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Pulsar Wind Nebulae as a Source of Cosmic-Ray Electrons and Positrons

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Modelling Pulsar Wind Nebulae

Part of the book series: Astrophysics and Space Science Library ((ASSL,volume 446))

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Abstract

Cosmic-ray electron positron (e ±) observations by PAMELA, H.E.S.S, Fermi and AMS-02 have reported possible excesses of the fluxes with respect to the standard theoretical prediction in an energy range of from a few 10–100 GeV. Pulsar wind nebulae (PWNe) are a promising source of the excesses; multi-wavelength observations of PWNe have shown that e ±s are accelerated up to PeV energies in situ and the inferred acceleration rate can be sufficient to provide the observed e ± flux. An uncertain point of this scenario is whether, how and when the accelerated e ±s can escape PWNe, which is also the key question for understanding the PWN physics.

In this chapter, we first review the classical model of cosmic-ray e ±s and the observational history. Possible origins of the e ± excess are generally discussed. Then, focusing on the PWN model, we consider the minimum requirements to be an e ± source and the observational signatures. We show that O(100) of pulsars with age of < 107 yrs and within a few kpc from the Earth or the nearby Geminga and Mongem pulsars alone can explain the observed e ± excess. On the other hand, the young nearby Vela pulsar can contribute to e ± cosmic rays with multiple-TeV energies. We discuss future prospects for testing the PWN scenarios and e ± escape from the PWNe with using CALET, DAMPE, and CTA.

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Notes

  1. 1.

    More precisely, electrons are less abundant than positrons due to the charge conservation.

  2. 2.

    http://galprop.stanford.edu/.

  3. 3.

    ATIC/PPB-BETS (Chang et al. 2008; Torii et al. 2008) suggest an sharp excess of the e ± with a peak at 600 GeV, which is controversial to the results of Fermi/H.E.S.S/AMS-02 are controversial. We note that the statistical errors of ATIC are much larger than those of Fermi (Israel 2010) and so on.

  4. 4.

    In order to explain the e ± excess, the annihilation cross section of the DM particle generally needs to be ∼ 100–1000 times larger than the thermal relic value by some unknown resonant processes.

  5. 5.

    Note that \(\mathcal{R}_{\mathrm{NS}}\) can be an order-of-magnitude higher in a starburst phase.

  6. 6.

    http://www.atnf.csiro.au/people/pulsar/psrcat/.

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Acknowledgements

The author thank Norita Kawanaka and Kohta Murase for discussion. KK is supported by JST CREST and NASA through Einstein Postdoctoral Fellowship grant number PF4-150123 awarded by the Chandra X-ray Center, which is operated by the Smithsonian Astrophysical Observatory for NASA under contract NAS8-03060.

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Correspondence to Kazumi Kashiyama .

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Kashiyama, K. (2017). Pulsar Wind Nebulae as a Source of Cosmic-Ray Electrons and Positrons. In: Torres, D. (eds) Modelling Pulsar Wind Nebulae. Astrophysics and Space Science Library, vol 446. Springer, Cham. https://doi.org/10.1007/978-3-319-63031-1_12

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