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arxiv: 1906.11477 · v2 · pith:T4XHQYXRnew · submitted 2019-06-27 · 🌌 astro-ph.HE · astro-ph.SR· hep-ph· physics.space-ph

Numerical modeling of cosmic-ray transport in the heliosphere and interpretation of the proton-to-helium ratio in Solar Cycle 24

Pith reviewed 2026-05-25 14:45 UTC · model grok-4.3

classification 🌌 astro-ph.HE astro-ph.SRhep-phphysics.space-ph
keywords cosmic raysheliospheric transportproton-to-helium ratiodiffusion coefficientsolar modulationsolar cycle 24
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The pith

The time variation of the cosmic-ray proton-to-helium ratio below 3 GV arises from mass-to-charge dependent diffusion during heliospheric transport.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper develops numerical models of cosmic-ray transport through the Milky Way and the heliosphere to connect diffusion properties to the observed evolution of the proton-to-helium ratio over Solar Cycle 24. It shows that the long-term behavior at rigidities below 3 GV follows from a diffusion coefficient that depends on particle mass and charge, producing different modulation for protons and helium nuclei. A sympathetic reader would care because this links measurable ratio changes directly to the physics of particle scattering off solar-wind irregularities rather than to source or galactic effects. The work uses both full numerical solutions and approximate analytical relations to isolate how the rigidity dependence of diffusion shapes the ratio's time profile.

Core claim

Within the transport model the time-dependent proton-to-helium ratio at R < 3 GV is reproduced by a diffusion coefficient whose magnitude scales with particle mass and charge; this scaling causes protons and helium to experience different levels of solar modulation as the heliospheric conditions evolve through the solar cycle, and the resulting ratio pattern matches the AMS monthly data without requiring changes in the interstellar source composition.

What carries the argument

Mass/charge-dependent diffusion coefficient for low-rigidity cosmic rays in the heliosphere, which produces differential modulation between protons and helium nuclei.

If this is right

  • The ratio pattern supplies a direct constraint on the rigidity and mass/charge scaling of the heliospheric diffusion coefficient.
  • Numerical heliospheric models that incorporate this scaling can be used to correct low-rigidity fluxes measured at Earth for solar modulation.
  • Similar ratio measurements for other light nuclei should exhibit the same mass/charge-driven time dependence if the mechanism is correct.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same diffusion scaling may affect the interpretation of other low-rigidity secondary-to-primary ratios during solar maximum and minimum.
  • If the mass/charge dependence is confirmed, it provides a new observable for testing models of cosmic-ray scattering on magnetic turbulence in the inner heliosphere.
  • Extending the model to include charge-sign dependent drifts could predict different ratio behaviors for positive and negative particles in future solar cycles.

Load-bearing premise

The observed time-dependent changes in the proton-to-helium ratio are caused mainly by heliospheric transport rather than by time-varying source composition or galactic propagation.

What would settle it

A data set in which the proton-to-helium ratio at fixed rigidity shows no solar-cycle variation after the source composition is held fixed would falsify the claim.

Figures

Figures reproduced from arXiv: 1906.11477 by Bruna Bertucci, Emanuele Fiandrini, Fernando Bar\~ao, Miguel Orcinha, Nicola Tomassetti.

