Hydrodynamics of Binary Bose- Einstein Condensates and Hydro- Elasticity of the Inner Crust of Neutron Stars
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Physical Vacuum Is a Special Superfluid Medium
Physical vacuum is a special superfluid medium Valeriy I. Sbitnev∗ St. Petersburg B. P. Konstantinov Nuclear Physics Institute, NRC Kurchatov Institute, Gatchina, Leningrad district, 188350, Russia; Department of Electrical Engineering and Computer Sciences, University of California, Berkeley, Berkeley, CA 94720, USA (Dated: August 9, 2016) The Navier-Stokes equation contains two terms which have been subjected to slight modification: (a) the viscosity term depends of time (the viscosity in average on time is zero, but its variance is non-zero); (b) the pressure gradient contains an added term describing the quantum entropy gradient multiplied by the pressure. Owing to these modifications, the Navier-Stokes equation can be reduced to the Schr¨odingerequation describing behavior of a particle into the vacuum being as a superfluid medium. Vortex structures arising in this medium show infinitely long life owing to zeroth average viscosity. The non-zero variance describes exchange of the vortex energy with zero-point energy of the vacuum. Radius of the vortex trembles around some average value. This observation sheds the light to the Zitterbewegung phenomenon. The long-lived vortex has a non-zero core where the vortex velocity vanishes. Keywords: Navier-Stokes; Schr¨odinger; zero-point fluctuations; superfluid vacuum; vortex; Bohmian trajectory; interference I. INTRODUCTION registered. Instead, the wave function represents it existence within an experimental scene [13]. A dramatic situation in physical understand- Another interpretation was proposed by Louis ing of the nature emerged in the late of 19th cen- de Broglie [18], which permits to explain such an tury. Observed phenomena on micro scales came experiment. In de Broglie's wave mechanics and into contradiction with the general positions of the double solution theory there are two waves. -
Phase Diagrams and Phase Separation
Phase Diagrams and Phase Separation Books MF Ashby and DA Jones, Engineering Materials Vol 2, Pergamon P Haasen, Physical Metallurgy, G Strobl, The Physics of Polymers, Springer Introduction Mixing two (or more) components together can lead to new properties: Metal alloys e.g. steel, bronze, brass…. Polymers e.g. rubber toughened systems. Can either get complete mixing on the atomic/molecular level, or phase separation. Phase Diagrams allow us to map out what happens under different conditions (specifically of concentration and temperature). Free Energy of Mixing Entropy of Mixing nA atoms of A nB atoms of B AM Donald 1 Phase Diagrams Total atoms N = nA + nB Then Smix = k ln W N! = k ln nA!nb! This can be rewritten in terms of concentrations of the two types of atoms: nA/N = cA nB/N = cB and using Stirling's approximation Smix = -Nk (cAln cA + cBln cB) / kN mix S AB0.5 This is a parabolic curve. There is always a positive entropy gain on mixing (note the logarithms are negative) – so that entropic considerations alone will lead to a homogeneous mixture. The infinite slope at cA=0 and 1 means that it is very hard to remove final few impurities from a mixture. AM Donald 2 Phase Diagrams This is the situation if no molecular interactions to lead to enthalpic contribution to the free energy (this corresponds to the athermal or ideal mixing case). Enthalpic Contribution Assume a coordination number Z. Within a mean field approximation there are 2 nAA bonds of A-A type = 1/2 NcAZcA = 1/2 NZcA nBB bonds of B-B type = 1/2 NcBZcB = 1/2 NZ(1- 2 cA) and nAB bonds of A-B type = NZcA(1-cA) where the factor 1/2 comes in to avoid double counting and cB = (1-cA). -
Suppression of Phase Separation in Lifepo4 Nanoparticles
