Selective Guide to Literature on Statistical Information for Engineers
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Arxiv:1910.10745V1 [Cond-Mat.Str-El] 23 Oct 2019 2.2 Symmetry-Protected Time Crystals
A Brief History of Time Crystals Vedika Khemania,b,∗, Roderich Moessnerc, S. L. Sondhid aDepartment of Physics, Harvard University, Cambridge, Massachusetts 02138, USA bDepartment of Physics, Stanford University, Stanford, California 94305, USA cMax-Planck-Institut f¨urPhysik komplexer Systeme, 01187 Dresden, Germany dDepartment of Physics, Princeton University, Princeton, New Jersey 08544, USA Abstract The idea of breaking time-translation symmetry has fascinated humanity at least since ancient proposals of the per- petuum mobile. Unlike the breaking of other symmetries, such as spatial translation in a crystal or spin rotation in a magnet, time translation symmetry breaking (TTSB) has been tantalisingly elusive. We review this history up to recent developments which have shown that discrete TTSB does takes place in periodically driven (Floquet) systems in the presence of many-body localization (MBL). Such Floquet time-crystals represent a new paradigm in quantum statistical mechanics — that of an intrinsically out-of-equilibrium many-body phase of matter with no equilibrium counterpart. We include a compendium of the necessary background on the statistical mechanics of phase structure in many- body systems, before specializing to a detailed discussion of the nature, and diagnostics, of TTSB. In particular, we provide precise definitions that formalize the notion of a time-crystal as a stable, macroscopic, conservative clock — explaining both the need for a many-body system in the infinite volume limit, and for a lack of net energy absorption or dissipation. Our discussion emphasizes that TTSB in a time-crystal is accompanied by the breaking of a spatial symmetry — so that time-crystals exhibit a novel form of spatiotemporal order. -
Introduction to Statistically Designed Experiments, NREL
Introduction to Statistically Designed Experiments Mike Heaney ([email protected]) ASQ Denver Section 1300 Monthly Membership Meeting September 13, 2016 Englewood, Colorado NREL/PR-5500-66898 Objectives Give some basic background information on statistically designed experiments Demonstrate the advantages of using statistically designed experiments1 1 Often referred to as design of experiments (DOE or DOX), or experimental design. 2 A Few Thoughts Many companies/organizations do experiments for Process improvement Product development Marketing strategies We need to plan our experiments as efficiently and effectively as possible Statistically designed experiments have a proven track record (Mullin 2013 in Chemical & Engineering News) Conclusions supported by statistical tests Substantial reduction in total experiments Why are we still planning experiments like it’s the 19th century? 3 Outline • Research Problems • The Linear Model • Key Types of Designs o Full Factorial o Fractional Factorial o Response Surface • Sequential Approach • Summary 4 Research Problems Research Problems Is a dependent variable (Y) affected by multiple independent variables (Xs)? Objective: Increase bearing lifetime (Hellstrand 1989) Y Bearing lifetime (hours) X1 Inner ring heat treatment Outer ring osculation (ratio Outer Ring X2 between ball diameter and outer ring raceway radius) Ball X3 Cage design Cage Inner Ring 6 Research Problems Objective: Hydrogen cyanide (HCN) removal in diesel exhaust gas (Zhao et al. 2006) Y HCN conversion X1 Propene -
Lecture 6: Entropy
Matthew Schwartz Statistical Mechanics, Spring 2019 Lecture 6: Entropy 1 Introduction In this lecture, we discuss many ways to think about entropy. The most important and most famous property of entropy is that it never decreases Stot > 0 (1) Here, Stot means the change in entropy of a system plus the change in entropy of the surroundings. This is the second law of thermodynamics that we met in the previous lecture. There's a great quote from Sir Arthur Eddington from 1927 summarizing the importance of the second law: If someone points out to you that your pet theory of the universe is in disagreement with Maxwell's equationsthen so much the worse for Maxwell's equations. If it is found to be contradicted by observationwell these experimentalists do bungle things sometimes. But if your theory is found to be against the second law of ther- modynamics I can give you no hope; there is nothing for it but to collapse in deepest humiliation. Another possibly relevant quote, from the introduction to the statistical mechanics book by David Goodstein: Ludwig Boltzmann who spent much of his life studying statistical mechanics, died in 1906, by his own hand. Paul Ehrenfest, carrying on the work, died similarly in 1933. Now it is our turn to study statistical mechanics. There are many ways to dene entropy. All of them are equivalent, although it can be hard to see. In this lecture we will compare and contrast dierent denitions, building up intuition for how to think about entropy in dierent contexts. The original denition of entropy, due to Clausius, was thermodynamic. -
