Computational Studies of Particle Dynamics during Magnetic Reconnection
|
|
- Wilfred Collins
- 5 years ago
- Views:
Transcription
1 Computational Studies of Particle Dynamics during Magnetic Reconnection Rebecca Melkerson (Washington and Lee University) Marc Swisdak, Ph.D. (UMD); James Drake, Ph.D. (UMD)
2 Background & Motivation During reconnection, magnetic field lines change topology and convert magnetic energy to kinetic and thermal particle energies. 11 August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 2
3 Background & Motivation Reconnection occurs in many space and astrophysical plasmas. The resultant charged particles have potentially hazardous consequences upon reaching earth. image by Soerfm, distributed under CC-BY-SA-3.0 license 11 August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 3
4 About the Simulations Particle-in-cell (PIC) simulations on massively parallel code 2D or 3D: reconnection occurs in xy-plane Code tracks E, B, J &, J ', P &, P ' (pressure tensors), n &, and n ' Example out of plane electron current: Jez 11 August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 4
5 Power Laws in Electron Energy Distributions Power laws arise when the governing physical processes are nominally scale invariant. In-situ observations of magnetic reconnection show power law (non-thermal) electron energy distribution production, but simulations have difficulty producing them. M. Øieroset et. al August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 5
6 Power Laws in Electron Energy Distributions There has been a recent claim of power law production in a 3D simulation, so we looked for power laws in a 3D simulation with similar parameters (guide field of 2 vs 1). Buechner et. al Buechner et. al E averaged over z direction Spatial distribution of E through central plane 11 August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 6
7 Power Laws in Electron Energy Distributions We are not convinced that the data shows a power law. Linear span is only ~1 order of magnitude. Gaussians can add to give illusion of linear region. Solid: initial Dashed: final f(e) Buechner et. al Energy 11 August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 7
8 Effect of β on Electron Energization We run 2D simulations with 5 different values for β, the ratio of thermal to magnetic pressure. We utilize a guiding-center model to evaluate electron energization: -. = E -/ J + p &, + m & n & u 6 &, u 7 κ + : ;,< >= + u = >/ 7 B The terms represent direct electric field acceleration fermi acceleration acceleration by magnetic moment conservation 11 August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 8
9 Effect of β on Electron Energization Energization Magnitude Energization vs Log(β) log(β ) Direct E field Fermi Magnetic moment Direct E field Fermi Magnetic moment ENERGIZATION KEY: Direct E field, increased particles per grid Fermi, increased ppg Magnetic moment, increased ppg Example figures. Graph values obtained by averaging over boxes as shown. 11 August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 9
10 Summary & Acknowledgements We analyzed a 3D simulation with similar parameters to the one claimed to show power laws, yet we still do not believe the data yields non-thermal electronenergydistributions. We find that Fermi acceleration is generally the most significant source of electron energization, with an uptick for low β, but we do not yet understand why. REU program sponsored by the National Science Foundation Award Number: PHY August 2017 TREND 2017: Computational Studies of Particle Dynamics during Magnetic Reconnection 10
Particle acceleration during 2D and 3D magnetic reconnection
Particle acceleration during 2D and 3D magnetic reconnection J. Dahlin University of Maryland J. F. Drake University of Maryland M. Swisdak University of Maryland Astrophysical reconnection Solar and stellar
More informationMechanisms for particle heating in flares
Mechanisms for particle heating in flares J. F. Drake University of Maryland J. T. Dahlin University of Maryland M. Swisdak University of Maryland C. Haggerty University of Delaware M. A. Shay University
More informationVlasov simulations of electron holes driven by particle distributions from PIC reconnection simulations with a guide field
GEOPHYSICAL RESEARCH LETTERS, VOL. 35, L22109, doi:10.1029/2008gl035608, 2008 Vlasov simulations of electron holes driven by particle distributions from PIC reconnection simulations with a guide field
More informationPhysics of Solar Wind and Terrestrial Magnetospheric Plasma Interactions With the Moon
Physics of Solar Wind and Terrestrial Magnetospheric Plasma Interactions With the Moon R.P. Lin Physics Dept & Space Sciences Laboratory University of California, Berkeley with help from J. Halekas, M.