Suppression of Phase Separation in LiFePO4 Nanoparticles During Battery Discharge Peng Bai,†,§ Daniel A. Cogswell† and Martin Z. Bazant*,†,‡ †Department of Chemical Engineering and ‡Department of Mathematics, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, Massachusetts 02139, USA §State Key Laboratory of Automotive Safety and Energy, Department of Automotive Engineering, Tsinghua University, Beijing 100084, P. R. China *Corresponding author: Dr. Martin Z. Bazant. Tel: (617)258-7039; Fax: (617)258-5766; Email: [email protected] August 8, 2011 ABSTRACT: Using a novel electrochemical phase-field model, we question the common belief that LixFePO4 nanoparticles separate into Li-rich and Li-poor phases during battery discharge. For small currents, spinodal decomposition or nucleation leads to moving phase boundaries. Above a critical current density (in the Tafel regime), the spinodal disappears, and particles fill homogeneously, which may explain the superior rate capability and long cycle life of nano-LiFePO4 cathodes. KEYWORDS: Li-ion battery, LiFePO4, phase-field model, Butler-Volmer equation, spinodal decomposition, intercalation waves. 1 Introduction. – LiFePO4-based electrochemical energy storage is one of the most promising developments for electric vehicle power systems and other high-rate applications such as power tools 2,3 and renewable energy storage. Nanoparticles of LiFePO4 have recently been used to demonstrate ultrafast battery discharge4 and high power density carbon pseudocapacitors.5 However, the -
Conformal Field Theory out of Equilibrium: a Review Denis Bernard
Conformal field theory out of equilibrium: a review Denis Bernard| and Benjamin Doyon♠ | Laboratoire de Physique Th´eoriquede l'Ecole Normale Sup´erieurede Paris, CNRS, ENS & PSL Research University, UMPC & Sorbonne Universit´es,France. ♠ Department of Mathematics, King's College London, London, United Kingdom. We provide a pedagogical review of the main ideas and results in non-equilibrium conformal field theory and connected subjects. These concern the understanding of quantum transport and its statistics at and near critical points. Starting with phenomenological considerations, we explain the general framework, illustrated by the example of the Heisenberg quantum chain. We then introduce the main concepts underlying conformal field theory (CFT), the emergence of critical ballistic transport, and the CFT scattering construction of non-equilibrium steady states. Using this we review the theory for energy transport in homogeneous one-dimensional critical systems, including the complete description of its large deviations and the resulting (extended) fluctuation relations. We generalize some of these ideas to one-dimensional critical charge transport and to the presence of defects, as well as beyond one-dimensional criticality. We describe non-equilibrium transport in free-particle models, where connections are made with generalized Gibbs ensembles, and in higher-dimensional and non-integrable quantum field theories, where the use of the powerful hydrodynamic ideas for non-equilibrium steady states is explained. We finish with a list of open questions. The review does not assume any advanced prior knowledge of conformal field theory, large-deviation theory or hydrodynamics. March 24, 2016 Contents 1 Introduction 1 2 Mesoscopic electronic transport: basics 3 2.1 Elementary phenomenology . -
1504.05850V4.Pdf
Compact Stars in the QCD Phase Diagram IV (CSQCD IV) September 26-30, 2014, Prerow, Germany http://www.ift.uni.wroc.pl/˜csqcdiv Entropic and enthalpic phase transitions in high energy density nuclear matter Igor Iosilevskiy1,2 1 Joint Institute for High Temperatures (Russian Academy of Sciences), Izhorskaya Str. 13/2, 125412 Moscow, Russia 2 Moscow Institute of Physics and Technology (State Research University), Dolgoprudny, 141700, Moscow Region, Russia 1 Abstract Features of Gas-Liquid (GL) and Quark-Hadron (QH) phase transitions (PT) in dense nuclear matter are under discussion in comparison with their terrestrial coun- terparts, e.g. so-called ”plasma” PT in shock-compressed hydrogen, nitrogen etc. Both, GLPT and QHPT, when being represented in widely accepted temperature – baryonic chemical potential plane, are often considered as similar, i.e. amenable to one-to-one mapping by simple scaling. It is argued that this impression is illusive and that GLPT and QHPT belong to different classes: GLPT is typical enthalpic PT (Van-der-Waals-like) while QHPT (”deconfinement-driven”) is typical entropic PT. Subdivision of 1st-order fluid-fluid phase transitions into enthalpic and entropic subclasses was proposed in [arXiv:1403.8053]. Properties of enthalpic and entropic PTs differ significantly. Entropic PT is always internal part of more general and ex- tended thermodynamic anomaly – domains with abnormal (negative) sign for the set of (usually positive) second derivatives of thermodynamic potential, e.g. Gruneizen and thermal expansion and thermal pressure coefficients etc. Negative sign of these derivatives lead to violation of standard behavior and relative order for many iso-lines in P –V plane, e.g. -