Appendix A: Mathematical Formulas
Appendix A: Mathematical Formulas Logarithms Inab = \na -\-\nb', \na/b = \na— \nb; \na^=b\na Geometric Series If Irl < 1, we find that oo oo E ar^ = ; y^akr^ = r; ^=0 A:=o y^ n Z-^ 1 -r ^^ 1 -r ^=1 k=0 Limits UHospitaVs rule. Suppose that \\vOix->XQ fix) = lim;c-^A:o sM = 0* or that liirix-^xo Z^-^) = l™x^jco SM — =t^^- Then, under some conditions, we can write that y fix) ^. fix) um = hm . x-^XQ g{x) x^xo g^{x) If the functions f\x) and g\x) satisfy the same conditions as f(x) and g(x), we can repeat the process. Moreover, the constant XQ may be equal to ±oo. Derivatives Derivative of a quotient: d fix) gix)fix) - fix)g\x) = 7^ 11 gix) ^0. dx gix) g^ix) 340 Appendix A: Mathematical Formulas Remark. This formula can also be obtained by differentiating the product f(x)h(x), where/Z(A:) := l/g(x). Chain rule. If w = ^(jc), then we have: d d du , , ^fiu) = —f(u) . — = f\u)g\x) = AgixWix). dx du dx For example, if w = jc^, we calculate — exp(M^) = exp(w^)2w • 2x = 4x^ expU"*). dx Integrals Integration by parts: j udv = uv — I vdu. Integration by substitution. If the inverse function g~^ exists, then we can write that rh rd j f(x)dx = j f[g(y)]g{y)dy, where a = g(c) ^ c = g ^(a) and b = g(d) <^ d = g ^(b). For example, / e''^'dx-^=^' f 2yeydy=2yey\l-2 f e^ dy = 2e^-\-2. -
Dirty Tricks for Statistical Mechanics
Dirty tricks for statistical mechanics Martin Grant Physics Department, McGill University c MG, August 2004, version 0.91 ° ii Preface These are lecture notes for PHYS 559, Advanced Statistical Mechanics, which I’ve taught at McGill for many years. I’m intending to tidy this up into a book, or rather the first half of a book. This half is on equilibrium, the second half would be on dynamics. These were handwritten notes which were heroically typed by Ryan Porter over the summer of 2004, and may someday be properly proof-read by me. Even better, maybe someday I will revise the reasoning in some of the sections. Some of it can be argued better, but it was too much trouble to rewrite the handwritten notes. I am also trying to come up with a good book title, amongst other things. The two titles I am thinking of are “Dirty tricks for statistical mechanics”, and “Valhalla, we are coming!”. Clearly, more thinking is necessary, and suggestions are welcome. While these lecture notes have gotten longer and longer until they are al- most self-sufficient, it is always nice to have real books to look over. My favorite modern text is “Lectures on Phase Transitions and the Renormalisation Group”, by Nigel Goldenfeld (Addison-Wesley, Reading Mass., 1992). This is referred to several times in the notes. Other nice texts are “Statistical Physics”, by L. D. Landau and E. M. Lifshitz (Addison-Wesley, Reading Mass., 1970) par- ticularly Chaps. 1, 12, and 14; “Statistical Mechanics”, by S.-K. Ma (World Science, Phila., 1986) particularly Chaps. -
STATISTICAL SCIENCE Volume 31, Number 4 November 2016
STATISTICAL SCIENCE Volume 31, Number 4 November 2016 ApproximateModelsandRobustDecisions..................James Watson and Chris Holmes 465 ModelUncertaintyFirst,NotAfterwards....................Ingrid Glad and Nils Lid Hjort 490 ContextualityofMisspecificationandData-DependentLosses..............Peter Grünwald 495 SelectionofKLNeighbourhoodinRobustBayesianInference..........Natalia A. Bochkina 499 IssuesinRobustnessAnalysis.............................................Michael Goldstein 503 Nonparametric Bayesian Clay for Robust Decision Bricks ..................................................Christian P. Robert and Judith Rousseau 506 Ambiguity Aversion and Model Misspecification: An Economic Perspective ................................................Lars Peter Hansen and Massimo Marinacci 511 Rejoinder: Approximate Models and Robust Decisions. .James Watson and Chris Holmes 516 Filtering and Tracking Survival Propensity (Reconsidering the Foundations of Reliability) .......................................................................Nozer D. Singpurwalla 521 On Software and System Reliability Growth and Testing. ..............FrankP.A.Coolen 541 HowAboutWearingTwoHats,FirstPopper’sandthendeFinetti’s?..............Elja Arjas 545 WhatDoes“Propensity”Add?...................................................Jane Hutton 549 Reconciling the Subjective and Objective Aspects of Probability ...............Glenn Shafer 552 Rejoinder:ConcertUnlikely,“Jugalbandi”Perhaps..................Nozer D. Singpurwalla 555 ChaosCommunication:ACaseofStatisticalEngineering...............Anthony -
Generalized Molecular Chaos Hypothesis and the H-Theorem: Problem of Constraints and Amendment of Nonextensive Statistical Mechanics