Figure 1
Figure 1. Figure 1: Calculations of the B/C ratio and CR propagation uncer￾tainties before and after the use of the new data from AMS (Aguilar et al., 2018c). heavy ions data are available at 110-600 MeV/n (Cum￾mings et al., 2016). These data have been collected by Voyager-1 in the period 2012-2016, i.e., while the space￾craft were moving in the interstellar space. Thus they provide direct and valuable constraints to CR propa… view at source ↗
Figure 3
Figure 3. Figure 3: Proton and helium data from AMS and Voyager-1 (Aguilar et al., 2015a,b; Cummings et al., 2016), in comparison with LIS from various works: long-dashed red (Tomassetti et al., 2017), dashed or￾ange (Boschini et al., 2017), dot-dashed black (Corti et al., 2016), dotted blue (Tomassetti, 2017a), dashed pink (Tomassetti et al., 2018), and solid green line (Tomassetti, 2015a, 2017b). propagation in two diffusiv… view at source ↗
Figure 2
Figure 2. Figure 2: (a) Measured and calculated proton and helium LIS’s. [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: Modulated energy spectra from 16 selected epochs. The calculations show the best-fit proton fluxes (pink), the predicted helium [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: (a) Time-series of the best-fit k0-values derived with the AMS proton data at R = 1 − 60 GV (Aguilar et al., 2018a); (b) time profile of the proton flux measured by AMS at R = 2 GV in comparison with calculations, LIS uncertainties and uncertainties from the fit; (c) time profile of the helium flux measured by AMS at R = 2 GV in comparison with best-fit calculations from the proton-driven fits (for K = βR)… view at source ↗
Figure 6
Figure 6. Figure 6: (a) time profiles of the p/He ratio evaluated the at rigidity R = 2.2, 2.5, 2.8, 3.4, 5.1, 7.4, 10.5, 15, and 22 GV (from top to bottom); (b) rigidity dependence of the ratio Γp/He = [p/He]t2 /[p/He]t1 calculated for February 2014 (t1) and May 2017 (t2). absorbed in the fit, i.e., by a proper scaling of the k0-values and the nuisance parameters. The relevant uncertainties in the proton flux are shown by th… view at source ↗
Figure 7
Figure 7. Figure 7: (a) time profiles of the p/He ratio evaluated at rigidity R = 2.2, 2.5, 2.8, 3.4, 5.1, 7.4, 10.5, 15, and 22 GV (from top to bottom); (b) rigidity dependence of the ratio Γp/He = [p/He]t2 /[p/He]t1 calculated for February 2014 (t1) and May 2017 (t2). In both plots, the new data from AMS are compared with convection-diffusion calculations. fluxes Based on such a correlation, one may expect that the p/He rat… view at source ↗
Figure 8
Figure 8. Figure 8: (a) time profiles of the p/He ratio evaluated the rigidity R = 2.2, 2.5, 2.8, 3.4, 5.1, 7.4, 10.5, 15, and 22 GV (from top to bottom); (b) rigidity dependence of the ratio Γp/He = [p/He]t2 /[p/He]t1 calculated for February 2014 (t1) and May 2017 (t2). In both plots, the new data from AMS are compared with the broken line fits. current moves always outward, following the solar wind, the key CDA hypothesis i… view at source ↗
read the original abstract

Thanks to space-borne experiments of cosmic-ray (CR) detection, such as the AMS and PAMELA missions in low-Earth orbit, or the Voyager-1 spacecraft in the interstellar space, a large collection of multi-channel and time-resolved CR data has become available. Recently, the AMS experiment has released new precision data, on the proton and helium fluxes in CRs, measured on monthly basis during its first six years of mission. The AMS data reveal a remarkable long-term behavior in the temporal evolution of the proton-to-helium ratio at rigidity $R = p/Z <$ 3 GV. As we have argued in a recent work, such a behavior may reflect the transport properties of low-rigidity CRs in the inteplanetary space. In particular, it can be caused by mass/charge dependence of the CR diffusion coefficient. In this paper, we present our developments in the numerical modeling of CR transport in the Milky Way and in the heliosphere. Within our model, and with the help of approximated analytical solutions, we describe in details the relations between the properties of CR diffusion and the time-dependent evolution of the proton-to-helium ratio.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The manuscript develops numerical models of cosmic-ray transport in the heliosphere (and Milky Way) and uses them, together with approximated analytical solutions, to interpret the long-term temporal evolution of the proton-to-helium ratio at R < 3 GV reported by AMS during Solar Cycle 24. The central claim is that this behavior is produced by a mass/charge dependence in the heliospheric diffusion coefficient.