More informationFast Magnetic Reconnection in Fluid Models of (Pair) Plasma
Fast Magnetic Reconnection in Fluid Models of (Pair) Plasma E. Alec Johnson Department of Mathematics, UW-Madison Presented on September 10, 2009, Postdoctoral Research Symposium, Argonne National Laboratories.
More informationREPORT DOCUMENTATION PAGE
REPORT DOCUMENTATION PAGE Form Approved OMB No. 0704-0188 Public reporting burden for this collection of information is estimated to average 1 hour per response, including the time for reviewing instructions,
More informationPHYS 480/580 Introduction to Plasma Physics Fall 2017
PHYS 480/580 Introduction to Plasma Physics Fall 2017 Instructor: Prof. Stephen Bradshaw (302 Herman Brown Hall, ext. 4045) Email: stephen.bradshaw {at} rice.edu Class Website: Owl Space Lectures: Tuesday
More informationDissipation Mechanism in 3D Magnetic Reconnection
Dissipation Mechanism in 3D Magnetic Reconnection Keizo Fujimoto Computational Astrophysics Laboratory, RIKEN Reconnection (in the Earth Magnetosphere) Coroniti [1985] 10 km 10 5 km 10 3 km Can induce
More informationMulti-scale simulation for plasma science
Journal of Physics: Conference Series Multi-scale simulation for plasma science To cite this article: S Ishiguro et al 2010 J. Phys.: Conf. Ser. 257 012026 View the article online for updates and enhancements.
More informationWhat can test particles tell us about magnetic reconnection in the solar corona?
What can test particles tell us about magnetic reconnection in the solar corona? James Threlfall, T. Neukirch, C. E. Parnell, A. W. Hood jwt9@st-andrews.ac.uk @JamesWThrelfall Overview Motivation (solar
More informationThe process of electron acceleration during collisionless magnetic reconnection
PHYSICS OF PLASMAS 13, 01309 006 The process of electron acceleration during collisionless magnetic reconnection X. R. Fu, Q. M. Lu, and S. Wang CAS Key Laboratory of Basic Plasma Physics, School of Earth
More informationFlare particle acceleration in the interaction of twisted coronal flux ropes
Flare particle acceleration in the interaction of twisted coronal flux ropes James Threlfall, A. W. Hood (University of St Andrews) P. K. Browning (University of Manchester) jwt9@st-andrews.ac.uk @JamesWThrelfall
More informationSingle particle motion
Single particle motion Plasma is a collection of a very large number of charged particles moving in, and giving rise to, electromagnetic fields. Before going to the statistical descriptions, let us learn
More informationMHD turbulence in the solar corona and solar wind
MHD turbulence in the solar corona and solar wind Pablo Dmitruk Departamento de Física, FCEN, Universidad de Buenos Aires Turbulence, magnetic reconnection, particle acceleration Understand the mechanisms
More informationJournal of Geophysical Research: Space Physics
RESEARCH ARTICLE Key Points: Electron acceleration (>100 kev) in magnetotail reconnection is due to perpendicular electric field Dependence of the parallel potential on physical parameters is derived Detail
More informationNON-INERTIAL FRAMES IN SPECIAL RELATIVITY
NON-INERTIAL FRAMES IN SPECIAL RELATIVITY A. Blato Creative Commons Attribution 3.0 License (208) Buenos Aires Argentina This article presents a new formulation of special relativity which is invariant
More informationMikhail V. Medvedev (KU)
Students (at KU): Sarah Reynolds, Sriharsha Pothapragada Mikhail V. Medvedev (KU) Collaborators: Anatoly Spitkovsky (Princeton) Luis Silva and the Plasma Simulation Group (Portugal) Ken-Ichi Nishikawa
More informationMagnetic Reconnection in Space Plasmas
Magnetic Reconnection in Space Plasmas Lin-Ni Hau et al. Institute of Space Science Department of Physics National Central University, Taiwan R.O.C. EANAM, 2012.10.31 Contents Introduction Some highlights
More informationPlasma Physics for Astrophysics
- ' ' * ' Plasma Physics for Astrophysics RUSSELL M. KULSRUD PRINCETON UNIVERSITY E;RESS '. ' PRINCETON AND OXFORD,, ', V. List of Figures Foreword by John N. Bahcall Preface Chapter 1. Introduction 1
More informationMagnetic field reconnection is said to involve an ion diffusion region surrounding an
The magnetic field reconnection site and dissipation region by P.L. Pritchett 1 and F.S. Mozer 2 1. Department of Physics and Astronomy, UCLA, Los Angeles, CA 90095-1547 2. Space Sciences Laboratory, University
More informationPlasma spectroscopy when there is magnetic reconnection associated with Rayleigh-Taylor instability in the Caltech spheromak jet experiment
Plasma spectroscopy when there is magnetic reconnection associated with Rayleigh-Taylor instability in the Caltech spheromak jet experiment KB Chai Korea Atomic Energy Research Institute/Caltech Paul M.