Generalized molecular chaos hypothesis and the H-theorem: Problem of constraints and amendment of nonextensive statistical mechanics Sumiyoshi Abe1,2,3 1Department of Physical Engineering, Mie University, Mie 514-8507, Japan*) 2Institut Supérieur des Matériaux et Mécaniques Avancés, 44 F. A. Bartholdi, 72000 Le Mans, France 3Inspire Institute Inc., McLean, Virginia 22101, USA Abstract Quite unexpectedly, kinetic theory is found to specify the correct definition of average value to be employed in nonextensive statistical mechanics. It is shown that the normal average is consistent with the generalized Stosszahlansatz (i.e., molecular chaos hypothesis) and the associated H-theorem, whereas the q-average widely used in the relevant literature is not. In the course of the analysis, the distributions with finite cut-off factors are rigorously treated. Accordingly, the formulation of nonextensive statistical mechanics is amended based on the normal average. In addition, the Shore- Johnson theorem, which supports the use of the q-average, is carefully reexamined, and it is found that one of the axioms may not be appropriate for systems to be treated within the framework of nonextensive statistical mechanics. PACS number(s): 05.20.Dd, 05.20.Gg, 05.90.+m ____________________________ *) Permanent address 1 I. INTRODUCTION There exist a number of physical systems that possess exotic properties in view of traditional Boltzmann-Gibbs statistical mechanics. They are said to be statistical- mechanically anomalous, since they often exhibit and realize broken ergodicity, strong correlation between elements, (multi)fractality of phase-space/configuration-space portraits, and long-range interactions, for example. In the past decade, nonextensive statistical mechanics [1,2], which is a generalization of the Boltzmann-Gibbs theory, has been drawing continuous attention as a possible theoretical framework for describing these systems. -
Statistics: Challenges and Opportunities for the Twenty-First Century
This is page i Printer: Opaque this Statistics: Challenges and Opportunities for the Twenty-First Century Edited by: Jon Kettenring, Bruce Lindsay, & David Siegmund Draft: 6 April 2003 ii This is page iii Printer: Opaque this Contents 1 Introduction 1 1.1 The workshop . 1 1.2 What is statistics? . 2 1.3 The statistical community . 3 1.4 Resources . 5 2 Historical Overview 7 3 Current Status 9 3.1 General overview . 9 3.1.1 The quality of the profession . 9 3.1.2 The size of the profession . 10 3.1.3 The Odom Report: Issues in mathematics and statistics 11 4 The Core of Statistics 15 4.1 Understanding core interactivity . 15 4.2 A detailed example of interplay . 18 4.3 A set of research challenges . 20 4.3.1 Scales of data . 20 4.3.2 Data reduction and compression. 21 4.3.3 Machine learning and neural networks . 21 4.3.4 Multivariate analysis for large p, small n. 21 4.3.5 Bayes and biased estimation . 22 4.3.6 Middle ground between proof and computational ex- periment. 22 4.4 Opportunities and needs for the core . 23 4.4.1 Adapting to data analysis outside the core . 23 4.4.2 Fragmentation of core research . 23 4.4.3 Growth in the professional needs. 24 4.4.4 Research funding . 24 4.4.5 A Possible Program . 24 5 Statistics in Science and Industry 27 5.1 Biological Sciences . 27 5.2 Engineering and Industry . 33 5.3 Geophysical and Environmental Sciences . -
LECTURE 9 Statistical Mechanics Basic Methods We Have Talked
LECTURE 9 Statistical Mechanics Basic Methods We have talked about ensembles being large collections of copies or clones of a system with some features being identical among all the copies. There are three different types of ensembles in statistical mechanics. 1. If the system under consideration is isolated, i.e., not interacting with any other system, then the ensemble is called the microcanonical ensemble. In this case the energy of the system is a constant. 2. If the system under consideration is in thermal equilibrium with a heat reservoir at temperature T , then the ensemble is called a canonical ensemble. In this case the energy of the system is not a constant; the temperature is constant. 3. If the system under consideration is in contact with both a heat reservoir and a particle reservoir, then the ensemble is called a grand canonical ensemble. In this case the energy and particle number of the system are not constant; the temperature and the chemical potential are constant. The chemical potential is the energy required to add a particle to the system. The most common ensemble encountered in doing statistical mechanics is the canonical ensemble. We will explore many examples of the canonical ensemble. The grand canon- ical ensemble is used in dealing with quantum systems. The microcanonical ensemble is not used much because of the difficulty in identifying and evaluating the accessible microstates, but we will explore one simple system (the ideal gas) as an example of the microcanonical ensemble. Microcanonical Ensemble Consider an isolated system described by an energy in the range between E and E + δE, and similar appropriate ranges for external parameters xα. -
H Theorems in Statistical Fluid Dynamics