Arxiv:2010.01933V2 [Cond-Mat.Quant-Gas] 18 Feb 2021 Tigated in Refs
Finite temperature spin dynamics of a two-dimensional Bose-Bose atomic mixture Arko Roy,1, ∗ Miki Ota,1, ∗ Alessio Recati,1, 2 and Franco Dalfovo1 1INO-CNR BEC Center and Universit`adi Trento, via Sommarive 14, I-38123 Trento, Italy 2Trento Institute for Fundamental Physics and Applications, INFN, 38123 Povo, Italy We examine the role of thermal fluctuations in uniform two-dimensional binary Bose mixtures of dilute ultracold atomic gases. We use a mean-field Hartree-Fock theory to derive analytical predictions for the miscible-immiscible transition. A nontrivial result of this theory is that a fully miscible phase at T = 0 may become unstable at T 6= 0, as a consequence of a divergent behaviour in the spin susceptibility. We test this prediction by performing numerical simulations with the Stochastic (Projected) Gross-Pitaevskii equation, which includes beyond mean-field effects. We calculate the equilibrium configurations at different temperatures and interaction strengths and we simulate spin oscillations produced by a weak external perturbation. Despite some qualitative agreement, the comparison between the two theories shows that the mean-field approximation is not able to properly describe the behavior of the two-dimensional mixture near the miscible-immiscible transition, as thermal fluctuations smoothen all sharp features both in the phase diagram and in spin dynamics, except for temperature well below the critical temperature for superfluidity. I. INTRODUCTION ing the Popov theory. It is then natural to ask whether such a phase-transition also exists in 2D. The study of phase-separation in two-component clas- It is worth stressing that, in 2D Bose gases, thermal sical fluids is of paramount importance and the role of fluctuations are much more important than in 3D, as they temperature can be rather nontrivial. -
Nucleation Initiated Spinodal Decomposition in a Polymerizing System Thein Yk U University of Akron Main Campus, [email protected]
The University of Akron IdeaExchange@UAkron College of Polymer Science and Polymer Engineering 5-1996 Nucleation Initiated Spinodal Decomposition in a Polymerizing System Thein yK u University of Akron Main Campus, [email protected] Jae Hyung Lee University of Akron Main Campus Please take a moment to share how this work helps you through this survey. Your feedback will be important as we plan further development of our repository. Follow this and additional works at: http://ideaexchange.uakron.edu/polymer_ideas Part of the Polymer Science Commons Recommended Citation Kyu, Thein nda Lee, Jae Hyung, "Nucleation Initiated Spinodal Decomposition in a Polymerizing System" (1996). College of Polymer Science and Polymer Engineering. 67. http://ideaexchange.uakron.edu/polymer_ideas/67 This Article is brought to you for free and open access by IdeaExchange@UAkron, the institutional repository of The nivU ersity of Akron in Akron, Ohio, USA. It has been accepted for inclusion in College of Polymer Science and Polymer Engineering by an authorized administrator of IdeaExchange@UAkron. For more information, please contact [email protected], [email protected]. VOLUME 76, NUMBER 20 PHYSICAL REVIEW LETTERS 13MAY 1996 Nucleation Initiated Spinodal Decomposition in a Polymerizing System Thein Kyu and Jae-Hyung Lee Institute of Polymer Engineering, The University of Akron, Akron, Ohio 44325 (Received 29 September 1995) Dynamics of phase separation in a polymerizing system, consisting of carboxyl terminated polybutadiene acrylonitrile/epoxy/methylene dianiline, was investigated by means of time-resolved light scattering. The initial length scale was found to decrease for some early periods of the reaction which has been explained in the context of nucleation initiated spinodal decomposition. -
Stochastic Hydrodynamic Analogy of Quantum Mechanics