More informationPHYS 2135 Exam I February 13, 2018
Exam Total /200 PHYS 2135 Exam I February 13, 2018 Name: Recitation Section: Five multiple choice questions, 8 points each Choose the best or most nearly correct answer For questions 6-9, solutions must
More informationHybrid Simulations: Numerical Details and Current Applications
Hybrid Simulations: Numerical Details and Current Applications Dietmar Krauss-Varban and numerous collaborators Space Sciences Laboratory, UC Berkeley, USA Boulder, 07/25/2008 Content 1. Heliospheric/Space
More informationVerification and Convergence Properties of a Particle-In-Cell Code
Verification and Convergence Properties of a Particle-In-Cell Code B. J. Winjum 1, J. J. Tu 2, S. S. Su 3, V. K. Decyk 1, W. B. Mori 1 1 UCLA 2 Fudan U., China 3 U. Michigan 2014 Anomalous Absorption Conference
More informationFrancesco Califano. Physics Department, University of Pisa. The role of the magnetic field in the interaction of the solar wind with a magnetosphere
Francesco Califano Physics Department, University of Pisa The role of the magnetic field in the interaction of the solar wind with a magnetosphere Collaboration with M. Faganello & F. Pegoraro Vien na,
More informationObservations of Suprathermal Electrons in Mercury s Magnetosphere During the Three MESSENGER Flybys
Observations of Suprathermal Electrons in Mercury s Magnetosphere During the Three MESSENGER Flybys Robert E. Gold, George C. Ho 1, Stamatios M. Krimigis, Richard D. Starr James A. Slavin, Dan N. Baker,
More information3D Reconnection of Weakly Stochastic Magnetic Field and its Implications
3D Reconnection of Weakly Stochastic Magnetic Field and its Implications Alex Lazarian Astronomy Department and Center for Magnetic Self- Organization in Astrophysical and Laboratory Plasmas Collaboration:
More informationmagnetic reconnection as the cause of cosmic ray excess from the heliospheric tail
magnetic reconnection as the cause of cosmic ray excess from the heliospheric tail Paolo Desiati 1,2 & Alexander Lazarian 2 1 IceCube Research Center 2 Department of Astronomy University of Wisconsin -
More informationTHE FRANCK-HERTZ EXPERIMENT
Rice University Physics 332 THE FRANCK-HERTZ EXPERIMENT I. INTRODUCTION... 2 II. THEORETICAL CONSIDERATIONS... 3 III. MEASUREMENT AND ANALYSIS... 5 Revised July 1991 I. Introduction By the early part of
More informationAt a Glance Course Expectations: Grade 8 Physical Science
Power Standard : prioritized academic expectations determined to be the most critical and essential for students to learn. Power Standards will be listed on the report card. : Concise, written descriptions
More information8.2.2 Rudiments of the acceleration of particles
430 The solar wind in the Universe intergalactic magnetic fields that these fields should not perturb them. Their arrival directions should thus point back to their sources in the sky, which does not appear
More informationContinuous, Localized Ion Heating due to Magnetic Reconnection in a Low Aspect Ratio Tokamak
Continuous, Localized Ion Heating due to Magnetic Reconnection in a Low Aspect Ratio Tokamak M. G. Burke, J.L. Barr, M.W. Bongard, R.J. Fonck, E.T. Hinson, J.M. Perry, J.A. Reusch, D.J. Schlossberg EPR
More informationX-ray observations of Solar Flares. Marina Battaglia Fachhochschule Nordwestschweiz (FHNW)
X-ray observations of Solar Flares Marina Battaglia Fachhochschule Nordwestschweiz (FHNW) marina.battaglia@fhnw.ch 2 3 The solar corona Close by astrophysical laboratory allows us to study: Release of
