Table of Contents
Fetching ...

Spectrum of cosmic-ray nucleons and the atmospheric muon charge ratio

Thomas K. Gaisser

TL;DR

This work links the TeV muon charge ratio to the composition of the primary cosmic-ray nucleons and to the forward production of π± and K± in the atmosphere by employing spectrum-weighted moments Z. It combines a three-component, rigidity-based model of the nucleon spectrum with detailed pion and kaon decay physics, including associated kaon production, to predict μ⁺/μ⁻ and νμ/ν̄μ fluxes. By comparing to multiple experimental datasets, it constrains the kaon production contribution (Z_{pK^+} ≈ 0.0079) and derives a kaon-to-pion ratio around 0.135, highlighting the non-negligible role of kaons at TeV energies. The findings have direct implications for atmospheric neutrino fluxes at high energy and demonstrate sensitivity to primary composition and forward hadroproduction.

Abstract

Interpretation of measurements of the muon charge ratio in the TeV range depends on the spectra of protons and neutrons in the primary cosmic radiation and on the inclusive cross sections for production of $π^\pm$ and $K^\pm$ in the atmosphere. Recent measurements of the spectra of cosmic-ray nuclei are used here to estimate separately the energy spectra of protons and neutrons and hence to calculate the charge separated hadronic cascade in the atmosphere. From the corresponding production spectra of $μ^+$ and $μ^-$ the $μ^+/μ^-$ ratio is calculated and compared to recent measurements. The comparison leads to a determination of the relative contribution of kaons and pions. Implications for the spectra of $ν_μ$ and $\barν_μ$ are discussed.

Spectrum of cosmic-ray nucleons and the atmospheric muon charge ratio

TL;DR

This work links the TeV muon charge ratio to the composition of the primary cosmic-ray nucleons and to the forward production of π± and K± in the atmosphere by employing spectrum-weighted moments Z. It combines a three-component, rigidity-based model of the nucleon spectrum with detailed pion and kaon decay physics, including associated kaon production, to predict μ⁺/μ⁻ and νμ/ν̄μ fluxes. By comparing to multiple experimental datasets, it constrains the kaon production contribution (Z_{pK^+} ≈ 0.0079) and derives a kaon-to-pion ratio around 0.135, highlighting the non-negligible role of kaons at TeV energies. The findings have direct implications for atmospheric neutrino fluxes at high energy and demonstrate sensitivity to primary composition and forward hadroproduction.

Abstract

Interpretation of measurements of the muon charge ratio in the TeV range depends on the spectra of protons and neutrons in the primary cosmic radiation and on the inclusive cross sections for production of and in the atmosphere. Recent measurements of the spectra of cosmic-ray nuclei are used here to estimate separately the energy spectra of protons and neutrons and hence to calculate the charge separated hadronic cascade in the atmosphere. From the corresponding production spectra of and the ratio is calculated and compared to recent measurements. The comparison leads to a determination of the relative contribution of kaons and pions. Implications for the spectra of and are discussed.

Paper Structure

This paper contains 7 sections, 30 equations, 5 figures, 1 table.

Figures (5)

  • Figure 1: Left: three-population model of the cosmic-ray spectrum from Eq. \ref{['ModelH3']} compared to data GrigorovAkenoMSUAntoniHEGRACasaMiaTibetKGAGASAHiResAuger. The extra-galactic population in this model has a mixed composition. Right: Corresponding fluxes of nucleons compared to an $E^{-2.7}$ differential spectrum of nucleons and to the all nucleon flux implied by the Polygonato model (galactic component only) Polygonato.
  • Figure 2: Solid line: charge ratio parameter $\delta_0$ for the model with parameters of Table \ref{['tab1']}. Dashed line: same for Polygonato model Polygonato.
  • Figure 3: Muon charge ratio compared to data of CMS CMS and L3-C L3C below 1 TeV and to MINOS MINOScharge at higher energy. The L3-C data plotted here are averaged over $0.9\le\cos(\theta)\le 1.0$ for comparison with the calculation for vertical muons. See text for a description of the lines.
  • Figure 4: Muon charge ratio compared to data of CMS CMS, OPERA OPERA and MINOS Schreiner. Measurements from the near detector of MINOS Jeff and from Park City Utah.
  • Figure 5: ratio of $\nu_\mu/\bar{\nu}_\mu$ calculated with the same parameters as for the charge ration of muons. The dashed line shows the results with parameters of the Polygonato model Polygonato.