The mass lowest limit of a black hole: the hydrodynamic approach to quantum gravity Piero Chiarelli National Council of Research of Italy, Area of Pisa, 56124 Pisa, Moruzzi 1, Italy Interdepartmental Center “E.Piaggio” University of Pisa Phone: +39-050-315-2359 Fax: +39-050-315-2166 Email: [email protected]. Abstract: In this work the quantum gravitational equations are derived by using the quantum hydrodynamic description. The outputs of the work show that the quantum dynamics of the mass distribution inside a black hole can hinder its formation if the mass is smaller than the Planck's one. The quantum-gravitational equations of motion show that the quantum potential generates a repulsive force that opposes itself to the gravitational collapse. The eigenstates in a central symmetric black hole realize themselves when the repulsive force of the quantum potential becomes equal to the gravitational one. The work shows that, in the case of maximum collapse, the mass of the black hole is concentrated inside a sphere whose radius is two times the Compton length of the black hole. The mass minimum is determined requiring that the gravitational radius is bigger than or at least equal to the radius of the state of maximum collapse. PACS: 04.60.-m Keywords: quantum gravity, minimum black hole mass, Planck's mass, quantum Kaluza Klein model 1. Introduction One of the unsolved problems of the theoretical physics is that of unifying the general relativity with the quantum mechanics. The former theory concerns the gravitation dynamics on large cosmological scale in a fully classical ambit, the latter one concerns, mainly, the atomic or sub-atomic quantum phenomena and the fundamental interactions [1-9]. -
Spinodal Lines and Equations of State: a Review
10 l Nuclear Engineering and Design 95 (1986) 297-314 297 North-Holland, Amsterdam SPINODAL LINES AND EQUATIONS OF STATE: A REVIEW John H. LIENHARD, N, SHAMSUNDAR and PaulO, BINEY * Heat Transfer/ Phase-Change Laboratory, Mechanical Engineering Department, University of Houston, Houston, TX 77004, USA The importance of knowing superheated liquid properties, and of locating the liquid spinodal line, is discussed, The measurement and prediction of the spinodal line, and the limits of isentropic pressure undershoot, are reviewed, Means are presented for formulating equations of state and fundamental equations to predict superheated liquid properties and spinodal limits, It is shown how the temperature dependence of surface tension can be used to verify p - v - T equations of state, or how this dependence can be predicted if the equation of state is known. 1. Scope methods for making simplified predictions of property information, which can be applied to the full range of Today's technology, with its emphasis on miniaturiz fluids - water, mercury, nitrogen, etc. [3-5]; and predic ing and intensifying thennal processes, steadily de tions of the depressurizations that might occur in ther mands higher heat fluxes and poses greater dangers of mohydraulic accidents. (See e.g. refs. [6,7].) sending liquids beyond their boiling points into the metastable, or superheated, state. This state poses the threat of serious thermohydraulic explosions. Yet we 2. The spinodal limit of liquid superheat know little about its thermal properties, and cannot predict process behavior after a liquid becomes super heated. Some of the practical situations that require a 2.1. The role of the equation of state in defining the spinodal line knowledge the limits of liquid superheat, and the physi cal properties of superheated liquids, include: - Thennohydraulic explosions as might occur in nuclear Fig. -
Notes on Phase Seperation Chem 130A Fall 2002 Prof
Notes on Phase Seperation Chem 130A Fall 2002 Prof. Groves Consider the process: Pure 1 + Pure 2 Æ Mixture of 1 and 2 We have previously derived the entropy of mixing for this process from statistical principles and found it to be: ∆ =− − Smix kN11ln X kN 2 ln X 2 where N1 and N2 are the number of molecules of type 1 and 2, respectively. We use k, the Boltzmann constant, since N1 and N2 are number of molecules. We could alternatively use R, the gas constant, if we chose to represent the number of molecules in terms of moles. X1 and X2 represent the mole fraction (e.g. X1 = N1 / (N1+N2)) of 1 and 2, respectively. If there are interactions between the two ∆ components, there will be a non-zero Hmix that we must consider. We can derive an expression ∆H = 2γ ∆ ∆ for Hmix using H of swapping one molecule of type 1, in pure type 1, with one molecule of type 2, in pure type 2 (see adjacent figure). We define γ as half of this ∆H of interchange. It is a differential interaction energy that tells us the energy difference between 1:1 and 2:2 interactions and 1:2 interactions. By defining 2γ = ∆H, γ represents the energy change associated with one molecule (note that two were involved in the swap). ∆ γ Now, to calculate Hmix from , we first consider 1 molecule of type 1 in the mixed system. For the moment we need not be concerned with whether or not they actually will mix, we just want ∆ to calculate Hmix as if they mix thoroughly. -
