2024A&A...690A.219P


Query : 2024A&A...690A.219P

2024A&A...690A.219P - Astronomy and Astrophysics, volume 690A219 (2024/10-1)

The Northern Cross Fast Radio Burst project IV. Multi-wavelength study of the actively repeating FRB 20220912A.

PELLICIARI D., BERNARDI G., PILIA M., NALDI G., MACCAFERRI G., VERRECCHIA F., CASENTINI C., PERRI M., KIRSTEN F., BIANCHI G., BORTOLOTTI C., BRUNO L., DALLACASA D., ESPOSITO P., GEMINARDI A., GIARRATANA S., GIROLETTI M., LULLI R., MACCAFERRI A., MAGRO A., MATTANA A., PERINI F., PUPILLO G., ROMA M., SCHIAFFINO M., SETTI G., TAVANI M., TRUDU M. and ZANICHELLI A.

Abstract (from CDS):

Context. Fast radio bursts (FRBs) are energetic, millisecond-duration radio pulses observed at extragalactic distances and whose origins are still a subject of heated debate. A fraction of the FRB population have shown repeating bursts, however it's still unclear whether these represent a distinct class of sources.
Aims. We investigated the bursting behaviour of FRB 20220912A, one of the most active repeating FRBs known thus far. In particular, we focused on its burst energy distribution, linked to the source energetics, and its emission spectrum, with the latter directly related to the underlying emission mechanism.
Methods. We monitored FRB 20220912A at 408 MHz with the Northern Cross radio telescope and at 1.4 GHz using the 32-m Medicina Grueff radio telescope. Additionally, we conducted 1.2 GHz observations taken with the upgraded Giant Meter Wave Radio Telescope (uGMRT) searching for a persistent radio source coincident with FRB 20220912A, and included high energy observations in the 0.3-10 keV, 0.4-100 MeV and 0.03-30 GeV energy range.
Results. We report 16 new bursts from FRB 20220912A at 408 MHz during the period between October 16th 2022 and December 31st 2023. Their cumulative spectral energy distribution follows a power law with slope αE = -1.3 ± 0.2 and we measured a repetition rate of 0.19 ± 0.03 hr–1 for bursts having a fluence of ℱ ≥ 17 Jy ms. Furthermore, we report no detections at 1.4 GHz for ℱ ≥ 20 Jy ms. These non-detections imply an upper limit of β < -2.3, with β being the 408 MHz - 1.4 GHz spectral index of FRB 20220912A. This is inconsistent with positive β values found for the only two known cases in which an FRB has been detected in separate spectral bands. We find that FRB 20220912A shows a decline of four orders of magnitude in its bursting activity at 1.4 GHz over a timescale of one year, while remaining active at 408 MHz. The cumulative spectral energy distribution (SED) shows a flattening for spectral energy Eν ≥ 1031 erg Hz–1, a feature seen thus far in only two hyperactive repeaters. In particular, we highlight a strong similarity between FRB 20220912A and FRB 20201124A, with respect to both the energy and repetition rate ranges. We also find a radio continuum source with 240 ± 36 μJy flux density at 1.2 GHz, centered on the FRB 20220912A coordinates. Finally, we place an upper limit on the γ to radio burst efficiency η to be η < 1.5 × 109 at 99.7% confidence level, in the 0.4-30 MeV energy range.
Conclusions. The strong similarity between the cumulative energy distributions of FRB 20220912A and FRB 20201124A indicate that bursts from these sources are generated via similar emission mechanisms. Our upper limit on β suggests that the spectrum of FRB 20220912A is intrinsically narrow-band. The radio continuum source detected at 1.2 GHz is likely due to a star formation environment surrounding the FRB, given the absence of a source compact on millisecond scales brighter than 48 μJy beam–1. Finally, the upper limit on the ratio between the γ and radio burst fluence disfavours a giant flare origin for the radio bursts unlike observed for the Galactic magnetar SGR 1806-20.

Abstract Copyright: © The Authors 2024

Journal keyword(s): methods: data analysis - methods: observational - stars: magnetars - radio continuum: galaxies

Simbad objects: 17

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Number of rows : 17
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
2 FRB 20180916B rB 01 58 00.750 +65 43 00.30           ~ 457 0
3 PSR B0329+54 Psr 03 32 59.3370698592 +54 34 45.028206408           ~ 690 1
4 FRB 20201124A rB 05 07 57.600 +26 11 24.00           ~ 307 0
5 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
6 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
7 PSR J1550-5418 Psr 15 50 54.18 -54 18 23.9           ~ 463 1
8 FRB 20190520B rB 16 02 04.270 -11 17 17.32           ~ 211 0
9 PSR J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1316 2
10 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 532 0
11 SWIFT J1818.0-1607 N* 18 18 00.23 -16 07 53.0           ~ 109 0
12 NAME Sgr 1935+2154 * 19 34 55.68 +21 53 48.2           ~ 820 1
13 FRB 200428 rB 19 35.0 +21 57           ~ 291 0
14 PSO J347.2702+48.7066 G 23 09 04.8 +48 42 24           ~ 10 0
15 FRB 20220912A rB 23 09 04.9 +48 42 25           ~ 126 0
16 APTF J230904+484222 Rad 23 09 04.92476882235 +48 42 22.3185074825           ~ 2 0
17 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1

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