More informationPIC Algorithm with Multiple Poisson Equation Solves During One Time Step
Journal of Physics: Conference Series PAPER OPEN ACCESS PIC Algorithm with Multiple Poisson Equation Solves During One Time Step To cite this article: Junxue Ren et al 2015 J. Phys.: Conf. Ser. 640 012033
More informationDensity cavity in magnetic reconnection diffusion region in the presence of guide field
JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 116,, doi:10.1029/2010ja016324, 2011 Density cavity in magnetic reconnection diffusion region in the presence of guide field M. Zhou, 1,2 Y. Pang, 1,2 X. H. Deng,
More informationBaryon Number Non-Conservation and the Topology of Gauge Fields
FERMILAB-Conf-96/266-A hep-ph/9608456 Baryon Number Non-Conservation and the Topology of Gauge Fields arxiv:hep-ph/9608456v1 27 Aug 1996 Minos Axenides 1,, Andrei Johansen 2,, Holger B. Nielsen 3, and
More informationMagnetic Reconnection: dynamics and particle acceleration J. F. Drake University of Maryland
Magnetic Reconnection: dynamics and particle acceleration J. F. Drake University of Maryland M. Swisdak University of Maryland T. Phan UC Berkeley E. Quatert UC Berkeley R. Lin UC Berkeley S. Lepri U Michican
More informationMagnetic Reconnection
Magnetic Reconnection J. Egedal In collaboration with Joe Olson, Cary Forest and the MPDX team UW-Madison, WI Les Houches, March, 2015 Madison Plasma Dynamo experiment 2 Key new hardware for TREX Cylindrical
More informationSearching for Heavy Photons Using TREK
Searching for Heavy Photons Using TREK Peter Monaghan Hampton University APS April Meeting, Savannah, GA, 7 th April 2014 Searching for Heavy Photons using TREK 1 Search for a Light Gauge Boson, A Astrophysical
More informationHigh Energy Astrophysics: A View on Chemical Enrichment, Outflows & Particle Acceleration. (Feedback at work)
High Energy Astrophysics: A View on Chemical Enrichment, Outflows & Particle Acceleration (Feedback at work) Jacco Vink Utrecht University High Energy Astrophysics HEA aims at understanding the extreme
More informationCombined Science: Trilogy
Co-teaching GCSE Physics and GCSE Combined Science: Trilogy This high level co-teaching guide will help you plan your route through the course. You ll be able to see what common themes and topics span
More informationMagnetic Reconnection: Recent Developments and Future Challenges
Magnetic Reconnection: Recent Developments and Future Challenges A. Bhattacharjee Center for Integrated Computation and Analysis of Reconnection and Turbulence (CICART) Space Science Center, University
More informationFrom billiards to thermodynamics. Renato Feres Washington University Department of Mathematics
From billiards to thermodynamics Renato Feres Washington University Department of Mathematics 1 / 21 Billiards Engraving from Charles Cotton s 1674 book, The Complete Gamester 2 / 21 Math billiards - different
More informationThe Laplace Expansion Theorem: Computing the Determinants and Inverses of Matrices
The Laplace Expansion Theorem: Computing the Determinants and Inverses of Matrices David Eberly, Geometric Tools, Redmond WA 98052 https://www.geometrictools.com/ This work is licensed under the Creative
More informationFavorable conditions for energetic electron acceleration during magnetic reconnection in the Earth s magnetotail
JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 116,, doi:10.1029/2011ja016576, 2011 Favorable conditions for energetic electron acceleration during magnetic reconnection in the Earth s magnetotail S. Imada, 1 M.
