Abstract:Alpha Magnetic Spectrometer (AMS-02) recently published its lepton spectra measurement. The results show that the positron fraction no longer increases above ∼200 GeV. The aim of this work is to investigate the possibility that the excess of positron fraction is due to pulsars. Nearby known pulsars from the ATNF catalog are considered to be a possible primary positron source of the high energy positrons. We find that the pulsars with age T (0.45−4.5) × 10 5 year and distance d < 0.5 kpc can explain the behavio… Show more
“…This general conclusion has also arrived at by a earlier paper [168]. Another article [169] has done a studied particularly on the pulsar interpretation of the new AMS02 data and found that any of the four pulsars they selected, or the combination of them can do the job. In the case of the multiple pulsars contribution, the positron fraction will show a particular structure at high energies.…”
Section: )supporting
confidence: 58%
“…We can now write down the solutions for the perturbation functions in Mode 1: 169) which will serve as the initial conditions, i.e., the leading term, for the perturbation functions outside the horizon. The solutions to be obtained later that are outside the horizon and valid in the time regime that includes this initial time at the temperature T = 10 9 K will have to be matched with Eqs.…”
Section: )mentioning
confidence: 99%
“…We will state briefly how to obtain the solutions and refer to [221] for details. 169) Substituting the expression of the second equation of Eq. (12.196) for −ψ q into the first equation, we 169) pp 283-284, [221].…”
Section: Long Wavelength -Outside the Horizon (Loh)mentioning
“…This general conclusion has also arrived at by a earlier paper [168]. Another article [169] has done a studied particularly on the pulsar interpretation of the new AMS02 data and found that any of the four pulsars they selected, or the combination of them can do the job. In the case of the multiple pulsars contribution, the positron fraction will show a particular structure at high energies.…”
Section: )supporting
confidence: 58%
“…We can now write down the solutions for the perturbation functions in Mode 1: 169) which will serve as the initial conditions, i.e., the leading term, for the perturbation functions outside the horizon. The solutions to be obtained later that are outside the horizon and valid in the time regime that includes this initial time at the temperature T = 10 9 K will have to be matched with Eqs.…”
Section: )mentioning
confidence: 99%
“…We will state briefly how to obtain the solutions and refer to [221] for details. 169) Substituting the expression of the second equation of Eq. (12.196) for −ψ q into the first equation, we 169) pp 283-284, [221].…”
Section: Long Wavelength -Outside the Horizon (Loh)mentioning
“…The latter scenario is widely adopted by some phenomenological works (Feng & Zhang 2016). It has been proposed also that in addition to the Galactic sources, the local sources may affect the CR spectra due to spectral difference between them (Kawanaka et al 2011).…”
The cosmic ray energy spectra of protons and helium nuclei, which are the most abundant components of cosmic radiation, exhibit a remarkable hardening at energies above one hundred GeV/nucleon. Recent data from AMS-02 confirms this feature with a higher significance. This data challenges the current models of cosmic ray acceleration in Galactic sources and propagation in the Galaxy. Here, we explain the observed break in the spectra of proton and helium nuclei in light of recent advances of cosmic ray diffusion theories in turbulent astrophysical sources as a result of a transition between different cosmic ray diffusion regimes. We reconstruct the observed cosmic ray spectra using the fact that transition from normal diffusion to superdiffusion changes the efficiency of particle acceleration and causes the change in the spectral index. We find that calculated proton and helium spectra match very well with the data.
“…Moreover, the spectra of CR leptons with a softening behavior at ∼0.9 TeV have been measured by DAMPE [19] and HESS [20], and confirmed by CALET [21]. These exciting features have triggered models involving: (i) nearby sources [22]; (ii) pulsars [23][24][25][26][27][28]; or (iii) dark matter [29][30][31][32][33]. These models usually contain at least two free parameters.…”
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