Reduction and Emergence in the Physical Sciences: Some Lessons from the Particle Physics and Condensed Matter Debate
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Symmetry and Ergodicity Breaking, Mean-Field Study of the Ising Model
Symmetry and ergodicity breaking, mean-field study of the Ising model Rafael Mottl, ETH Zurich Advisor: Dr. Ingo Kirsch Topics Introduction Formalism The model system: Ising model Solutions in one and more dimensions Symmetry and ergodicity breaking Conclusion Introduction phase A phase B Tc temperature T phase transition order parameter Critical exponents Tc T Formalism Statistical mechanical basics sample region Ω i) certain dimension d ii) volume V (Ω) iii) number of particles/sites N(Ω) iv) boundary conditions Hamiltonian defined on the sample region H − Ω = K Θ k T n n B n Depending on the degrees of freedom Coupling constants Partition function 1 −βHΩ({Kn},{Θn}) β = ZΩ[{Kn}] = T r exp kBT Free energy FΩ[{Kn}] = FΩ[K] = −kBT logZΩ[{Kn}] Free energy per site FΩ[K] fb[K] = lim N(Ω)→∞ N(Ω) i) Non-trivial existence of limit ii) Independent of Ω iii) N(Ω) lim = const N(Ω)→∞ V (Ω) Phases and phase boundaries Supp.: -fb[K] exists - there exist D coulping constants: {K1,...,KD} -fb[K] is analytic almost everywhere - non-analyticities of f b [ { K n } ] are points, lines, planes, hyperplanes in the phase diagram Dimension of these singular loci: Ds = 0, 1, 2,... Codimension C for each type of singular loci: C = D − Ds Phase : region of analyticity of fb[K] Phase boundaries : loci of codimension C = 1 Types of phase transitions fb[K] is everywhere continuous. Two types of phase transitions: ∂fb[K] a) Discontinuity across the phase boundary of ∂Ki first-order phase transition b) All derivatives of the free energy per site are continuous -
PHIL 145(002) Spring 2008
Please note: This is only a provisional draft of the course outline. It is intended to give you a sense of what the course will be about. Readings and important course dates may change before the semester begins. PHIL 220 A01 - Fall 2018 Introduction to Philosophy of Science Instructor: Eric Hochstein CRN: 12520 Time: Tuesday/Wednesday/Friday 11:30 AM – 12:20 PM Place: Clearihue Building C112 Office Hours (in Clearihue B330): Wednesday, 3:00-5:00 pm; and by appointment Email: [email protected] Description: Science is considered to be our best and most effective way of learning about the world. But what exactly differentiates science from non-science, and what are its limits? In this course, we will explore fundamental philosophical questions regarding the nature of science, and how it relates to more traditional philosophical questions regarding metaphysics and epistemology. More specifically, we will explore topics like: what is the demarcation between science from non-science? Does science get closer to truth as it progresses? Can the theories of one science (e.g. psychology) be reduced to theories of another (e.g. neuroscience)? Structure: The course comprises three lectures (50min) per week, the contents of which will be based on the course readings. The course will proceed primarily through lectures and discussions. Readings for the class will all be uploaded onto the course website. Evaluation: The course will be graded as follows: • Attendance and Class Participation, worth 10% (you can miss 5 classes with no penalty. Each additional class missed will be -1% to your attendance/participation grade). -
Book of Abstracts
Book of Abstracts 3 Foreword The 23 rd International Conference on Atomic Physics takes place in Ecole Polytechnique, a high level graduate school close to Paris. Following the tradition of ICAP, the conference presents an outstanding programme of invited VSHDNHUVFRYHULQJWKHPRVWUHFHQWVXEMHFWVLQWKH¿HOGRIDWRPLFSK\VLFVVXFKDV Ultracold gases and Bose Einstein condensates, Ultracold Fermi gases, Fundamental atomic tests and measurements, Precision measurements, atomic clocks and interferometers, Quantum information and simulations with atoms and ions, Quantum optics and cavity QED with atoms, Atoms and molecules in optical lattices, From two-body to many-body systems, Ultrafast phenomena and free electron lasers, Beyond atomic physics (biophysics, optomechanics...). The program includes 31 invited talks and 13 ‘hot topic’ talks. This book of abstracts gathers the contributions of these talks and of all posters, organized in three sessions. The proceedings of the conference will be published online in open access by the “European 3K\VLFDO-RXUQDO:HERI&RQIHUHQFHV´KWWSZZZHSMFRQIHUHQFHVRUJ On behalf of the committees, we would like to welcome you in Palaiseau, and to wish you an excit- ing conference. 