More informationDELPHI Collaboration DELPHI PHYS 656. Measurement of mass dierence between? and + and mass of -neutrino from three-prong -decays
DELPHI Collaboration DELPHI 96-167 PHYS 656 2 December, 1996 Measurement of mass dierence between? and + and mass of -neutrino from three-prong -decays M.Chapkin V.Obraztsov IHEP, Protvino Abstract The
More informationCompound Perpendicular Diffusion of Cosmic Rays and Field Line Random Walk, with Drift
Compound Perpendicular Diffusion of Cosmic Rays and Field Line Random Walk, with Drift G.M. Webb, J. A. le Roux, G. P. Zank, E. Kh. Kaghashvili and G. Li Institute of Geophysics and Planetary Physics,
More informationQuizbank/Test. CalcPhysIIT1_Study. From Wikiversity
Quizbank/Test From Wikiversity CalcPhysIIT1_Study If you are reading this as a Wikiversity page, proper pagebreaks should result if printed using your browser's print option. On Chrome, Explorer, and Firefox,
More informationPHY 140A: Solid State Physics. Solution to Homework #7
PHY 14A: Solid State Physics Solution to Homework #7 Xun Jia 1 December 5, 26 1 Email: jiaxun@physics.ucla.edu Fall 26 Physics 14A c Xun Jia (December 5, 26) Problem #1 Static magnetoconductivity tensor.
More informationInterstellar Medium V1
Interstellar Medium V1 Heliosheath Termina/on Shock V2 which can be used to distinguish spatial and temporal effects. The V2 flows derived from the energetic particles using the Compton-Getting effect
More informationRelativistic reconnection at the origin of the Crab gamma-ray flares
Relativistic reconnection at the origin of the Crab gamma-ray flares Benoît Cerutti Center for Integrated Plasma Studies University of Colorado, Boulder, USA Collaborators: Gregory Werner (CIPS), Dmitri
More informationPhysics /09 Released Exam June 2009 Form A Provincial Examination Answer Key
Physics 12 2008/09 Released Exam June 2009 Form A Provincial Examination Answer Key Cognitive Processes K = Knowledge U = Understanding H = Higher Mental Processes Weightings 10% 80% 10% Types 35 = Multiple
More informationReminders: Show your work! As appropriate, include references on your submitted version. Write legibly!
Phys 782 - Computer Simulation of Plasmas Homework # 4 (Project #1) Due Wednesday, October 22, 2014 Reminders: Show your work! As appropriate, include references on your submitted version. Write legibly!
More informationInvestigations of short-term variations of vector and tensor anisotropies of cosmic rays using magnetic mirror model
Investigations of short-term variations of vector and tensor anisotropies of cosmic rays using magnetic mirror model and G.F. Krymsky and P.A. Krivoshapkin Yu.G. Shafer insitute of cosmophysical research
More informationObservation of topological surface state quantum Hall effect in an intrinsic three-dimensional topological insulator
Observation of topological surface state quantum Hall effect in an intrinsic three-dimensional topological insulator Authors: Yang Xu 1,2, Ireneusz Miotkowski 1, Chang Liu 3,4, Jifa Tian 1,2, Hyoungdo
More informationGyrokinetic Simulations of Tearing Instability
Gyrokinetic Simulations of Tearing Instability July 6, 2009 R. NUMATA A,, W. Dorland A, N. F. Loureiro B, B. N. Rogers C, A. A. Schekochihin D, T. Tatsuno A rnumata@umd.edu A) Center for Multiscale Plasma
More informationParsek2D: An Implicit Parallel Particle-in-Cell Code
NUMERICAL MODELING OF SPACE PLASMA FLOWS: ASTRONUM-2008 ASP Conference Series, Vol. 406, c 2009 Nikolai V. Pogorelov, Edouard Audit, Phillip Colella, and Gary P. Zank, eds. Parsek2D: An Implicit Parallel
More informationPhys 102 Lecture 28 Life, the universe, and everything
Phys 102 Lecture 28 Life, the universe, and everything 1 Today we will... Learn about the building blocks of matter & fundamental forces Quarks and leptons Exchange particle ( gauge bosons ) Learn about
More informationGraduate Course Structure for PhD and MS Students Specialization areas and their corresponding courses
Graduate Course Structure for PhD and MS Students Specialization areas and their corresponding courses Note: if you want to use a course not on this list, get approval from your faculty advisor. Specialization:
More informationarxiv:astro-ph/ v1 27 May 2005
2D stationary resistive MHD flows: borderline to magnetic reconnection solutions D.H. Nickeler a,, H.-J. Fahr b arxiv:astro-ph/0505554v1 27 May 2005 a Astronomical Institute, Utrecht University, Princetonplein
More informationWhy study plasma astrophysics?
