Time and Relativity
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Path Integrals in Quantum Mechanics
Path Integrals in Quantum Mechanics Dennis V. Perepelitsa MIT Department of Physics 70 Amherst Ave. Cambridge, MA 02142 Abstract We present the path integral formulation of quantum mechanics and demon- strate its equivalence to the Schr¨odinger picture. We apply the method to the free particle and quantum harmonic oscillator, investigate the Euclidean path integral, and discuss other applications. 1 Introduction A fundamental question in quantum mechanics is how does the state of a particle evolve with time? That is, the determination the time-evolution ψ(t) of some initial | i state ψ(t ) . Quantum mechanics is fully predictive [3] in the sense that initial | 0 i conditions and knowledge of the potential occupied by the particle is enough to fully specify the state of the particle for all future times.1 In the early twentieth century, Erwin Schr¨odinger derived an equation specifies how the instantaneous change in the wavefunction d ψ(t) depends on the system dt | i inhabited by the state in the form of the Hamiltonian. In this formulation, the eigenstates of the Hamiltonian play an important role, since their time-evolution is easy to calculate (i.e. they are stationary). A well-established method of solution, after the entire eigenspectrum of Hˆ is known, is to decompose the initial state into this eigenbasis, apply time evolution to each and then reassemble the eigenstates. That is, 1In the analysis below, we consider only the position of a particle, and not any other quantum property such as spin. 2 D.V. Perepelitsa n=∞ ψ(t) = exp [ iE t/~] n ψ(t ) n (1) | i − n h | 0 i| i n=0 X This (Hamiltonian) formulation works in many cases. -
The Second Law of Thermodynamics Forbids Time Travel
Cosmology, 2014, Vol. 18. 212-222 Cosmology.com, 2014 The Second Law Of Thermodynamics Forbids Time Travel Marko Popovic Department of Chemistry and Biochemistry, Brigham Young University, Provo, UT 84602, USA Abstract Four space-time coordinates define one thermodynamic parameter - Volume. Cell/ organism growth is one of the most fundamental properties of living creatures. The growth is characterized by irreversible change of the volume of the cell/organism. This irreversible change of volume (growth of the cell/organism) makes the system irreversibly change its thermodynamic state. Irreversible change of the systems thermodynamic state makes impossible return to the previous state characterized by state parameters. The impossibility to return the system to the previous state leads to conclusion that even to artificially turn back the arrow of time (as a parameter), it is not possible to turn back the state of the organism and its surroundings. Irreversible change of thermodynamic state of the organism is also consequence of the accumulation of entropy during life. So even if we find the way to turn back the time arrow it is impossible to turn back the state of the thermodynamic system (including organism) because of irreversibility of thermodynamic/ physiologic processes in it. Keywords: Time travel, Entropy, Living Organism, Surroundings, Irreversibility Cosmology, 2014, Vol. 18. 212-222 Cosmology.com, 2014 1. Introduction The idea of time travel has fascinated humanity since ancient times and can be found in texts as old as Mahabharata and Talmud. Later it continued to be developed in literature (i.e. Dickens' “A Christmas Carol”, or Twain's “A Connecticut Yankee in King Arthur's Court”…). -
Basics of Thermal Field Theory
September 2021 Basics of Thermal Field Theory A Tutorial on Perturbative Computations 1 Mikko Lainea and Aleksi Vuorinenb aAEC, Institute for Theoretical Physics, University of Bern, Sidlerstrasse 5, CH-3012 Bern, Switzerland bDepartment of Physics, University of Helsinki, P.O. Box 64, FI-00014 University of Helsinki, Finland Abstract These lecture notes, suitable for a two-semester introductory course or self-study, offer an elemen- tary and self-contained exposition of the basic tools and concepts that are encountered in practical computations in perturbative thermal field theory. Selected applications to heavy ion collision physics and cosmology are outlined in the last chapter. 