Generation Mechanisms for Low-energy Interstellar Pickup Ions

We present a test-particle simulation describing the interstellar pickup ion (PUI) velocity distribution in the turbulent solar wind (SW). The classical Vasyliunas and Siscoe (V&S) model assumes instantaneous pitch angle scattering that leads to an isotropic distribution in the SW frame, and considers only convection and adiabatic cooling as PUIs propagate in the expanding SW. In this paper, the nearly isotropic PUI transport equation, including the effect of spatial diffusion due to the fluctuating magnetic field, is solved at different heliospheric distances. The creation of PUIs due to the ionization of interstellar neutral hydrogen (H) and charge exchange between SW protons and neutral H are considered separately. The varying SW velocity, density, and temperature with heliocentric distance from a comprehensive fluid model have been incorporated into our simulations. Specifically, we find (1) the spatial diffusion augments adiabatic cooling effects by extending the transport time and distance, which leads to an enhanced production of low-energy PUIs, especially at small heliospheric distances; (2) spatial diffusion is unimportant at large distances (≥15 au), because the particles have had a sufficiently long time to undergo adiabatic cooling; (3) moments of the simulated velocity distribution function are consistent with PUI hydrogen properties measured by the New Horizons’ SW Around Pluto instrument; and (4) the simulated PUI distribution is of potential importance for the PUI measurements to be carried out by IMAP at 1 au.

[1]  G. Zank,et al.  The Pickup Ion-mediated Solar Wind , 2018, The Astrophysical Journal.

[2]  C. Russell,et al.  Interstellar Mapping and Acceleration Probe (IMAP): A New NASA Mission , 2018, Space Science Reviews.

[3]  R. D. Strauss,et al.  A Tractable Estimate for the Dissipation Range Onset Wavenumber Throughout the Heliosphere , 2018 .

[4]  G. Zank,et al.  Influence of the Solar Cycle on Turbulence Properties and Cosmic-Ray Diffusion , 2018 .

[5]  G. Zank,et al.  Cosmic Ray Diffusion Tensor throughout the Heliosphere Derived from a Nearly Incompressible Magnetohydrodynamic Turbulence Model , 2017 .

[6]  H. Weaver,et al.  Interstellar Pickup Ion Observations to 38 au , 2017, 1710.05194.

[7]  A. Shalchi,et al.  Simple Analytical Forms of the Perpendicular Diffusion Coefficient for Two-component Turbulence. III. Damping Model of Dynamical Turbulence , 2017 .

[8]  Qiang Hu,et al.  II. Transport of Nearly Incompressible Magnetohydrodynamic Turbulence from 1 to 75 au , 2017 .

[9]  G. Zank,et al.  Theory and Transport of Nearly Incompressible Magnetohydrodynamic Turbulence , 2017, The Astrophysical Journal.

[10]  G. Zank,et al.  THE TRANSPORT OF LOW-FREQUENCY TURBULENCE IN ASTROPHYSICAL FLOWS. II. SOLUTIONS FOR THE SUPER-ALFVÉNIC SOLAR WIND , 2015 .

[11]  G. Zank,et al.  PICKUP ION MEDIATED PLASMAS. I. BASIC MODEL AND LINEAR WAVES IN THE SOLAR WIND AND LOCAL INTERSTELLAR MEDIUM , 2014 .

[12]  A. Shalchi SIMPLE ANALYTICAL FORMS OF THE PERPENDICULAR DIFFUSION COEFFICIENT FOR TWO-COMPONENT TURBULENCE. II. DYNAMICAL TURBULENCE WITH CONSTANT CORRELATION TIME , 2013 .

[13]  G. Zank Transport Processes in Space Physics and Astrophysics , 2013 .

[14]  W. Matthaeus,et al.  THE TRANSPORT OF LOW-FREQUENCY TURBULENCE IN ASTROPHYSICAL FLOWS. I. GOVERNING EQUATIONS , 2012 .

[15]  A. Shalchi Charged-particle transport in space plasmas: an improved theory for cross-field scattering , 2011 .

[16]  R. D. Strauss,et al.  MODELING THE MODULATION OF GALACTIC AND JOVIAN ELECTRONS BY STOCHASTIC PROCESSES , 2011 .

[17]  A. Shalchi A UNIFIED PARTICLE DIFFUSION THEORY FOR CROSS-FIELD SCATTERING: SUBDIFFUSION, RECOVERY OF DIFFUSION, AND DIFFUSION IN THREE-DIMENSIONAL TURBULENCE , 2010 .

[18]  A. Shalchi,et al.  Nonlinear Guiding Center Theory of Perpendicular Diffusion: Derivation from the Newton-Lorentz Equation , 2008 .

[19]  D. Mccomas,et al.  The Solar Wind Around Pluto (SWAP) Instrument Aboard New Horizons , 2007, 0709.4505.

[20]  J. Richardson,et al.  Turbulent Heating of the Solar Wind by Newborn Interstellar Pickup Protons , 2006 .

[21]  A. Shalchi,et al.  Nonlinear Parallel and Perpendicular Diffusion of Charged Cosmic Rays in Weak Turbulence , 2004 .

[22]  W. Matthaeus,et al.  Nonlinear Collisionless Perpendicular Diffusion of Charged Particles , 2003 .

[23]  W. Matthaeus,et al.  MHD-driven Kinetic Dissipation in the Solar Wind and Corona , 2000 .

[24]  Ming Zhang A Markov Stochastic Process Theory of Cosmic-Ray Modulation , 1999 .

[25]  G. Zank,et al.  Analytic forms of the perpendicular cosmic ray diffusion coefficient for an arbitrary turbulence spectrum and applications on transport of Galactic protons and acceleration at interplanetary shocks , 2009 .

[26]  A. Teufel,et al.  Analytic calculation of the parallel mean free path of heliospheric cosmic rays. II. Dynamical magnetic slab turbulence and random sweeping slab turbulence with finite wave power at small wavenumbers , 2003 .

[27]  John W. Bieber,et al.  Proton and Electron Mean Free Paths: The Palmer Consensus Revisited , 1994 .

[28]  W. Matthaeus,et al.  Nearly incompressible fluids. II - Magnetohydrodynamics, turbulence, and waves , 1993 .

[29]  J. R. Jokipii COSMIC-RAY PROPAGATION. I. CHARGED PARTICLES IN A RANDOM MAGNETIC FIELD. , 1966 .