Why study plasma astrophysics? Nick Murphy and Xuening Bai Harvard-Smithsonian Center for Astrophysics Astronomy 253: Plasma Astrophysics January 25, 2016 Today s plan Definition of a plasma Plasma astrophysics:
More informationRigorous free fermion entanglement renormalization from wavelets
Computational Complexity and High Energy Physics August 1st, 2017 Rigorous free fermion entanglement renormalization from wavelets arxiv: 1707.06243 Jutho Haegeman Ghent University in collaboration with:
More informationElectron heating in shocks and reconnection
Electron heating in shocks and reconnection 11th Plasma Kinetics Working Meeting, Vienna, July 23rd 2018 Lorenzo Sironi (Columbia) with: Xinyi Guo & Michael Rowan (Harvard), Aaron Tran (Columbia) Electron
More informationEXASCALE COMPUTING. Implementation of a 2D Electrostatic Particle in Cell algorithm in UniÞed Parallel C with dynamic load-balancing
ExaScience Lab Intel Labs Europe EXASCALE COMPUTING Implementation of a 2D Electrostatic Particle in Cell algorithm in UniÞed Parallel C with dynamic load-balancing B. Verleye P. Henry R. Wuyts G. Lapenta
More informationA particle-in-cell method with adaptive phase-space remapping for kinetic plasmas
A particle-in-cell method with adaptive phase-space remapping for kinetic plasmas Bei Wang 1 Greg Miller 2 Phil Colella 3 1 Princeton Institute of Computational Science and Engineering Princeton University
More informationStability of strong waves and its implications for pulsar wind shocks
Stability of strong waves and its implications for pulsar wind shocks Iwona Mochol in collaboration with John Kirk Max-Planck-Institut für Kernphysik Heidelberg, Germany Madrid, 22/05/2013 Pulsar winds
More informationCross-Scale: multi-scale coupling in space plasmas
Cross-Scale: multi-scale coupling in space plasmas Steve Schwartz on behalf of the international Cross-Scale community (www.cross-scale.org) including 372 scientists from 23 Countries X supported by Masaki
More informationLecture Outline Chapter 10. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.
Lecture Outline Chapter 10 Physics, 4 th Edition James S. Walker Chapter 10 Rotational Kinematics and Energy Units of Chapter 10 Angular Position, Velocity, and Acceleration Rotational Kinematics Connections
More informationGraduate Course Structure for PhD and MS Students Specialization areas and their corresponding courses
Graduate Course Structure for PhD and MS Students Specialization areas and their corresponding courses Note: if you want to use a course not on this list, get approval from your faculty advisor. Specialization:
More informationQuizbank/Calculus Physics I/T2study
Quizbank/Calculus Physics I/T2study From Wikiversity CalcPhys1T2_Study If you are reading this as a Wikiversity page, proper pagebreaks should result if printed using your browser's print option. On Chrome,
More informationSupporting Information: Ultraintense. femtosecond magnetic nanoprobes induced by. azimuthally polarized laser beams
Supporting Information: Ultraintense femtosecond magnetic nanoprobes induced by azimuthally polarized laser beams Manuel Blanco, Ferran Cambronero, M. Teresa Flores-Arias, Enrique Conejero Jarque, Luis
More informationQuizbank/Calculus Physics I/T3study
Quizbank/Calculus Physics I/T3study From Wikiversity CalcPhys1T3_Study If you are reading this as a Wikiversity page, proper pagebreaks should result if printed using your browser's print option. On Chrome,