1An earlier version of these notes is available as an ebook (Springer Lecture Notes in Physics 925) at dx.doi.org/10.1007/978-3-319-31933-9; a citable eprint can be found at arxiv.org/abs/1701.01554; the very latest version is kept up to date at www.laine.itp.unibe.ch/basics.pdf. Contents Foreword ........................................... i Notation............................................ ii Generaloutline....................................... iii 1 Quantummechanics ................................... 1 1.1 Path integral representation of the partition function . ....... 1 1.2 Evaluation of the path integral for the harmonic oscillator . ..... 6 2 Freescalarfields ..................................... 13 2.1 Path integral for the partition function . ... 13 2.2 Evaluation of thermal sums and their low-temperature limit . .... 16 2.3 High-temperatureexpansion. 23 3 Interactingscalarfields............................... ... 30 3.1 Principles of the weak-coupling expansion . 30 3.2 Problems of the naive weak-coupling expansion . .. 38 3.3 Proper free energy density to (λ): ultraviolet renormalization . 40 O 3 3.4 Proper free energy density to (λ 2 ): infraredresummation . -
The Arrow of Time Volume 7 Paul Davies Summer 2014 Beyond Center for Fundamental Concepts in Science, Arizona State University, Journal Homepage P.O
The arrow of time Volume 7 Paul Davies Summer 2014 Beyond Center for Fundamental Concepts in Science, Arizona State University, journal homepage P.O. Box 871504, Tempe, AZ 852871504, USA. www.euresisjournal.org [email protected] Abstract The arrow of time is often conflated with the popular but hopelessly muddled concept of the “flow” or \passage" of time. I argue that the latter is at best an illusion with its roots in neuroscience, at worst a meaningless concept. However, what is beyond dispute is that physical states of the universe evolve in time with an objective and readily-observable directionality. The ultimate origin of this asymmetry in time, which is most famously captured by the second law of thermodynamics and the irreversible rise of entropy, rests with cosmology and the state of the universe at its origin. I trace the various physical processes that contribute to the growth of entropy, and conclude that gravitation holds the key to providing a comprehensive explanation of the elusive arrow. 1. Time's arrow versus the flow of time The subject of time's arrow is bedeviled by ambiguous or poor terminology and the con- flation of concepts. Therefore I shall begin my essay by carefully defining terms. First an uncontentious statement: the states of the physical universe are observed to be distributed asymmetrically with respect to the time dimension (see, for example, Refs. [1, 2, 3, 4]). A simple example is provided by an earthquake: the ground shakes and buildings fall down. We would not expect to see the reverse sequence, in which shaking ground results in the assembly of a building from a heap of rubble. -
Euclidean Field Theory
February 2, 2011 Euclidean Field Theory Kasper Peeters & Marija Zamaklar Lecture notes for the M.Sc. in Elementary Particle Theory at Durham University. Copyright c 2009-2011 Kasper Peeters & Marija Zamaklar Department of Mathematical Sciences University of Durham South Road Durham DH1 3LE United Kingdom http://maths.dur.ac.uk/users/kasper.peeters/eft.html [email protected] [email protected] 1 Introducing Euclidean Field Theory5 1.1 Executive summary and recommended literature............5 1.2 Path integrals and partition sums.....................7 1.3 Finite temperature quantum field theory.................8 1.4 Phase transitions and critical phenomena................ 10 2 Discrete models 15 2.1 Ising models................................. 15 2.1.1 One-dimensional Ising model................... 15 2.1.2 Two-dimensional Ising model................... 18 2.1.3 Kramers-Wannier duality and dual lattices........... 19 2.2 Kosterlitz-Thouless model......................... 21 3 Effective descriptions 25 3.1 Characterising phase transitions..................... 25 3.2 Mean field theory.............................. 27 3.3 Landau-Ginzburg.............................. 28 4 Universality and renormalisation 31 4.1 Kadanoff block scaling........................... 31 4.2 Renormalisation group flow........................ 33 4.2.1 Scaling near the critical point................... 