4 Committees Programme committee Alain Aspect France Michèle Leduc France Hans Bachor Australia Maciej Lewenstein Spain Vanderlei Bagnato Brazil Anne L’Huillier Sweden Victor Balykin Russia Luis Orozco USA Rainer Blatt Austria Jian-Wei Pan China Denise Caldwell USA Hélène Perrin France Gordon Drake Canada Monika Ritsch-Marte Austria Wolfgang Ertmer Germany Sandro Stringari Italy Peter Hannaford Australia Regina de Vivie-Riedle Germany Philippe Grangier France Vladan Vuletic USA Massimo Inguscio Italy Ian Walmsley UK Hidetoshi Katori Japan Jun Ye USA Local organizing committee Philippe Grangier (co-chair) Institut d’Optique - CNRS Michèle Leduc (co-chair) ENS - CNRS Hélène Perrin (co-chair) U. -
On the Unity and Continuity of Science: Structural Realism's Underdetermination Problem and Reductive Structuralism's Solution
Georgia State University ScholarWorks @ Georgia State University Philosophy Theses Department of Philosophy 8-12-2014 On the Unity and Continuity of Science: Structural Realism's Underdetermination Problem and Reductive Structuralism's Solution Anthony Blake Nespica Follow this and additional works at: https://scholarworks.gsu.edu/philosophy_theses Recommended Citation Nespica, Anthony Blake, "On the Unity and Continuity of Science: Structural Realism's Underdetermination Problem and Reductive Structuralism's Solution." Thesis, Georgia State University, 2014. https://scholarworks.gsu.edu/philosophy_theses/151 This Thesis is brought to you for free and open access by the Department of Philosophy at ScholarWorks @ Georgia State University. It has been accepted for inclusion in Philosophy Theses by an authorized administrator of ScholarWorks @ Georgia State University. For more information, please contact [email protected]. ON THE UNITY AND CONTINUITY OF SCIENCE: STRUCTURAL REALISM’S UNDERDETERMINATION PROBLEM AND REDUCTIVE STRUCTURALISM’S SOLUTION by ANTHONY BLAKE NESPICA Under the Direction of Daniel A. Weiskopf ABSTRACT Russell’s claim that only structural knowledge of the world is possible was influentially criticized by Newman as rendering scientific discoveries trivial. I show that a version of this crit- icism also applies to the “structural realism” more recently advocated by Worrall, which requires continuity of formal structure between predecessor and successor scientific theories. The prob- lem is that structure, in its common set-theoretical construal, is radically underdetermined by the entities and relations over which it is defined, rendering intertheoretic continuity intolerably cheap. I show that this problem may be overcome by supplementing the purely formal relation of intertheoretic isomorphism with the semiformal “Ontological Reductive Links” developed by Moulines and others of the German “structuralist” approach to the philosophy of science. -
Josiah Willard Gibbs
GENERAL ARTICLE Josiah Willard Gibbs V Kumaran The foundations of classical thermodynamics, as taught in V Kumaran is a professor textbooks today, were laid down in nearly complete form by of chemical engineering at the Indian Institute of Josiah Willard Gibbs more than a century ago. This article Science, Bangalore. His presentsaportraitofGibbs,aquietandmodestmanwhowas research interests include responsible for some of the most important advances in the statistical mechanics and history of science. fluid mechanics. Thermodynamics, the science of the interconversion of heat and work, originated from the necessity of designing efficient engines in the late 18th and early 19th centuries. Engines are machines that convert heat energy obtained by combustion of coal, wood or other types of fuel into useful work for running trains, ships, etc. The efficiency of an engine is determined by the amount of useful work obtained for a given amount of heat input. There are two laws related to the efficiency of an engine. The first law of thermodynamics states that heat and work are inter-convertible, and it is not possible to obtain more work than the amount of heat input into the machine. The formulation of this law can be traced back to the work of Leibniz, Dalton, Joule, Clausius, and a host of other scientists in the late 17th and early 18th century. The more subtle second law of thermodynamics states that it is not possible to convert all heat into work; all engines have to ‘waste’ some of the heat input by transferring it to a heat sink. The second law also established the minimum amount of heat that has to be wasted based on the absolute temperatures of the heat source and the heat sink. -
