Studi Metodologiczne 39.Pdf
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Part 5: the Bose-Einstein Distribution
PHYS393 – Statistical Physics Part 5: The Bose-Einstein Distribution Distinguishable and indistinguishable particles In the previous parts of this course, we derived the Boltzmann distribution, which described how the number of distinguishable particles in different energy states varied with the energy of those states, at different temperatures: N εj nj = e− kT . (1) Z However, in systems consisting of collections of identical fermions or identical bosons, the wave function of the system has to be either antisymmetric (for fermions) or symmetric (for bosons) under interchange of any two particles. With the allowed wave functions, it is no longer possible to identify a particular particle with a particular energy state. Instead, all the particles are “shared” between the occupied states. The particles are said to be indistinguishable . Statistical Physics 1 Part 5: The Bose-Einstein Distribution Indistinguishable fermions In the case of indistinguishable fermions, the wave function for the overall system must be antisymmetric under the interchange of any two particles. One consequence of this is the Pauli exclusion principle: any given state can be occupied by at most one particle (though we can’t say which particle!) For example, for a system of two fermions, a possible wave function might be: 1 ψ(x1, x 2) = [ψ (x1)ψ (x2) ψ (x2)ψ (x1)] . (2) √2 A B − A B Here, x1 and x2 are the coordinates of the two particles, and A and B are the two occupied states. If we try to put the two particles into the same state, then the wave function vanishes. Statistical Physics 2 Part 5: The Bose-Einstein Distribution Indistinguishable fermions Finding the distribution with the maximum number of microstates for a system of identical fermions leads to the Fermi-Dirac distribution: g n = i . -
Game Theory- Prisoners Dilemma Vs Battle of the Sexes EXCERPTS
Lesson 14. Game Theory 1 Lesson 14 Game Theory c 2010, 2011 ⃝ Roberto Serrano and Allan M. Feldman All rights reserved Version C 1. Introduction In the last lesson we discussed duopoly markets in which two firms compete to sell a product. In such markets, the firms behave strategically; each firm must think about what the other firm is doing in order to decide what it should do itself. The theory of duopoly was originally developed in the 19th century, but it led to the theory of games in the 20th century. The first major book in game theory, published in 1944, was Theory of Games and Economic Behavior,byJohnvon Neumann (1903-1957) and Oskar Morgenstern (1902-1977). We will return to the contributions of Von Neumann and Morgenstern in Lesson 19, on uncertainty and expected utility. Agroupofpeople(orteams,firms,armies,countries)areinagame if their decision problems are interdependent, in the sense that the actions that all of them take influence the outcomes for everyone. Game theory is the study of games; it can also be called interactive decision theory. Many real-life interactions can be viewed as games. Obviously football, soccer, and baseball games are games.Butsoaretheinteractionsofduopolists,thepoliticalcampaignsbetweenparties before an election, and the interactions of armed forces and countries. Even some interactions between animal or plant species in nature can be modeled as games. In fact, game theory has been used in many different fields in recent decades, including economics, political science, psychology, sociology, computer science, and biology. This brief lesson is not meant to replace a formal course in game theory; it is only an in- troduction. -
The Debye Model of Lattice Heat Capacity