33 4.2.2 Critical surface and universality................. 34 4.3 Momentum space flow and quantum field theory........... 35 5 Lattice gauge theory 37 5.1 Lattice action................................. 37 5.2 Wilson loops................................. 38 5.3 Strong coupling expansion and confinement.............. 39 5.4 Monopole condensation.......................... 39 3 4 1 Introducing Euclidean Field Theory 1.1. Executive summary and recommended literature This course is all about the close relation between two subjects which at first sight have very little to do with each other: quantum field theory and the theory of criti- cal statistical phenomena. -
Ads/CFT Correspondence
AdS/CFT Correspondence GEORGE SIOPSIS Department of Physics and Astronomy The University of Tennessee Knoxville, TN 37996-1200 U.S.A. e-mail: [email protected] Notes by James Kettner Fall 2010 ii Contents 1 Path Integral 1 1.1 Quantum Mechanics ........................ 1 1.2 Statistical Mechanics ........................ 3 1.3 Thermodynamics .......................... 4 1.3.1 Canonical ensemble . 4 1.3.2 Microcanonical ensemble . 4 1.4 Field Theory ............................. 4 2 Schwarzschild Black Hole 7 3 Reissner-Nordstrom¨ Black Holes 11 3.1 The holes . 11 3.2 Extremal limit . 13 3.3 Generalizations . 15 3.3.1 Multi-center solution . 15 3.3.2 Arbitrary dimension . 16 3.3.3 Kaluza-Klein reduction . 17 4 Black Branes from String Theory 19 5 Microscopic calculation of Entropy and Hawking Radiation 23 5.1 The hole . 23 5.2 Entropy . 25 5.3 Finite temperature . 27 5.4 Scattering and Hawking radiation . 29 iii iv CONTENTS LECTURE 1 Path Integral 1.1 Quantum Mechanics Set ~ = 1. Given a particle described by coordinates (q, t) with initial and final coor- dinates of (qi, ti) and (qf , tf ), the amplitude of the transition is ∗ hqi, ti | qf , tf i = hψ |qf , tf i = ψ (qf , tf ) . where ψ satisfies the Schrodinger¨ equation ∂ψ 1 ∂2ψ i = − . ∂t 2m ∂q2 Feynman introduced the path integral formalism Z −iS hqi, ti | qf , tf i = [dq] e q(ti)=qi,q(tf )=qf R where S = dtL is the action and L = L(q, q˙) is the Lagrangian, e.g., 1 L = mq˙2 − V (q) 2 We convert to imaginary time via the Wick rotation τ = it so 1 L → − mq˙2 − V (q) ≡ −L 2 E where the derivative is with respect to τ, LE is the total energy (which is bounded Rbelow), and the subscript E stands for Euclidean. -
On Mass Interaction Principle
On Mass Interaction Principle Chu-Jun Gu∗ Institute of Theoretical Physics, Grand Genius Group, 100085, Beijing, China 1 2 Abstract This paper proposes mass interaction principle (MIP) as: the particles will be subjected to the random frictionless quantum Brownian motion by the collision of space time particle (STP) prevalent in spacetime. The change in the amount of action of the particles during each collision is an integer multiple of the Planck constant h. The motion of particles under the action of STP is a quantum Markov process. Under this principle, we infer that the statistical inertial mass of a particle is a statistical property that characterizes the difficulty of particle diffusion in spacetime. Starting from this principle, this article has the following six aspects of work: First, we derive the mass-diffusion coefficient uncertainty and the quantized commutation, and derive the most basic coordinate-momentum uncertainty and time-energy uncertainty of quantum mechanics, and then clearly reveal the particle-wave duality, which are properties exhibited by particles collided by STP. Second, we created the three decompositions of particles velocity. The comprehensive property of three velocities deduced the equation of motion of the particle as Schrödinger equation, and made a novel interpretation of Heisenberg’s uncertainty principle and Feynman’s path integral expression. And reexamine the quantum measurement problem, so that the EPR paradox can be explained in a self-consistent manner. Third, we reinterpret the physical origin of quantum spins. Each spacetime random impact not only gives the particle of matter the action of a Planck constant , but also produces the quantum fluctuation properties of the material particles. -
Arxiv:2006.02298V1 [Gr-Qc] 3 Jun 2020