More informationElement Abundances and Source Plasma Temperatures of Solar Energetic Particles
15th AIAC: The Science of Ed Stone: Celebrating his 80th Birthday IOP Publishing Journal of Physics: Conference Series 767 (2016) 012023 doi:10.1088/1742-6596/767/1/012023 Element Abundances and Source
More informationDiffusive cosmic ray acceleration at shock waves of arbitrary speed
Diffusive cosmic ray acceleration at shock waves of arbitrary speed Institut für Theoretische Physik, Lehrstuhl IV: Weltraum- und Astrophysik, Ruhr-Universität Bochum, D-4478 Bochum, Germany E-mail: rsch@tp4.rub.de
More informationSimulation of CESR-c Luminosity from Beam Functions
Simulation of CESR-c Luminosity from Beam Functions Abhijit C. Mehta Trinity College, Duke University, Durham, North Carolina, 27708 (Dated: August 13, 2004) It is desirable to have the ability to compute
More informationUnderstanding the pulsar magnetosphere through first-principle simulations
Understanding the pulsar magnetosphere through first-principle simulations Alexander Y. Chen In collaboration with: Andrei Beloborodov Rui Hu The Many Faces of Neutron Stars August 25, 2015 Pulsars: Rotating
More informationA Superfluid Universe
A Superfluid Universe Lecture 2 Quantum field theory & superfluidity Kerson Huang MIT & IAS, NTU Lecture 2. Quantum fields The dynamical vacuum Vacuumscalar field Superfluidity Ginsburg Landau theory BEC
More informationThe fast-ion distribution function
The fast-ion distribution function Source Collisions Orbits RF Losses W. Heidbrink 3 MeV & 14.7 MeV protons Charge Exchange Reactivity σv Complex neutral beam sources are described by a few parameters
More informationSelf-Assembly. Lecture 2 Lecture 2 Models of Self-Assembly
Self-Assembly Lecture 2 Lecture 2 Models of Self-Assembly Models of Self-Assembly The eaim: Solving the engineering ee g problems of self-assembly: forward, backward and the yield. understand the feasibility
More informationSolar-terrestrial relation and space weather. Mateja Dumbović Hvar Observatory, University of Zagreb Croatia
Solar-terrestrial relation and space weather Mateja Dumbović Hvar Observatory, University of Zagreb Croatia Planets Comets Solar wind Interplanetary magnetic field Cosmic rays Satellites Astronauts HELIOSPHERE
More informationForced hybrid-kinetic turbulence in 2D3V
Forced hybrid-kinetic turbulence in 2D3V Silvio Sergio Cerri1,2 1 In collaboration with: 3 F. Califano, F. Rincon, F. Jenko4, D. Told4 1 Physics Department E. Fermi, University of Pisa, Italy fu r Plasmaphysik,
More informationEffect of Surface Topography on the Lunar Electrostatic Environment: 3D Plasma Particle Simulations
Effect of Surface Topography on the Lunar Electrostatic Environment: 3D Plasma Particle Simulations Yohei Miyake and Masaki N Nishino Education Center on Computational Science and Engineering, Kobe University
More informationNUMERICAL STUDY OF NON-THERMAL EMISSION FROM LAGRANGIAN PARTICLES IN AGN ENVIRONMENTS.
13th AGILE Workshop, ASI, Rome May 25, 2015 NUMERICAL STUDY OF NON-THERMAL EMISSION FROM LAGRANGIAN PARTICLES IN AGN ENVIRONMENTS. Dr. Bhargav Vaidya Università degli Studi di Torino, Torino. Collaborators:
More informationParticle-In-Cell, fully kinetic scale modelling of solar radio bursts based on non-gyrotropic and plasma emission mechanisms.
