First predicted cosmic ray spectra, primary-to-secondary ratios, and ionization rates from MHD galaxy formation simulations

Author:

Hopkins Philip F1ORCID,Butsky Iryna S12,Panopoulou Georgia V1ORCID,Ji Suoqing1ORCID,Quataert Eliot3ORCID,Faucher-Giguère Claude-André4ORCID,Kereš Dušan5

Affiliation:

1. TAPIR, California Institute of Technology , Mailcode 350-17, Pasadena, CA 91125, USA

2. Astronomy Department, University of Washington , Seattle, WA 98195, USA

3. Department of Astrophysical Sciences, Princeton University , Peyton Hall, Princeton, NJ 08544, USA

4. Department of Physics and Astronomy and CIERA, Northwestern University , 2145 Sheridan Road, Evanston, IL 60208, USA

5. Department of Physics, Center for Astrophysics and Space Science, University of California at San Diego , 9500 Gilman Drive, La Jolla, CA 92093, USA

Abstract

ABSTRACT We present the first simulations evolving resolved spectra of cosmic rays (CRs) from MeV–TeV energies (including electrons, positrons, (anti)protons, and heavier nuclei), in live kinetic-magnetohydrodynamics galaxy simulations with star formation and feedback. We utilize new numerical methods including terms often neglected in historical models, comparing Milky Way analogues with phenomenological scattering coefficients ν to Solar-neighbourhood [Local interstellar medium (LISM)] observations (spectra, B/C, e+/e−, $\mathrm{\bar{p}}/\mathrm{p}$, 10Be/9Be, ionization, and γ-rays). We show it is possible to reproduce observations with simple single-power-law injection and scattering coefficients (scaling with rigidity R), similar to previous (non-dynamical) calculations. We also find: (1) The circumgalactic medium in realistic galaxies necessarily imposes an $\sim 10\,$ kpc CR scattering halo, influencing the required ν(R). (2) Increasing the normalization of ν(R) re-normalizes CR secondary spectra but also changes primary spectral slopes, owing to source distribution and loss effects. (3) Diffusive/turbulent reacceleration is unimportant and generally sub-dominant to gyroresonant/streaming losses, which are sub-dominant to adiabatic/convective terms dominated by $\sim 0.1-1\,$ kpc turbulent/fountain motions. (4) CR spectra vary considerably across galaxies; certain features can arise from local structure rather than transport physics. (5) Systematic variation in CR ionization rates between LISM and molecular clouds (or Galactic position) arises naturally without invoking alternative sources. (6) Abundances of CNO nuclei require most CR acceleration occurs around when reverse shocks form in SNe, not in OB wind bubbles or later Sedov–Taylor stages of SNe remnants.

Funder

NSF

NASA

STScI

Research Corporation for Science Advancement

Simons Foundation

Space Telescope Science Institute

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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1. Synchrotron emission on FIRE: equipartition estimators of magnetic fields in simulated galaxies with spectrally resolved cosmic rays;Monthly Notices of the Royal Astronomical Society;2023-12-23

2. Cosmic ray feedback in galaxies and galaxy clusters;The Astronomy and Astrophysics Review;2023-12

3. On the impact of runaway stars on dwarf galaxies with resolved interstellar medium;Monthly Notices of the Royal Astronomical Society;2023-09-12

4. Cosmic ray transport in large-amplitude turbulence with small-scale field reversals;Monthly Notices of the Royal Astronomical Society;2023-09-01

5. Cosmic Ray Processes in Galactic Ecosystems;Galaxies;2023-07-16

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