Lorentzian quantum cosmology in novel Gauss-Bonnet gravity from Picard-Lefschetz methods Gaurav Narain a∗ and Hai-Qing Zhang a,b† a Center for Gravitational Physics, Department of Space Science, Beihang University, Beijing 100191, China. b International Research Institute for Multidisciplinary Science, Beihang University, Beijing 100191, China Abstract In this paper we study some aspects of classical and quantum cosmology in the novel-Gauss- Bonnet (nGB) gravity in four space-time dimensions. Starting with a generalised Friedmann- Lemaˆıtre-Robertson-Walker (FLRW) metric respecting homogeneity and isotropicity in arbitrary space-time dimension D, we find the action of theory in four spacetime dimension where the limit D 4 is smoothly obtained after an integration by parts. The peculiar rescaling of Gauss-Bonnet → coupling by factor of D 4 results in a non-trivial contribution to the action. We study the system − of equation of motion to first order nGB coupling. We then go on to compute the transition probability from one 3-geometry to another directly in Lorentzian signature. We make use of combination of WKB approximation and Picard-Lefschetz (PL) theory to achieve our aim. PL theory allows to analyse the path-integral directly in Lorentzian signature without doing Wick rotation. Due to complication caused by non-linear nature of action, we compute the transition amplitude to first order in nGB coupling. We find non-trivial correction coming from the nGB coupling to the transition amplitude, even if the analysis was done perturbatively. We use this result to investigate the case of classical boundary conditions. arXiv:2006.02298v1 [gr-qc] 3 Jun 2020 ∗ [email protected] † [email protected] 1 I. -
1 Temporal Arrows in Space-Time Temporality
Temporal Arrows in Space-Time Temporality (…) has nothing to do with mechanics. It has to do with statistical mechanics, thermodynamics (…).C. Rovelli, in Dieks, 2006, 35 Abstract The prevailing current of thought in both physics and philosophy is that relativistic space-time provides no means for the objective measurement of the passage of time. Kurt Gödel, for instance, denied the possibility of an objective lapse of time, both in the Special and the General theory of relativity. From this failure many writers have inferred that a static block universe is the only acceptable conceptual consequence of a four-dimensional world. The aim of this paper is to investigate how arrows of time could be measured objectively in space-time. In order to carry out this investigation it is proposed to consider both local and global arrows of time. In particular the investigation will focus on a) invariant thermodynamic parameters in both the Special and the General theory for local regions of space-time (passage of time); b) the evolution of the universe under appropriate boundary conditions for the whole of space-time (arrow of time), as envisaged in modern quantum cosmology. The upshot of this investigation is that a number of invariant physical indicators in space-time can be found, which would allow observers to measure the lapse of time and to infer both the existence of an objective passage and an arrow of time. Keywords Arrows of time; entropy; four-dimensional world; invariance; space-time; thermodynamics 1 I. Introduction Philosophical debates about the nature of space-time often centre on questions of its ontology, i.e. -
The Origin of the Universe and the Arrow of Time
The Origin of the Universe and the Arrow of Time Sean M Carroll Caltech, Pasadena, CA One of the most obvious facts about the universe is that the past is different from the future. The world around us is full of irreversible processes: we can turn an egg into an omelet, but can't turn an omelet into an egg. Physicists have codified this difference into the Second Law of Thermodynamics: the entropy of a closed system always increases with time. But why? The ultimate explanation is to be found in cosmology: special conditions in the early universe are responsible for the arrow of time. I will talk about the nature of time, the origin of entropy, and how what happened before the Big Bang may be responsible for the arrow of time we observe today. Sean Carroll is a Senior Research Associate in Physics at the California Institute of Technology. He received his Ph.D. in 1993 from Harvard