Abstract:We provide a compilation of predictions of the QGSJET-II-04m model for the production of secondary species (photons, neutrinos, electrons, positrons, and antinucleons) that are covering a wide range of energies of the beam particles in proton-proton, proton-nucleus, nucleus-proton, and nucleus-nucleus reactions. The current version of QGSJET-II-04m has an improved treatment of the production of secondary particles at low energies: the parameters of the hadronization procedure have been fine-tuned, based on a n… Show more
“…In general, however, production cross sections calculated for the specific primary and target nuclei should be used, which are provided e.g. by the parametrisation AAfrag [131].…”
We review progress in high-energy cosmic ray physics focusing on recent experimental results and models developed for their interpretation. Emphasis is put on the propagation of charged cosmic rays, covering the whole range from ∼ (20 − 50) GV, i.e. the rigidity when solar modulations can be neglected, up to the highest energies observed. We discuss models aiming to explain the anomalies in Galactic cosmic rays, the knee, and the transition from Galactic to extragalactic cosmic rays.
“…In general, however, production cross sections calculated for the specific primary and target nuclei should be used, which are provided e.g. by the parametrisation AAfrag [131].…”
We review progress in high-energy cosmic ray physics focusing on recent experimental results and models developed for their interpretation. Emphasis is put on the propagation of charged cosmic rays, covering the whole range from ∼ (20 − 50) GV, i.e. the rigidity when solar modulations can be neglected, up to the highest energies observed. We discuss models aiming to explain the anomalies in Galactic cosmic rays, the knee, and the transition from Galactic to extragalactic cosmic rays.
“…Our analysis is mostly sensitive to the low-energy part, so the latter model is only used to get a rough estimate of the theoretical uncertainties in the production cross sections. The secondary positron flux is 10-20% larger with Kachelrieß et al (2019) than with Kamae et al (2006) values.…”
Section: Error Budgetmentioning
confidence: 86%
“…Concerning production cross-section uncertainties, we recall that we use Kamae et al (2006) parametrisation. More recent values exist (Kachelrieß et al 2019) -they are calibrated on more recent collider data and include incident and target species up to Fe -, but they are only valid for incident nucleus energy greater than 4 GeV. Our analysis is mostly sensitive to the low-energy part, so the latter model is only used to get a rough estimate of the theoretical uncertainties in the production cross sections.…”
Context. The vertical diffusive halo size of the Galaxy, L, is a key parameter for dark matter indirect searches. It can be better determined thanks to recent AMS-02 data.Aims. We set constraints on L from Be/B and 10Be/Be data, and we performed a consistency check with positron data. We detail the dependence of Be/B and 10Be/Be on L and forecast on which energy range better data would be helpful for future L improvements.Methods. We used USINE V3.5 for the propagation of nuclei, and e+ were calculated with the pinching method.Results. The current AMS-02 Be/B (∼3% precision) and ACE-CRIS 10Be/Be (∼10% precision) data bring similar and consistent constraints on L. The AMS-02 Be/B data alone constrain L = 5−2+3 kpc at a 68% confidence level (spanning different benchmark transport configurations), a range for which most models do not overproduce positrons. Future experiments need to deliver percent-level accuracy on 10Be/9Be anywhere below 10 GV to further constrain L.Conclusions. Forthcoming AMS-02, HELIX, and PAMELA 10Be/9Be results will further test and possibly tighten the limits derived here. Elemental ratios involving radioactive species with different lifetimes (e.g. Al/Mg and Cl/Ar) are also awaited to provide complementary and robuster constraints.
“…GALPROP calculates production of secondary particles in pp-, pA-, Ap-, AA-interactions. Calculations ofp production and propagation are detailed in Moskalenko et al (2002), , and Kachelriess et al (2015Kachelriess et al ( , 2019. Production of neutral mesons (π 0 , K 0 ,K 0 , etc.…”
Section: Galprop Model For Galactic Cr Propagation and Diffuse Emissionmentioning
confidence: 99%
“…Production of neutral mesons (π 0 , K 0 ,K 0 , etc. ), and secondary e ± is calculated using the formalism by Dermer (1986a,b), as described in , or recent parameterizations by Kamae et al (2006), Kachelrieß & Ostapchenko (2012), Kachelriess et al (2014Kachelriess et al ( , 2019. γ-ray production and synchrotron emission are calculated using the propagated CR distributions, including primary e − , secondary e ± , and for γ-rays -including secondary p from inelastic processes (Strong et al 2004(Strong et al , 2010Porter et al 2008;Orlando & Strong 2013).…”
Section: Galprop Model For Galactic Cr Propagation and Diffuse Emissionmentioning
Local interstellar spectra (LIS) of secondary cosmic ray (CR) nuclei, lithium, beryllium, boron, and partially secondary nitrogen, are derived in the rigidity range from 10 MV to ∼200 TV using the most recent experimental results combined with the state-of-the-art models for CR propagation in the Galaxy and in the heliosphere. The lithium spectrum appears somewhat flatter at high energies compared to other secondary species that may imply a primary lithium component. Two propagation packages, GALPROP and HELMOD, are combined to provide a single framework that is run to reproduce direct measurements of CR species at different modulation levels, and at both polarities of the solar magnetic field. An iterative maximum-likelihood method is developed that uses GALPROP-predicted LIS as input to HELMOD, which provides the modulated spectra for specific time periods of the selected experiments for the model-data comparison. The proposed LIS accommodate the low-energy interstellar spectra measured by Voyager 1, HEAO-3, and ACE/CRIS as well as the high-energy observations by PAMELA, AMS-02, and earlier experiments that are made deep in the heliosphere. The interstellar and heliospheric propagation parameters derived in this study are consistent with our earlier results for propagation of CR protons, helium, carbon, oxygen, antiprotons, and electrons.
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