A multi-wavelength investigation of PSR J2229+6114 and its pulsar wind nebula in the radio, X-ray, and gamma-ray bands
G106.3$+$2.7, commonly considered a composite supernova remnant (SNR), is characterized by a boomerang-shaped pulsar wind nebula (PWN) and two distinct ("head" & "tail") regions in the radio band. A discovery of very-high-energy (VHE) gamma-ray emission ($E_\gamma > 100$ G...
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Format | Journal Article |
Language | English |
Published |
06.10.2023
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Subjects | |
Online Access | Get full text |
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Summary: | G106.3$+$2.7, commonly considered a composite supernova remnant (SNR), is
characterized by a boomerang-shaped pulsar wind nebula (PWN) and two distinct
("head" & "tail") regions in the radio band. A discovery of very-high-energy
(VHE) gamma-ray emission ($E_\gamma > 100$ GeV) followed by the recent
detection of ultra-high-energy (UHE) gamma-ray emission ($E_\gamma > 100$ TeV)
from the tail region suggests that G106.3$+$2.7 is a PeVatron candidate. We
present a comprehensive multi-wavelength study of the Boomerang PWN (100"
around PSR J2229+6114) using archival radio and Chandra data obtained from two
decades ago, a new NuSTAR X-ray observation from 2020, and upper limits on
gamma-ray fluxes obtained by Fermi and VERITAS observatories. The NuSTAR
observation allowed us to detect a 51.67 ms spin period from the pulsar PSR
J2229+6114 and the PWN emission characterized by a power-law model with $\Gamma
= 1.52\pm0.06$ up to 20 keV. Contrary to the previous radio study by Kothes et
al. 2006, we prefer a much lower PWN B-field ($B\sim3$ $\mu$G) and larger
distance ($d \sim 8$ kpc) based on (1) the non-varying X-ray flux over the last
two decades, (2) the energy-dependent X-ray PWN size resulting from synchrotron
burn-off and (3) the multi-wavelength spectral energy distribution (SED) data.
Our SED model suggests that the PWN is currently re-expanding after being
compressed by the SNR reverse shock $\sim 1000$ years ago. In this case, the
head region should be formed by GeV--TeV electrons injected earlier by the
pulsar propagating into the low density environment. |
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DOI: | 10.48550/arxiv.2310.04512 |