2016
DOI: 10.1088/1475-7516/2016/04/010
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IceCube constraints on fast-spinning pulsars as high-energy neutrino sources

Abstract: Abstract. Relativistic winds of fast-spinning pulsars have been proposed as a potential site for cosmic-ray acceleration from very high energies (VHE) to ultrahigh energies (UHE). We re-examine conditions for high-energy neutrino production, considering the interaction of accelerated particles with baryons of the expanding supernova ejecta and the radiation fields in the wind nebula. We make use of the current IceCube sensitivity in diffusive highenergy neutrino background, in order to constrain the parameter … Show more

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Cited by 26 publications
(21 citation statements)
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“…This is because for UHECRs crossing the supernova ejecta surrounding neutron stars, the effective optical depth to hadronic interactions is larger than unity, and so even in the most pessimistic case we expect fluxes of neutrinos in the energy range 10 8 E ν /GeV 10 9 [100]. Indeed, upper limits on the diffuse neutrino flux from IceCube [101,102] and the Pierre Auger Observatory [103] already constrain models of UHECR acceleration in the core of starburst galaxies [104,105]. Note, however, that if highenergy cosmic rays are re-accelerated to ultrahigh energies at the terminal shock of the starburst superwind, we expect the neutrino emission from starbursts to cutoff somewhat above 10 7 GeV, as entertained in [106].…”
mentioning
confidence: 99%
“…This is because for UHECRs crossing the supernova ejecta surrounding neutron stars, the effective optical depth to hadronic interactions is larger than unity, and so even in the most pessimistic case we expect fluxes of neutrinos in the energy range 10 8 E ν /GeV 10 9 [100]. Indeed, upper limits on the diffuse neutrino flux from IceCube [101,102] and the Pierre Auger Observatory [103] already constrain models of UHECR acceleration in the core of starburst galaxies [104,105]. Note, however, that if highenergy cosmic rays are re-accelerated to ultrahigh energies at the terminal shock of the starburst superwind, we expect the neutrino emission from starbursts to cutoff somewhat above 10 7 GeV, as entertained in [106].…”
mentioning
confidence: 99%
“…Furthermore, we assume that 0.2 of the energy of a given UHECR can be converted to the energy of a pion, and 0.25 of the pion energy then goes into the neutrino (as was done in Fang et al 2016). This provides us with an overall conversion factor ofñ f 0.05 from a given UHECR to a neutrino.…”
Section: Constraints From High-energy Neutrinosmentioning
confidence: 99%
“…Thus, for the same reason that we are able to efficiently produce UHECRs, we are also able to not overproduce high-energy neutrinos. We note that there may also be photo-hadronic interactions within the nebula that may also produce neutrinos (Lemoine et al 2015;Fang et al 2016). Since this process is stronger for protons than heavy nuclei, and since our main focus here is on the heavy nuclei as UHECRs, we save such a calculation for future work where the spectra of UHECRs and the non-thermal radiation is computed in more detail.…”
Section: Constraints From High-energy Neutrinosmentioning
confidence: 99%
“…Furthermore, we assume that 0.2 of the energy of a given UHECR can be converted to the energy of a pion, and 0.25 of the pion energy then goes into the neutrino (as was done in Fang et al 2016). This gives an overall conversion factor of f ν ∼ 0.05 from a given UHECR to a neutrino.…”
Section: Intergalactic Propagationmentioning
confidence: 99%