White Dwarf Pulsars as Possible Cosmic Ray Electron-Positron Factories

We suggest that white dwarf (WD) pulsars can compete with neutron star (NS) pulsars for producing the excesses of cosmic ray electrons/positrons observed by the PAMELA, ATIC/PPB-BETS, Fermi and HESS experiments. A merger of two WDs leads to a rapidly spinning WD with a rotational energy comparable to the NS case. The birth rate is also similar, providing the right energy budget for the cosmic ray electrons/positrons. Applying the NS theory, we suggest that the WD pulsars can in principle produce electrons/positrons up to 10 TeV. In contrast to the NS model, the adiabatic and radiative energy losses of electrons/positrons are negligible since their injection continues after the expansion of the pulsar wind nebula, and hence it is enough that a fraction 1% of WDs are magnetized as observed. The long activity also increases the number of nearby sources, which reduces the Poisson fluctuation in the flux. The WD pulsars could dominate the quickly cooling electrons/positrons above TeV energy as a second spectral bump or even surpass the NS pulsars in the observing energy range 10 GeV - 1 TeV, providing a background for the dark matter signals and a nice target for the future AMS-02, CALET and CTA experiment.Comment: 20 pages, 7 figures and 1 tabl

Shock acceleration of electrons and synchrotron emission from the dynamical ejecta of neutron star mergers

Neutron star mergers (NSMs) eject energetic sub-relativistic dynamical ejecta into the circumbinary media. As analogous to supernovae and supernova remnants, the NSM dynamical ejecta are expected to produce non-thermal emission by electrons accelerated at a shock wave. In this paper, we present expected radio and X-ray signals by this mechanism, taking into account non-linear diffusive shock acceleration (DSA) and magnetic field amplification. We suggest that the NSM has a unique nature as a DSA site, where the seed relativistic electrons are abundantly provided by the decays of r-process elements. The signal is predicted to peak at a few 100 - 1,000 days after the merger, determined by the balance between the decrease of the number of seed electrons and the increase of the dissipated kinetic energy due to the shock expansion. While the resulting flux can ideally reach to the maximum flux expected from near-equipartition, the available kinetic energy dissipation rate of the NSM ejecta limits the detectability of such a signal. It is likely that the radio and X-ray emission are overwhelmed by other mechanisms (e.g., an off-axis jet) for an observer placed to a jet direction (i.e., for GW170817). On the other hand, for an off-axis observer, to be discovered once a number of NSMs are identified, the dynamical ejecta component is predicted to dominate the non-thermal emission. While the detection of this signal is challenging even with near-future facilities, this potentially provides a robust probe of the creation of r-process elements in NSMs.Comment: 7 pages, 7 figures, accepted for publication in The Astrophysical Journa