Significance. If the central claim is substantiated, the work would show that time-dependent heliospheric modulation with explicit (A/Z) dependence can reproduce observed low-rigidity ratio variations, thereby providing a transport-based explanation that does not require time-varying source composition or galactic propagation changes. This would strengthen the interpretive power of combined numerical-plus-analytical heliospheric models for precision CR data.

major comments (1)
  1. [Sections describing the analytical approximations and their application to the p/He ratio] The central claim requires that the approximated analytical solutions remain accurate when the diffusion coefficient carries explicit mass/charge dependence and the modulation potential varies over the multi-year timescale of Solar Cycle 24. No explicit validation (e.g., direct comparison of analytical vs. full numerical solutions for p and He fluxes under the same (A/Z)-dependent diffusion) is described for the strongly modulated, time-dependent regime.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the detailed and constructive review. The manuscript combines numerical transport modeling with analytical approximations to interpret the AMS proton-to-helium ratio variations. Below we address the single major comment point by point. We agree that additional validation will strengthen the presentation and will incorporate it in the revision.

read point-by-point responses
  1. Referee: [Sections describing the analytical approximations and their application to the p/He ratio] The central claim requires that the approximated analytical solutions remain accurate when the diffusion coefficient carries explicit mass/charge dependence and the modulation potential varies over the multi-year timescale of Solar Cycle 24. No explicit validation (e.g., direct comparison of analytical vs. full numerical solutions for p and He fluxes under the same (A/Z)-dependent diffusion) is described for the strongly modulated, time-dependent regime.

    Authors: We agree that explicit validation of the analytical approximations under simultaneous (A/Z) dependence and time variation of the modulation potential is important for substantiating the central claim. Our analytical solutions are derived from the time-dependent transport equation with a rigidity- and (A/Z)-dependent diffusion coefficient; they were previously cross-checked against the numerical code in the steady-state limit and for (A/Z)-independent cases. However, a direct side-by-side comparison for the full time-dependent, (A/Z)-dependent heliospheric modulation over Solar Cycle 24 is not shown. In the revised manuscript we will add this comparison: we will run the numerical model with the same (A/Z)-dependent diffusion coefficient and time-varying modulation potential used in the analytical treatment, then overlay the resulting proton and helium fluxes (and their ratio) against the analytical predictions at rigidities below 3 GV. This will quantify the accuracy of the approximations in the strongly modulated regime relevant to the AMS data. revision: yes

Circularity Check

1 steps flagged

Central interpretation of p/He ratio evolution relies on self-cited prior argument for (A/Z)-dependent diffusion

specific steps
  1. self citation load bearing [Abstract]
    "As we have argued in a recent work, such a behavior may reflect the transport properties of low-rigidity CRs in the inteplanetary space. In particular, it can be caused by mass/charge dependence of the CR diffusion coefficient. In this paper, we present our developments in the numerical modeling of CR transport in the Milky Way and in the heliosphere. Within our model, and with the help of approximated analytical solutions, we describe in details the relations between the properties of CR diffusion and the time-dependent evolution of the proton-to-helium ratio."

    The paper states that the observed ratio evolution 'can be caused by mass/charge dependence' and then uses its numerical/analytical framework to 'describe the relations' between that dependence and the ratio. The justification for invoking the dependence at all is the self-citation ('as we have argued in a recent work'), with no independent derivation or external validation supplied here. The central interpretive claim therefore reduces to the prior paper's conclusion rather than emerging from the present model's first-principles transport equations.

full rationale

The paper's core claim attributes the long-term p/He ratio behavior at R<3 GV to mass/charge-dependent heliospheric diffusion. This attribution is introduced via explicit self-citation to the authors' recent work rather than derived from the numerical model or external constraints within this manuscript. The numerical modeling and analytical approximations are then used to relate diffusion properties to the ratio evolution, but the load-bearing premise (that the dependence exists and drives the observation) traces directly to the self-citation. This creates partial circularity because the interpretation reduces to re-describing the same dataset under an assumption justified only by prior work from the same group. No machine-checked theorem, parameter-free external benchmark, or independent falsification is shown for the (A/Z) dependence itself.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the assumption that the diffusion coefficient carries an explicit mass-to-charge dependence whose functional form is chosen to reproduce the AMS ratio time series; no independent evidence for that functional form is supplied in the abstract.

free parameters (1)
  • mass/charge scaling exponent in diffusion coefficient
    The dependence is introduced to match the observed ratio evolution and is therefore fitted rather than derived from first principles.
axioms (1)
  • domain assumption Heliospheric transport dominates the time variation of the low-rigidity p/He ratio
    Invoked in the abstract to attribute the AMS pattern to diffusion properties rather than galactic or source effects.

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Reference graph

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