The Debye Model of Lattice Heat Capacity The Debye model of lattice heat capacity is more involved than the relatively simple Einstein model, but it does keep the same basic idea: the internal energy depends on the energy per phonon (ε=ℏΩ) times the ℏΩ/kT average number of phonons (Planck distribution: navg=1/[e -1]) times the number of modes. It is in the number of modes that the difference between the two models occurs. In the Einstein model, we simply assumed that each mode was the same (same frequency, Ω), and that the number of modes was equal to the number of atoms in the lattice. In the Debye model, we assume that each mode has its own K (that is, has its own λ). Since Ω is related to K (by the dispersion relation), each mode has a different Ω. 1. Number of modes In the Debye model we assume that the normal modes consist of STANDING WAVES. If we have travelling waves, they will carry energy through the material; if they contain the heat energy (that will not move) they need to be standing waves. Standing waves are waves that do travel but go back and forth and interfere with each other to create standing waves. Recall that Newton's Second Law gave us atoms that oscillate: [here x = sa where s is an integer and a the lattice spacing] iΩt iKsa us = uo e e ; and if we use the form sin(Ksa) for eiKsa [both indicate oscillations]: iΩt us = uo e sin(Ksa) . We now apply the boundary conditions on our solution: to have standing waves both ends of the wave must be tied down, that is, we must have u0 = 0 and uN = 0. -
Prisoners of Reason Game Theory and Neoliberal Political Economy
C:/ITOOLS/WMS/CUP-NEW/6549131/WORKINGFOLDER/AMADAE/9781107064034PRE.3D iii [1–28] 11.8.2015 9:57PM Prisoners of Reason Game Theory and Neoliberal Political Economy S. M. AMADAE Massachusetts Institute of Technology C:/ITOOLS/WMS/CUP-NEW/6549131/WORKINGFOLDER/AMADAE/9781107064034PRE.3D iv [1–28] 11.8.2015 9:57PM 32 Avenue of the Americas, New York, ny 10013-2473, usa Cambridge University Press is part of the University of Cambridge. It furthers the University’s mission by disseminating knowledge in the pursuit of education, learning, and research at the highest international levels of excellence. www.cambridge.org Information on this title: www.cambridge.org/9781107671195 © S. M. Amadae 2015 This publication is in copyright. Subject to statutory exception and to the provisions of relevant collective licensing agreements, no reproduction of any part may take place without the written permission of Cambridge University Press. First published 2015 Printed in the United States of America A catalog record for this publication is available from the British Library. Library of Congress Cataloging in Publication Data Amadae, S. M., author. Prisoners of reason : game theory and neoliberal political economy / S.M. Amadae. pages cm Includes bibliographical references and index. isbn 978-1-107-06403-4 (hbk. : alk. paper) – isbn 978-1-107-67119-5 (pbk. : alk. paper) 1. Game theory – Political aspects. 2. International relations. 3. Neoliberalism. 4. Social choice – Political aspects. 5. Political science – Philosophy. I. Title. hb144.a43 2015 320.01′5193 – dc23 2015020954 isbn 978-1-107-06403-4 Hardback isbn 978-1-107-67119-5 Paperback Cambridge University Press has no responsibility for the persistence or accuracy of URLs for external or third-party Internet Web sites referred to in this publication and does not guarantee that any content on such Web sites is, or will remain, accurate or appropriate. -
Repeated Games
REPEATED GAMES 1 Early PD experiments In 1950, Merrill Flood and Melvin Dresher (at RAND) devised an experiment to test Nash’s theory about defection in a two-person prisoners’ dilemma. Experimental Design – They asked two friends to play the PD 100 times. – They measured the success of Nash’s equilibrium concept by counting the number of times the players chose {D;D}. 2 Flood and Dresher’s results Player 1 cooperated in 68 rounds Player 2 cooperated in 78 rounds Both cooperated in 60 of last 89 rounds Flood Dresher Nash 3 Flood and Dresher’s results Player 1 cooperated in 68 rounds Player 2 cooperated in 78 rounds Both cooperated in 60 of last 89 rounds Wait a Ha! That jerk I can’tI’mOh a be Ha! Nash second... Nash was genius...