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News 6/2013 Physics H. Friedrich, TU München, Germany R. Gendler, Rob Gendler Astropics, Avon, CT, USA G. Ghisellini, The Astronomical Observatory of Brera, Scattering Theory (Ed) Merate, Italy Lessons from the Masters Radiative Processes in High This book presents a concise and modern coverage of scattering theory. It is motivated by the fact that Current Concepts in Astronomical Image Energy Astrophysics experimental advances have shifted and broad- Processing This book grew out of the author’s notes from his ened the scope of applications where concepts course on Radiative Processes in High Energy from scattering theory are used, e.g. to the field of There are currently thousands of amateur astrono- Astrophysics. The course provides fundamental ultracold atoms and molecules, which has been mers around the world engaged in astrophotogra- definitions of radiative processes and serves as a experiencing enormous growth in recent years, phy at a sophisticated level. brief introduction to Bremsstrahlung and black largely triggered by the successful realization of Features body emission, relativistic beaming, synchrotron Bose-Einstein condensates of dilute atomic gases 7 Written by a brilliant body of recognized emission and absorption, Compton scattering, in 1995. In the present treatment, special atten- leaders 7 Contains the most current, sophisti- synchrotron self-compton emission, pair creation tion is given to the role played by the long-range cated and useful information on astrophotogra- and emission. The final chapter discusses the ob- behaviour of the projectile-target interaction, phy 7 Covers all types of astronomical image served features of Active Galactic Nuclei and their and a theory is developed, which is well suited processing, including processing of events such interpretation based on the radiative processes to describe near-threshold bound and continuum as eclipses, using DSLRs, and deep sky, planetary, presented in the book. -
Arxiv:2105.05054V2 [Cond-Mat.Stat-Mech] 1 Sep 2021 2
Exact entanglement growth of a one-dimensional hard-core quantum gas during a free expansion Stefano Scopa1, Alexandre Krajenbrink1, Pasquale Calabrese1;2 and Jer´ omeˆ Dubail3 1 SISSA and INFN, via Bonomea 265, 34136 Trieste, Italy 2 International Centre for Theoretical Physics (ICTP), I-34151, Trieste, Italy 3 Universite´ de Lorraine, CNRS, LPCT, F-54000 Nancy, France Abstract. We consider the non-equilibrium dynamics of the entanglement entropy of a one- dimensional quantum gas of hard-core particles, initially confined in a box potential at zero temperature. At t = 0 the right edge of the box is suddenly released and the system is let free to expand. During this expansion, the initially correlated region propagates with a non-homogeneous profile, leading to the growth of entanglement entropy. This setting is investigated in the hydrodynamic regime, with tools stemming from semi-classical Wigner function approach and with recent developments of quantum fluctuating hydrodynamics. Within this framework, the entanglement entropy can be associated to a correlation function of chiral twist-fields of the conformal field theory that lives along the Fermi contour and it can be exactly determined. Our predictions for the entanglement evolution are found in agreement with and generalize previous results in literature based on numerical calculations and heuristic arguments. arXiv:2105.05054v2 [cond-mat.stat-mech] 1 Sep 2021 2 Contents 1 Introduction3 2 Setup and main result5 2.1 The model: free expansion of a lattice hard-core gas . .5 2.2 Previous results in the literature . .6 2.3 Main result of this paper . .7 3 Classical and quantum fluctuating hydrodynamic description8 3.1 Continuum limit and regularization of the problem .