1 Introduction 3 2 Thetraditionalfoundationsofquantumphysics 4 2.1 Postulates for the formal core of quantum physics . ......... 5 2.2 Thepurestateidealization. .... 6 2.3 Schr¨odingerequationandBorn’srule . ....... 7 2.4 Interpretingtheformalcore . .... 9 3 A critique of Born’s rule 10 3.1 Early, measurement-free formulations of Born’s rule . ............ 11 3.2 Formulations of Born’s rule in terms of measurement . -
Arxiv:Gr-Qc/0601043V3 2 Dec 2006 Can Gravitons Be Detected?
Can Gravitons Be Detected? Tony Rothman ∗ and Stephen Boughn† ∗ Princeton University, Princeton, NJ 08544 † Haverford College, Haverford, PA 19041 LATEX-ed February 4, 2008 Abstract Freeman Dyson has questioned whether any conceivable experiment in the real universe can detect a single graviton. If not, is it meaningful to talk about gravitons as physical entities? We attempt to answer Dyson’s question and find it is possible concoct an idealized thought experiment capable of detecting one graviton; however, when anything remotely resembling realistic physics is taken into account, detection becomes impossible, indicating that Dyson’s conjecture is very likely true. We also point out several mistakes in the literature dealing with graviton detection and production. arXiv:gr-qc/0601043v3 2 Dec 2006 PACS: .03.65.Sq, .04.30.Db, .04.30.Nk, .04.80.Cc, .04.80.Nn, 95.30.Cq Keywords: Gravitons, Gravitational Waves, Gravitational Bremsstrahlung, Graviton- electron Cross Sections. 1 Introduction The search for gravitational waves, one of the central predictions of general relativity, has been ongoing for several decades. Strong indirect evidence for their existence comes from the timing of the orbital decay rate of the binary pulsar PSR1913+16, and with the completion of LIGO II and other gravity-wave observatories, researchers expect a direct detection. Gravitons themselves present a thornier issue. Although physicists routinely speak as if bosons mediating the gravitational force exist, the extraordinary weakness of the gravitational interaction makes the detection of one ∗[email protected] †[email protected] 1 Gravitons ... 2 gravitational quantum a remote proposition. Recently, Dyson[1] has suggested that detection of a single graviton may in fact be ruled out in the real universe. -
Philosophy and Foundations of Physics Series Editors: Dennis Dieks and Miklos Redei
Philosophy and Foundations of Physics Series Editors: Dennis Dieks and Miklos Redei In this series: Vol. 1: The Ontology of Spacetime Edited by Dennis Dieks Vol. 2: The Structure and Interpretation of the Standard Model By Gordon McCabe Vol. 3: Symmetry, Structure, and Spacetime By Dean Rickles Vol. 4: The Ontology of Spacetime II Edited by Dennis Dieks The Ontology of Spacetime II Edited by Dennis Dieks Institute for History and Foundations of Science Utrecht University Utrecht, The Netherlands Amsterdam – Boston – Heidelberg – London – New York – Oxford – Paris San Diego – San Francisco – Singapore – Sydney – Tokyo Elsevier Radarweg 29, PO Box 211, 1000 AE Amsterdam, The Netherlands The Boulevard, Langford Lane, Kidlington, Oxford OX5 1GB, UK First edition 2008 Copyright © 2008 Elsevier B.V. All rights reserved No part of this publication may be reproduced, stored in a retrieval system or transmitted in any form or by any means electronic, mechanical, photocopying, recording or otherwise without the prior written permission of the publisher Permissions may be sought directly from Elsevier’s Science & Technology Rights Department in Oxford, UK: phone (+44) (0) 1865 843830; fax (+44) (0) 1865 853333; email: [email protected]. Alternatively you can submit your request online by visiting the Elsevier web site at http://elsevier.com/locate/permissions, and selecting Obtaining permission to use Elsevier material Notice No responsibility is assumed by the publisher for any injury and/or damage to persons or property as a matter of products liability, negligence or otherwise, or from any use or operation of any methods, products, instructions or ideas contained in the material herein. -
Mimetic Gravity
Mimetic Gravity Ali Chamseddine American University of Beirut, Lebanon & Radboud University Excellence Professor Modern Trends in Particle Physics, Nathfest 80, May 17 2019, Northeastern University, Boston, MA. Modified Gravity • Modifications of gravity in most cases involve adding new fields. • Modifications of GR or adding new fields are needs to solve well known problems in cosmology, such as adding an inflaton, curvaton, quintessence, or F( R) gravity (equivalent to φR+ f(φ) ) or as in Hordinski model using scalar with higher safe derivatives. • In some modified theories utilize breaking diffeomorphism invariance such as in unimodular gravity, or Horava‐Lifschitz gravity Dark Matter • Various new particles and interactions are proposed to account for the missing mostly non‐baryonic matter in the universe. • Examples: Supersymmetric neutralino, axions, WIMP, dilaton, • Lack of direct evidence for dark matter made some physicists to propose modification of GR at large scales. • Most modifications of GR are made to solve one problem at a time, and do not address solving the problems simultaneously. Scale factor for metric • GR is not invariant under scale transformations of the metric • Newton constant will be redefined. If we take Ω(x) then it will get kinetic term. It is related to determinant of metric. • Unimodular gravity assumes |det(g)|=1 breaking diffeomorphism Invariance. Scale factor • In string theory the metric is accompanied by a dilaton and axionin the form of antisymmetric tensor. New degrees of freedom. • How can one isolate physics of scaling factor? • Let Then it is scale invariant under This imply Mimetic gravity (with S. Mukhanov) • The system ( has 11 components subject to the constraint leaving 10 degrees, same as GR. -
Non-Commutative Geometry, Non-Associative Geometry and the Standard Model of Particle Physics
Non-commutative geometry, non-associative geometry and the standard model of particle physics Latham Boyle and Shane Farnsworth Perimeter Institute for Theoretical Physics, Waterloo, Ontario N2L 2Y5, Canada Received 1 October 2014 Accepted for publication 28 October 2014 Published 10 December 2014 New Journal of Physics 16 (2014) 123027 doi:10.1088/1367-2630/16/12/123027 Abstract Connes’ notion of non-commutative geometry (NCG) generalizes Riemannian geometry and yields a striking reinterepretation of the standard model of particle physics, coupled to Einstein gravity. We suggest a simple reformulation with two key mathematical advantages: (i) it unifies many of the traditional NCG axioms into a single one; and (ii) it immediately generalizes from non-com- mutative to non-associative geometry. Remarkably, it also resolves a long- standing problem plaguing the NCG construction of the standard model, by precisely eliminating from the action the collection of seven unwanted terms that previously had to be removed by an extra, non-geometric, assumption. With this problem solved, the NCG algorithm for constructing the standard model action is tighter and more explanatory than the traditional one based on effective field theory. Keywords: non-commutative geometry, non-associative geometry, standard model of particle physics Introduction Since the early 1980s, Connes and others have been developing the subject of non-commutative geometry (NCG) [1, 2]. Its mathematical interest stems from the fact that it provides a natural generalization of Riemannian geometry (much as Riemannian geometry, in turn, provides a natural generalization of Euclidean geometry). Its physical interest stems from the fact that it Content from this work may be used under the terms of the Creative Commons Attribution 3.0 licence.