%&@#!wrong! was wrong! wrong! Flood Dresher Nash 4 Nash’s response “If this experiment were conducted with various different players rotating the competition and with no information given to a player of what choices the others have been making until the end of all trials, then the experimental results would have been quite different, for this modification of procedure would remove the interaction between the trials.” 5 Nash’s response “The flaw in this experiment as a test of equilibrium point theory is that the experiment really amounts to having the players play one large multimove game. One cannot...think of the thing as a sequence of independent games...there is too much interaction.” In other words, Nash said that repeating the game changes the game itself. -
Phys 446: Solid State Physics / Optical Properties Lattice Vibrations
Solid State Physics Lecture 5 Last week: Phys 446: (Ch. 3) • Phonons Solid State Physics / Optical Properties • Today: Einstein and Debye models for thermal capacity Lattice vibrations: Thermal conductivity Thermal, acoustic, and optical properties HW2 discussion Fall 2007 Lecture 5 Andrei Sirenko, NJIT 1 2 Material to be included in the test •Factors affecting the diffraction amplitude: Oct. 12th 2007 Atomic scattering factor (form factor): f = n(r)ei∆k⋅rl d 3r reflects distribution of electronic cloud. a ∫ r • Crystalline structures. 0 sin()∆k ⋅r In case of spherical distribution f = 4πr 2n(r) dr 7 crystal systems and 14 Bravais lattices a ∫ n 0 ∆k ⋅r • Crystallographic directions dhkl = 2 2 2 1 2 ⎛ h k l ⎞ 2πi(hu j +kv j +lw j ) and Miller indices ⎜ + + ⎟ •Structure factor F = f e ⎜ a2 b2 c2 ⎟ ∑ aj ⎝ ⎠ j • Definition of reciprocal lattice vectors: •Elastic stiffness and compliance. Strain and stress: definitions and relation between them in a linear regime (Hooke's law): σ ij = ∑Cijklε kl ε ij = ∑ Sijklσ kl • What is Brillouin zone kl kl 2 2 C •Elastic wave equation: ∂ u C ∂ u eff • Bragg formula: 2d·sinθ = mλ ; ∆k = G = eff x sound velocity v = ∂t 2 ρ ∂x2 ρ 3 4 • Lattice vibrations: acoustic and optical branches Summary of the Last Lecture In three-dimensional lattice with s atoms per unit cell there are Elastic properties – crystal is considered as continuous anisotropic 3s phonon branches: 3 acoustic, 3s - 3 optical medium • Phonon - the quantum of lattice vibration. Elastic stiffness and compliance tensors relate the strain and the Energy ħω; momentum ħq stress in a linear region (small displacements, harmonic potential) • Concept of the phonon density of states Hooke's law: σ ij = ∑Cijklε kl ε ij = ∑ Sijklσ kl • Einstein and Debye models for lattice heat capacity. -
A Beautiful Math : John Nash, Game Theory, and the Modern Quest for a Code of Nature / Tom Siegfried
A BEAUTIFULA BEAUTIFUL MATH MATH JOHN NASH, GAME THEORY, AND THE MODERN QUEST FOR A CODE OF NATURE TOM SIEGFRIED JOSEPH HENRY PRESS Washington, D.C. Joseph Henry Press • 500 Fifth Street, NW • Washington, DC 20001 The Joseph Henry Press, an imprint of the National Academies Press, was created with the goal of making books on science, technology, and health more widely available to professionals and the public. Joseph Henry was one of the founders of the National Academy of Sciences and a leader in early Ameri- can science. Any opinions, findings, conclusions, or recommendations expressed in this volume are those of the author and do not necessarily reflect the views of the National Academy of Sciences or its affiliated institutions. Library of Congress Cataloging-in-Publication Data Siegfried, Tom, 1950- A beautiful math : John Nash, game theory, and the modern quest for a code of nature / Tom Siegfried. — 1st ed. p. cm. Includes bibliographical references and index. ISBN 0-309-10192-1 (hardback) — ISBN 0-309-65928-0 (pdfs) 1. Game theory. I. Title. QA269.S574 2006 519.3—dc22 2006012394 Copyright 2006 by Tom Siegfried. All rights reserved. Printed in the United States of America. Preface Shortly after 9/11, a Russian scientist named Dmitri Gusev pro- posed an explanation for the origin of the name Al Qaeda. He suggested that the terrorist organization took its name from Isaac Asimov’s famous 1950s science fiction novels known as the Foun- dation Trilogy. After all, he reasoned, the Arabic word “qaeda” means something like “base” or “foundation.” And the first novel in Asimov’s trilogy, Foundation, apparently was titled “al-Qaida” in an Arabic translation. -
RM Calendar 2017
Rudi Mathematici x3 – 6’135x2 + 12’545’291 x – 8’550’637’845 = 0 www.rudimathematici.com 1 S (1803) Guglielmo Libri Carucci dalla Sommaja RM132 (1878) Agner Krarup Erlang Rudi Mathematici (1894) Satyendranath Bose RM168 (1912) Boris Gnedenko 1 2 M (1822) Rudolf Julius Emmanuel Clausius (1905) Lev Genrichovich Shnirelman (1938) Anatoly Samoilenko 3 T (1917) Yuri Alexeievich Mitropolsky January 4 W (1643) Isaac Newton RM071 5 T (1723) Nicole-Reine Etable de Labrière Lepaute (1838) Marie Ennemond Camille Jordan Putnam 2002, A1 (1871) Federigo Enriques RM084 Let k be a fixed positive integer. The n-th derivative of (1871) Gino Fano k k n+1 1/( x −1) has the form P n(x)/(x −1) where P n(x) is a 6 F (1807) Jozeph Mitza Petzval polynomial. Find P n(1). (1841) Rudolf Sturm 7 S (1871) Felix Edouard Justin Emile Borel A college football coach walked into the locker room (1907) Raymond Edward Alan Christopher Paley before a big game, looked at his star quarterback, and 8 S (1888) Richard Courant RM156 said, “You’re academically ineligible because you failed (1924) Paul Moritz Cohn your math mid-term. But we really need you today. I (1942) Stephen William Hawking talked to your math professor, and he said that if you 2 9 M (1864) Vladimir Adreievich Steklov can answer just one question correctly, then you can (1915) Mollie Orshansky play today. So, pay attention. I really need you to 10 T (1875) Issai Schur concentrate on the question I’m about to ask you.” (1905) Ruth Moufang “Okay, coach,” the player agreed. -
(November 12-13)- Page 545
College Park Program (October 30-31) - Page 531 Baton Rouge Program (November 12-13)- Page 545 Notices of the American Mathematical Society < 2.. c: 3 ('1) ~ z c: 3 C" ..,('1) 0'1 October 1982, Issue 220 Volume 29, Number 6, Pages 497-616 Providence, Rhode Island USA ISSN 0002-9920 Calendar of AMS Meetings THIS CALENDAR lists all meetings which have been approved by the Council prior to the date this issue of the Notices 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 submitred 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. -
Game Theory and Its Practical Applications
University of Northern Iowa UNI ScholarWorks Presidential Scholars Theses (1990 – 2006) Honors Program 1997 Game theory and its practical applications Angela M. Koos University of Northern Iowa Let us know how access to this document benefits ouy Copyright ©1997 Angela M. Koos Follow this and additional works at: https://scholarworks.uni.edu/pst Part of the Other Economics Commons Recommended Citation Koos, Angela M., "Game theory and its practical applications" (1997). Presidential Scholars Theses (1990 – 2006). 100. https://scholarworks.uni.edu/pst/100 This Open Access Presidential Scholars Thesis is brought to you for free and open access by the Honors Program at UNI ScholarWorks. It has been accepted for inclusion in Presidential Scholars Theses (1990 – 2006) by an authorized administrator of UNI ScholarWorks. For more information, please contact [email protected]. Game Theory and its Practical Applications A Presidential Scholar Senior Thesis University of Northern Iowa by Angela M. Koos Spring 1997 Dr. Ken Brown, 7 Dfrte Thesis and Major Advisor ,~-,, Dr. Ed Rathmell, Date Chair of Presidential Scholars Board Table of Contents Section Page(s) I. Historical Overview 1 I.A. Early Contributions to Game Theory 1 - 3 LB. John von Neumann, the RAND Corporation, and the Arms Race 3 - 7 LC. John Nash 7 - 8 I.D. Other Contributions to Game Theory 9 II. Defining Game Theory 9 - 12 II.A. Formal Representations of Games 12 - 13 II.A. I. Extensive Form 13 - 24 II.A.2. Normal Form 24 - 25 III. The Minimax Theorem 25 - 26 III.A. Preliminary Comments 26 - 27 III.B. The Theorem 27 - 28 IV. -