J. Phys. A: Math. Gen. 14 (1981) 1701-1718. Printed in Great Britain H theorems in statistical fluid dynamics George F Camevaleit, Uriel FrischO and Rick Salmon1 $National Center for Atmospheric Researchq, Boulder, Colorado 80307, USA §Division of Applied Sciences, Harvard University, Cambridge, Massachusetts 02138, USA and CNRS, Observatoire de Nice, Nice, France SScripps Institution of Oceanography, La Jolla, California 92093, USA Received 28 April 1980, in final form 6 November 1980 Abstract. It is demonstrated that the second-order Markovian closures frequently used in turbulence theory imply an H theorem for inviscid flow with an ultraviolet spectral cut-off. That is, from the inviscid closure equations, it follows that a certain functional of the energy spectrum (namely entropy) increases monotonically in time to a maximum value at absolute equilibrium. This is shown explicitly for isotropic homogeneous flow in dimensions d 3 2, and then a generalised theorem which covers a wide class of systems of current interest is presented. It is shown that the H theorem for closure can be derived from a Gibbs-type H theorem for the exact non-dissipative dynamics. 1. Introduction In the kinetic theory of classical and quantum many-particle systems, statistical evolution is described by a Boltzmann equation. This equation provides a collisional representation for nonlinear interactions, and through the Boltzmann H theorem it implies monotonic relaxation toward absolute canonical equilibrium. Here we show to what extent this same framework formally applies in statistical macroscopic fluid dynamics. Naturally, since canonical equilibrium applies only to conservative systems, a strong analogy can be produced only by confining ourselves to non-dissipative idealisations of fluid systems. -
Why Distinguish Between Statistics and Mathematical Statistics – the Case of Swedish Academia
Why distinguish between statistics and mathematical statistics { the case of Swedish academia Peter Guttorp1 and Georg Lindgren2 1Department of Statistics, University of Washington, Seattle 2Mathematical Statistics, Lund University, Lund 2017/10/11 Abstract A separation between the academic subjects statistics and mathematical statistics has existed in Sweden almost as long as there have been statistics professors. The same distinction has not been maintained in other countries. Why has it been kept so for long in Sweden, and what consequences may it have had? In May 2015 it was 100 years since Mathematical Statistics was formally estab- lished as an academic discipline at a Swedish university where Statistics had existed since the turn of the century. We give an account of the debate in Lund and elsewhere about this division dur- ing the first decades after 1900 and present two of its leading personalities. The Lund University astronomer (and mathematical statistician) C.V.L. Charlier was a lead- ing proponent for a position in mathematical statistics at the university. Charlier's adversary in the debate was Pontus Fahlbeck, professor in political science and statis- tics, who reserved the word statistics for \statistics as a social science". Charlier not only secured the first academic position in Sweden in mathematical statistics for his former Ph.D. student Sven Wicksell, but he also demonstrated that a mathematical statistician can be influential in matters of state, finance, as well as in different nat- ural sciences. Fahlbeck saw mathematical statistics as a set of tools that sometimes could be useful in his brand of statistics. After a summary of the organisational, educational, and scientific growth of the statistical sciences in Sweden that has taken place during the last 50 years, we discuss what effects the Charlier-Fahlbeck divergence might have had on this development. -
Science and Engineering Labor Force
National Science Board | Science & Engineering Indicators 2018 3 | 1 CHAPTER 3 Science and Engineering Labor Force Table of Contents Highlights................................................................................................................................................................................. 3-6 U.S. S&E Workforce: Definition, Size, and Growth ............................................................................................................ 3-6 S&E Workers in the Economy .............................................................................................................................................. 3-6 S&E Labor Market Conditions ............................................................................................................................................. 3-7 Demographics of the S&E Workforce ................................................................................................................................. 3-7 Global S&E Labor Force........................................................................................................................................................ 3-8 Introduction............................................................................................................................................................................. 3-9 Chapter Overview ................................................................................................................................................................. 3-9 Chapter