Aleksei A. Abrikosov 1928–2017
Aleksei A. Abrikosov 1928–2017 A Biographical Memoir by M. R. Norman ©2018 National Academy of Sciences. Any opinions expressed in this memoir are those of the author and do not necessarily reflect the views of the National Academy of Sciences. ALEKSEI ALEKSEEVICH ABRIKOSOV June 25, 1928–March 29, 2017 Elected to the NAS, 2000 Shortly after the 2003 announcement that Aleksei Abrikosov had won the Nobel Prize in Physics, a number of colleagues took Alex to lunch at a nearby Italian restau- rant. During lunch, one of the Russian visitors exclaimed that Alex should get a second Nobel Prize, this time in Literature for his famous “AGD” book with Lev Gor’kov and Igor Dzyaloshinskii (Methods of Quantum Field Theory in Statistical Physics.) Somewhat taken aback, I looked closely at this individual and realized that he was deadly serious. Although I could imagine the reaction of the Nobel Literature committee to such a book (for a lay person, perhaps analogous to trying to read Finnegan’s Wake), I had to admit that my own copy of this book is quite dog-eared, having been put to good use over the By M. R. Norman years. In fact, you know you have made it in physics when your book gets a Dover edition. One of the most charming pictures I ever saw was a rare drawing in color that Alexei Tsvelik did (commissioned by Andrei Varlamov for Alex’s 50th birthday) that was proudly displayed in Alex’s home in Lemont, IL. It showed Alex with his fingers raised in a curled fashion as in the habit of medieval Popes. -
Who's Afraid of Nagelian Reduction?
Who's Afraid of Nagelian Reduction? Foad Dizadji-Bahmani Roman Frigg Stephan Hartmann∗ Abstract We reconsider the Nagelian theory of reduction and argue that, contrary to a widely held view, it is the right analysis of intertheoretic reduction, since the alleged difficulties of the theory either vanish upon closer inspection or turn out to be substantive philosophical questions rather than knock-down arguments. 1 Introduction The purpose of this paper is to examine synchronic intertheoretic reduction, i.e. the reductive relation between pairs of theories which have the same (or largely overlapping) domains of application and which are simultaneously valid to various extents.1 Examples of putative synchronic intertheoretic re- duction are the reduction of chemistry to atomic physics, rigid body mechan- ics to particle mechanics, and thermodynamics (TD) to statistical mechanics (SM). The central contention of this paper is that a Nagelian account of reduction is essentially on the right track: With some modifications and qualifications ∗Authors are listed alphabetically; the paper is fully collaborative. To contact the authors write to [email protected], [email protected], or [email protected]. 1There are, of course, other types of reductive relations, most notably diachronic theory reductions, an example of which is Newtonian and relativistic mechanics. See Nickles (1975). For an in-depth discussion of such cases, see Batterman (2002). 1 that account tells the right story about how synchronic intertheoretic reduc- tion works. For reasons that will become clear as we proceed, we refer to this modified and qualified account as the Generalised Nagel-Schaffner Model of Reduction (GNS). -
CURRICULUM VITAE SANDRO STRINGARI Born in Italy on March