Statistical Physics of Social Dynamics
Statistical physics of social dynamics Claudio Castellano∗ SMC, INFM-CNR and Dipartimento di Fisica, “Sapienza” Universit`adi Roma, Piazzale A. Moro 2, 00185 Roma I-ITALY Santo Fortunato† Complex Networks Lagrange Laboratory, ISI Foundation, Viale S. Severo 65, 10133, Torino, I-ITALY Vittorio Loreto‡ Dipartimento di Fisica, “Sapienza” Universit`adi Roma and SMC, INFM-CNR, Piazzale A. Moro 2, 00185 Roma I-ITALY and Complex Networks Lagrange Laboratory, ISI Foundation, Viale S. Severo 65, 10133, Torino, I-ITALY Statistical physics has proven to be a very fruitful framework to describe phenomena outside the realm of traditional physics. The last years have witnessed the attempt by physicists to study collective phenomena emerging from the interactions of individuals as elementary units in social structures. Here we review the state of the art by focusing on a wide list of topics ranging from opinion, cultural and language dynamics to crowd behavior, hierarchy formation, human dynamics, social spreading. We highlight the connections between these problems and other, more traditional, topics of statistical physics. We also emphasize the comparison of model results with empirical data from social systems. Contents 1. The Naming Game 30 2. Symmetry breaking: a controlled case 31 I. INTRODUCTION 2 3. The role of the interaction topology 32 C. Other models 33 II. GENERAL FRAMEWORK: CONCEPTS AND TOOLS 3 D. Language competition 33 A. Order and disorder: the Ising paradigm 4 1. Macroscopic models 34 B. Role of topology 5 2. Microscopic models 35 C. Dynamical systems approach 7 D. Agent-based modeling 7 VI. CROWD BEHAVIOR 35 A. Flocking 36 III. -
Hodge Theory on Metric Spaces
Hodge Theory on Metric Spaces Laurent Bartholdi∗ Georg-August-Universit¨atG¨ottingen Deutschland Thomas Schick∗ Nat Smale Georg-August-Universit¨atG¨ottingen University of Utah Deutschland Steve Smaley City University of Hong Kong With an appendix by Anthony W. Baker z Mathematics and Computing Technology The Boeing Company. Last compiled December 1, 2009; last edited December 1, by LB Abstract Hodge theory is a beautiful synthesis of geometry, topology, and anal- ysis, which has been developed in the setting of Riemannian manifolds. On the other hand, spaces of images, which are important in the math- ematical foundations of vision and pattern recognition, do not fit this framework. This motivates us to develop a version of Hodge theory on metric spaces with a probability measure. We believe that this constitutes a step towards understanding the geometry of vision. The appendix by Anthony Baker provides a separable, compact metric space with infinite dimensional α-scale homology. 1 Introduction Hodge Theory [21] studies the relationships of topology, functional analysis and geometry of a manifold. It extends the theory of the Laplacian on domains of Euclidean space or on a manifold. ∗email: [email protected] and [email protected] www: http://www.uni-math.gwdg.de/schick Laurent Bartholdi and Thomas Schick were partially supported by the Courant Research Center \Higher order structures in Mathematics" of the German Initiative of Excellence ySteve Smale was supported in part by the NSF, and the Toyota Technological Institute, Chicago zemail: [email protected] 1 2 Laurent Bartholdi, Thomas Schick, Nat Smale, Steve Smale However, there are a number of spaces, not manifolds, which could ben- efit from an extension of Hodge theory, and that is the motivation here.