Data di Pubblicazione:
2022
Abstract:
We report on a ∼5σ detection of polarized 3-6 keV X-ray emission from the supernova remnant Cassiopeia A (Cas A) with the Imaging X-ray Polarimetry Explorer (IXPE). The overall polarization degree of 1.8% ± 0.3% is detected by summing over a large region, assuming circular symmetry for the polarization vectors. The measurements imply an average polarization degree for the synchrotron component of ∼2.5%, and close to 5% for the X-ray synchrotron-dominated forward shock region. These numbers are based on an assessment of the thermal and nonthermal radiation contributions, for which we used a detailed spatial-spectral model based on Chandra X-ray data. A pixel-by-pixel search for polarization provides a few tentative detections from discrete regions at the ∼3σ confidence level. Given the number of pixels, the significance is insufficient to claim a detection for individual pixels, but implies considerable turbulence on scales smaller than the angular resolution. Cas A's X-ray continuum emission is dominated by synchrotron radiation from regions within ≲ 1017 cm of the forward and reverse shocks. We find that (i) the measured polarization angle corresponds to a radially oriented magnetic field, similar to what has been inferred from radio observations; (ii) the X-ray polarization degree is lower than in the radio band (∼5%). Since shock compression should impose a tangential magnetic-field structure, the IXPE results imply that magnetic fields are reoriented within ∼1017 cm of the shock. If the magnetic-field alignment is due to locally enhanced acceleration near quasi-parallel shocks, the preferred X-ray polarization angle suggests a size of 3 × 1016 cm for cells with radial magnetic fields.
Tipologia CRIS:
03A-Articolo su Rivista
Elenco autori:
Vink J.; Prokhorov D.; Ferrazzoli R.; Slane P.; Zhou P.; Asakura K.; Baldini L.; Bucciantini N.; Costa E.; Di Marco A.; Heyl J.; Marin F.; Mizuno T.; Ng C.-Y.; Pesce-Rollins M.; Ramsey B.D.; Rankin J.; Ratheesh A.; Sgro C.; Soffitta P.; Swartz D.A.; Tamagawa T.; Weisskopf M.C.; Yang Y.-J.; Bellazzini R.; Bonino R.; Cavazzuti E.; Costamante L.; Di Lalla N.; Latronico L.; Maldera S.; Manfreda A.; Massaro F.; Mitsuishi I.; Omodei N.; Oppedisano C.; Zane S.; Agudo I.; Antonelli L.A.; Bachetti M.; Baumgartner W.H.; Bianchi S.; Bongiorno S.D.; Brez A.; Capitanio F.; Castellano S.; Ciprini S.; Rosa A.D.; Del Monte E.; Gesu L.D.; Donnarumma I.; Doroshenko V.; Dovciak M.; Ehlert S.R.; Enoto T.; Evangelista Y.; Fabiani S.; Garcia J.A.; Gunji S.; Hayashida K.; Iwakiri W.; Jorstad S.G.; Karas V.; Kitaguchi T.; Kolodziejczak J.J.; Krawczynski H.; La Monaca F.; Liodakis I.; Marinucci A.; Marscher A.P.; Marshall H.L.; Matt G.; Muleri F.; O'Dell S.L.; Papitto A.; Pavlov G.G.; Peirson A.L.; Perri M.; Pilia M.; Possenti A.; Poutanen J.; Puccetti S.; Romani R.W.; Spandre G.; Tavecchio F.; Taverna R.; Tawara Y.; Tennant A.F.; