Abstract

A precision measurement of the nitrogen flux with rigidity (momentum per unit charge) from 2.2GV to 3.3 TV based on 2.2×10^{6} events is presented. The detailed rigidity dependence of the nitrogen flux spectral index is presented for the first time. The spectral index rapidly hardens at high rigidities and becomes identical to the spectral indices of primary He, C, and O cosmic rays above ∼700 GV. We observed that the nitrogen flux Φ_{N} can be presented as the sum of its primary component Φ_{N}^{P} and secondary component Φ_{N}^{S}, Φ_{N}=Φ_{N}^{P}+Φ_{N}^{S}, and we found Φ_{N} is well described by the weighted sum of the oxygen flux Φ_{O} (primary cosmic rays) and the boron flux Φ_{B} (secondary cosmic rays), with Φ_{N}^{P}=(0.090±0.002)×Φ_{O} and Φ_{N}^{S}=(0.62±0.02)×Φ_{B} over the entire rigidity range. This corresponds to a change of the contribution of the secondary cosmic ray component in the nitrogen flux from 70% at a few GV to <30% above 1TV.

Highlights

  • from 2.2 GV to 3.3 TV based on 2.2 × 106 events is presented

  • The detailed rigidity dependence of the nitrogen flux spectral index is presented for the first time

  • The spectral index rapidly hardens at high rigidities

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Summary

Published by the American Physical Society

We observed that the nitrogen flux ΦN can be presented as the sum of its primary component ΦPN and secondary component ΦSN, ΦN 1⁄4 ΦPN þ ΦSN, and we found ΦN is well described by the weighted sum of the oxygen flux ΦO (primary cosmic rays) and the boron flux ΦB (secondary cosmic rays), with ΦPN 1⁄4 ð0.090 Æ 0.002Þ × ΦO and ΦSN 1⁄4 ð0.62 Æ 0.02Þ × ΦB over the entire rigidity range. In this Letter we report the precision measurement of the nitrogen flux in cosmic rays in the rigidity range from 2.2 GV to 3.3 TV based on data collected by the AMS during the first five years (May 19, 2011 to May 26, 2016) of operation aboard the International Space Station (ISS). The charge confusion from noninteracting nuclei (a)

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