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arXiv 2004.03676astro-ph.HE
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Gamma-Ray and X-Ray Observations of the Periodic-Repeater FRB 180916 During Active Phases

M. Tavani, F. Verrecchia, C. Casentini, M. Perri, A. Ursi, L. Pacciani, C. Pittori, A. Bulgarelli, G. Piano, M. Pilia, G. Bernardi, A. Addis, L. A. Antonelli, A… 展开作者

M. Tavani, F. Verrecchia, C. Casentini, M. Perri, A. Ursi, L. Pacciani, C. Pittori, A. Bulgarelli, G. Piano, M. Pilia, G. Bernardi, A. Addis, L. A. Antonelli, A. Argan, L. Baroncelli, P. Caraveo, P. W. Cattaneo, A. Chen, E. Costa, G. Di Persio, I. Donnarumma, Y. Evangelista, M. Feroci, A. Ferrari, V. Fioretti, F. Lazzarotto, F. Longo, A. Morselli, F. Paoletti, N. Parmiggiani, A. Trois, S. Vercellone, G. Naldi, G. Pupillo, G. Bianchi, S. Puccetti

英文摘要:

FRB 180916 is a most intriguing source at 150 Mpc distance capable of producing repeating fast radio bursts with a periodic 16.35 day temporal pattern. We report on the X-ray and $γ$-ray observations of FRB 180916 obtained by AGILE and Swift. We focused on the recurrent 5-day time intervals of active radio bursting and present results obtained on Feb. 3 - 8; Feb. 25; Mar. 5 - 10; Mar. 22 - 28, 2020 during a multiwavelength campaign involving high-energy and radio observations. We also searched for temporal coincidences at millisecond timescales between all known radio bursts of FRB 180916 and X-ray and MeV events detectable by AGILE. We do not detect any simultaneous event or any extended X-ray and $γ$-ray emission on timescales of hours/days/weeks. Our cumulative X-ray (0.3-10 keV) flux upper limit of $5 \times\,10^{-14} \rm \, erg \, cm^{-2} s^{-1}$ (obtained during 5-day active intervals) translates into an isotropic luminosity upper limit of $L_{X,UL} \sim 1.5 \times\, 10^{41} \rm erg \, s^{-1}$. Observations above 100 MeV over a many-year timescale provide an average luminosity upper limit one order of magnitude larger. These results provide the so-far most stringent limits on high-energy emission from FRB 180916 and constrain the dissipation of magnetic energy from a magnetar-like source of radius $R_m$, internal magnetic field $B_m$ and dissipation timescale $τ_d$ to satisfy the relation $R_{m,6}^3 B_{m,16}^2 τ_{d,8}^{-1} \lesssim 1$, where $R_{m,6}$ is $R_m$ in units of $10^6$ cm, $B_{m,16}$ is $B_m$ in units of $10^{16}$ G, and $τ_{d,8}$ in units of $10^8$ s.

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