Particle-In-Cell, fully kinetic scale modelling of solar radio bursts based on non-gyrotropic and plasma emission mechanisms David Tsiklauri Queen Mary University of London 9 September, 017 Type III burst
More informationThe Vlasov equation for cold dark matter and gravity
The Vlasov equation for cold dark matter and gravity Alaric Erschfeld Ruprecht-Karls-Universität Heidelberg Master seminar, 25.11.2016 1 / 50 Table of Contents 1 Introduction 2 The Vlasov equation 3 Virial
More informationI. PLATEAU TRANSITION AS CRITICAL POINT. A. Scaling flow diagram
1 I. PLATEAU TRANSITION AS CRITICAL POINT The IQHE plateau transitions are examples of quantum critical points. What sort of theoretical description should we look for? Recall Anton Andreev s lectures,
More informationPick-up Calibration in CESR Beam Position Monitors
Pick-up Calibration in CESR Beam Position Monitors Beau Meredith Department of Physics, Greenville College, Greenville, IL, 62246 (Dated: August 21, 2003) The beam position algorithm presently used in
More informationComparative Planetary Foreshocks: Results from recent studies. Karim Meziane University of New Brunswick
Comparative Planetary Foreshocks: Results from recent studies Karim Meziane University of New Brunswick Outline Motivation Bow shock curvature New results from MAVEN Venus similarity with Earth Quasi-parallel
More informationInsights on Shock Acceleration from Solar Energetic Particles
Insights on Shock Acceleration from Solar Energetic Particles aka Reading Shakespeare letter-by-letter (J. Vink, 04-01-2015) Allan J. Tylka Code 672, NASA Goddard Space Flight Center, Greenbelt, MD 20771
More informationConstructing Potential Energy Diagrams
potential ENERGY diagrams Visual Quantum Mechanics Teaching Guide ACTIVITY 2B Constructing Potential Energy Diagrams Goal In this activity, you will explore energy diagrams for magnets in repulsive configurations.
More informationSelf-consistent particle tracking in a simulation of the entropy mode in a Z pinch
Self-consistent particle tracking in a simulation of the entropy mode in a Z pinch K. Gustafson, I. Broemstrup, D. del-castillo-negrete, W. Dorland and M. Barnes Department of Physics, CSCAMM, University
More information1020 ' (L7) (ii) 3 accept '
Level 7 Physics Questions - Answers 1. (a) (i) Paul James Sylvia accept light accept vibration accept sound answers must be in the correct order all three answers in the correct order are required for
More informationUltrahigh Energy Cosmic Rays propagation I
Ultrahigh Energy Cosmic Rays propagation I Microwave background Energy loss processes for protons: - photoproduction interactions - pair production interactions - adiabatic loss due to the expansion of
More informationTurbulent Magnetic Helicity Transport and the Rapid Growth of Large Scale Magnetic Fields
Turbulent Magnetic Helicity Transport and the Rapid Growth of Large Scale Magnetic Fields Jungyeon Cho Dmitry Shapovalov MWMF Madison, Wisconsin April 2012 The Large Scale Dynamo The accumulation of magnetic
More informationUsing Electron Scattering Superscaling to predict Charge-changing Neutrino Cross Sections in Nuclei
Using Electron Scattering Superscaling to predict Charge-changing Neutrino Cross Sections in Nuclei Maria B. Barbaro University of Torino (Italy) and INFN Maria B. Barbaro NUFACT05, Frascati, June 21-26,
More informationteam Hans Peter Büchler Nicolai Lang Mikhail Lukin Norman Yao Sebastian Huber
title 1 team 2 Hans Peter Büchler Nicolai Lang Mikhail Lukin Norman Yao Sebastian Huber motivation: topological states of matter 3 fermions non-interacting, filled band (single particle physics) topological
More informationPhase Space Tomography of an Electron Beam in a Superconducting RF Linac
Phase Space Tomography of an Electron Beam in a Superconducting RF Linac Tianyi Ge 1, and Jayakar Thangaraj 2, 1 Department of Physics and Astronomy, University of California, Los Angeles, California 90095,
More informationFast ion physics in the C-2U advanced, beam-driven FRC
Fast ion physics in the C-2U advanced, beam-driven FRC Richard Magee for the TAE Team 216 US-Japan Workshop on the Compact Torus August 23, 216! High β FRC embedded in magnetic mirror is a unique fast
More informationParticle-in-cell Simulations of Potential Structure around Electric Solar Wind Sail Tethers
Particle-in-cell Simulations of Potential Structure around Electric Solar Wind Sail Tethers IEPC-2015-298/ISTS-2015-b-298 Presented at Joint Conference of 30th International Symposium on Space Technology
More information