CURRICULUM VITAE SANDRO STRINGARI Born in Italy on March 2nd, 1949 Married with two daughters. Italian citizenship EDUCATION, MAIN APPOINTMENTS AND AWARDS 1972 Laurea in Physics cum laude at the Università di Pisa and Scuola Normale Superiore 1972/1973 Fellowship at the Scuola Normale Superiore 1973-1976 Research assistant at the Università di Trento 1976 Visiting scientist at the Department of Theoretical Physics, Oxford (6 months) 1976-1980 Assistant professor at the Università di Trento 1978/1979 CNRS visitor at the Institute de Physique Nucleaire, Orsay 1980-1990 Associate professor at the Università di Trento 1985/1986 CNRS visitor at the Institute de Physique Nucleaire, Orsay 1990 Visiting scientist at the Laue-Langevin Institute, Grenoble (1 month) 1990 Full professor at the Università di Trento 2002 M.T. Messori Roncaglia and E. Mari prize of the Accademia dei Lincei 2002 Visiting professor at the Ecole Normale Superieure, Paris (1 month) 2004/2005 European Chair at the College de France, Paris 2007 Visiting professor at the Institut Henri Poincaré, Paris (1 month) 2008 Visiting professor at the Center for Ultracold Atoms, MIT-Harvard (2 months) ORGANIZATION ACTIVITIES (selection) 1992-1995 Chairman of the Physics Department, Università di Trento 1996/1997 Vice-Rector of the Università di Trento 1996-2000 National coordinator of the INFM Project "Experimental and Theoretical Investigation of Bose-Einstein Condensation in Alkali Atoms” 2002 Director of the INFM Research and Development BEC Center 2006 Member of the Evaluation Committee -
Viscosity from Newton to Modern Non-Equilibrium Statistical Mechanics
Viscosity from Newton to Modern Non-equilibrium Statistical Mechanics S´ebastien Viscardy Belgian Institute for Space Aeronomy, 3, Avenue Circulaire, B-1180 Brussels, Belgium Abstract In the second half of the 19th century, the kinetic theory of gases has probably raised one of the most impassioned de- bates in the history of science. The so-called reversibility paradox around which intense polemics occurred reveals the apparent incompatibility between the microscopic and macroscopic levels. While classical mechanics describes the motionof bodies such as atoms and moleculesby means of time reversible equations, thermodynamics emphasizes the irreversible character of macroscopic phenomena such as viscosity. Aiming at reconciling both levels of description, Boltzmann proposed a probabilistic explanation. Nevertheless, such an interpretation has not totally convinced gen- erations of physicists, so that this question has constantly animated the scientific community since his seminal work. In this context, an important breakthrough in dynamical systems theory has shown that the hypothesis of microscopic chaos played a key role and provided a dynamical interpretation of the emergence of irreversibility. Using viscosity as a leading concept, we sketch the historical development of the concepts related to this fundamental issue up to recent advances. Following the analysis of the Liouville equation introducing the concept of Pollicott-Ruelle resonances, two successful approaches — the escape-rate formalism and the hydrodynamic-mode method — establish remarkable relationships between transport processes and chaotic properties of the underlying Hamiltonian dynamics. Keywords: statistical mechanics, viscosity, reversibility paradox, chaos, dynamical systems theory Contents 1 Introduction 2 2 Irreversibility 3 2.1 Mechanics. Energyconservationand reversibility . ........................ 3 2.2 Thermodynamics. -
Hamiltonian Mechanics Wednesday, ß November Óþõõ
Hamiltonian Mechanics Wednesday, ß November óþÕÕ Lagrange developed an alternative formulation of Newtonian me- Physics ÕÕÕ chanics, and Hamilton developed yet another. Of the three methods, Hamilton’s proved the most readily extensible to the elds of statistical mechanics and quantum mechanics. We have already been introduced to the Hamiltonian, N ∂L = Q ˙ − = Q( ˙ ) − (Õ) H q j ˙ L q j p j L j=Õ ∂q j j where the generalized momenta are dened by ∂L p j ≡ (ó) ∂q˙j and we have shown that dH = −∂L dt ∂t Õ. Legendre Transformation We will now show that the Hamiltonian is a so-called “natural function” of the general- ized coordinates and generalized momenta, using a trick that is just about as sophisticated as the product rule of dierentiation. You may have seen Legendre transformations in ther- modynamics, where they are used to switch independent variables from the ones you have to the ones you want. For example, the internal energy U satises ∂U ∂U dU = T dS − p dV = dS + dV (ì) ∂S V ∂V S e expression between the equal signs has the physics. It says that you can change the internal energy by changing the entropy S (scaled by the temperature T) or by changing the volume V (scaled by the negative of the pressure p). e nal expression is simply a mathematical statement that the function U(S, V) has a total dierential. By lining up the various quantities, we deduce that = ∂U and = − ∂U . T ∂S V p ∂V S In performing an experiment at constant temperature, however, the T dS term is awk- ward. -