University, and has previously worked as a postdoctoral researcher at the Center for Theoretical Physics at MIT and at the Institute for Theoretical Physics at the University of California, Santa Barbara, as well as on the faculty at the University of Chicago. His research ranges over a number of topics in theoretical physics, focusing on cosmology, field theory, particle physics, and gravitation. Carroll is the author of From Eternity to Here: The Quest for the Ultimate Theory of Time, an upcoming popular-level book on cosmology and the arrow of time. He has also written a graduate textbook, Spacetime and Geometry: An Introduction to General Relativity, and recorded a set of lectures on cosmology for the Teaching Company. -
Causality Is an Effect, II
entropy Article Causality Is an Effect, II Lawrence S. Schulman Physics Department, Clarkson University, Potsdam, NY 13699-5820, USA; [email protected] Abstract: Causality follows the thermodynamic arrow of time, where the latter is defined by the direction of entropy increase. After a brief review of an earlier version of this article, rooted in classical mechanics, we give a quantum generalization of the results. The quantum proofs are limited to a gas of Gaussian wave packets. Keywords: causality; arrow of time; entropy increase; quantum generalization; Gaussian wave packets 1. Introduction The history of multiple time boundary conditions goes back—as far as I know—to Schottky [1,2], who, in 1921, considered a single slice of time inadequate for prediction or retrodiction (see AppendixA). There was later work of Watanabe [ 3] concerned with predic- tion and retrodiction. Then, Schulman [4] uses this as a conceptual way to eliminate “initial conditions” prejudice from Gold’s [5] rationale for the arrow of time and Wheeler [6,7] discusses two time boundary conditions. Gell–Mann and Hartle also contributed to this subject [8] and include a review of some previous work. Finally, Aharonov et al. [9,10] pro- posed that this could solve the measurement problem of quantum mechanics, although this is disputed [11]. See also AppendixB. This formalism has also allowed me to come to a conclusion: effect follows cause in the direction of entropy increase. This result is not unanticipated; most likely everything Citation: Schulman, L.S. Causality Is having to do with arrows of time has been anticipated. What is unusual, however, is the an Effect, II. -
The Nature and Origin of Time-Asymmetric Spacetime Structures*
The nature and origin of time-asymmetric spacetime structures* H. D. Zeh (University of Heidelberg) www.zeh-hd.de Abstract: Time-asymmetric spacetime structures, in particular those representing black holes and the expansion of the universe, are intimately related to other arrows of time, such as the second law and the retardation of radiation. The nature of the quantum ar- row, often attributed to a collapse of the wave function, is essential, in particular, for understanding the much discussed "black hole information loss paradox". However, this paradox assumes a new form and might not even occur in a consistent causal treatment that would prevent the formation of horizons and singularities. A “master arrow”, which combines all arrows of time, does not have to be identified with the direction of a formal time parameter that serves to define the dynamics as a succes- sion of global states (a trajectory in configuration or Hilbert space). It may even change direction with respect to a fundamental physical clock, such as the cosmic expansion parameter if this was formally extended either into a future contraction era or to nega- tive "pre-big-bang" values. 1 Introduction Since gravity is attractive, most gravitational phenomena are asymmetric in time: ob- jects fall down or contract under the influence of gravity. In General Relativity, this asymmetry leads to drastically asymmetric spacetime structures, such as future hori- zons and future singularities as properties of black holes. However, since the relativistic and nonrelativistic laws of gravitation are symmetric under time reversal, all time asymmetries must arise as consequences of specific (only seemingly "normal") initial conditions, for example a situation of rest that can be prepared by means of other ar- * arXiv:1012.4708v11.