Arxiv:1610.06882V2 [Astro-Ph.HE] 1 Mar 2017
International Journal of Modern Physics D c World Scientific Publishing Company NEUTRON STARS IN THE LABORATORY VANESSA GRABER1;2 [email protected] NILS ANDERSSON1 [email protected] MICHAEL HOGG1 1Mathematical Sciences and STAG Research Centre, University of Southampton Southampton SO17 1BJ, United Kingdom 2Department of Physics and McGill Space Institute, McGill University, 3550 rue University, Montreal, QC, H3A 2T8, Canada Received Day Month Year Revised Day Month Year Neutron stars are astrophysical laboratories of many extremes of physics. Their rich phe- nomenology provides insights into the state and composition of matter at densities which cannot be reached in terrestrial experiments. Since the core of a mature neutron star is expected to be dominated by superfluid and superconducting components, observations also probe the dynamics of large-scale quantum condensates. The testing and under- standing of the relevant theory tends to focus on the interface between the astrophysics phenomenology and nuclear physics. The connections with low-temperature experiments tend to be ignored. However, there has been dramatic progress in understanding labo- ratory condensates (from the different phases of superfluid helium to the entire range of superconductors and cold atom condensates). In this review, we provide an overview of these developments, compare and contrast the mathematical descriptions of laboratory condensates and neutron stars and summarise the current experimental state-of-the-art. arXiv:1610.06882v2 [astro-ph.HE] 1 Mar 2017 This discussion suggests novel ways that we may make progress in understanding neutron star physics using low-temperature laboratory experiments. Keywords: PACS numbers: Contents 1. Neutron Stars and Fundamental Physics . -
Ergodic Theory in the Perspective of Functional Analysis
Ergodic Theory in the Perspective of Functional Analysis 13 Lectures by Roland Derndinger, Rainer Nagel, GÄunther Palm (uncompleted version) In July 1984 this manuscript has been accepted for publication in the series \Lecture Notes in Mathematics" by Springer-Verlag. Due to a combination of unfortunate circumstances none of the authors was able to perform the necessary ¯nal revision of the manuscript. TÄubingen,July 1987 1 2 I. What is Ergodic Theory? The notion \ergodic" is an arti¯cial creation, and the newcomer to \ergodic theory" will have no intuitive understanding of its content: \elementary ergodic theory" neither is part of high school- or college- mathematics (as does \algebra") nor does its name explain its subject (as does \number theory"). Therefore it might be useful ¯rst to explain the name and the subject of \ergodic theory". Let us begin with the quotation of the ¯rst sentence of P. Walters' introductory lectures (1975, p. 1): \Generally speaking, ergodic theory is the study of transformations and flows from the point of view of recurrence properties, mixing properties, and other global, dynamical, properties connected with asymptotic behavior." Certainly, this de¯nition is very systematic and complete (compare the beginning of our Lectures III. and IV.). Still we will try to add a few more answers to the question: \What is Ergodic Theory ?" Naive answer: A container is divided into two parts with one part empty and the other ¯lled with gas. Ergodic theory predicts what happens in the long run after we remove the dividing wall. First etymological answer: ergodhc=di±cult. Historical answer: 1880 - Boltzmann, Maxwell - ergodic hypothesis 1900 - Poincar¶e - recurrence theorem 1931 - von Neumann - mean ergodic theorem 1931 - Birkho® - individual ergodic theorem 1958 - Kolmogorov - entropy as an invariant 1963 - Sinai - billiard flow is ergodic 1970 - Ornstein - entropy classi¯es Bernoulli shifts 1975 - Akcoglu - individual Lp-ergodic theorem Naive answer of a physicist: Ergodic theory proves that time mean equals space mean.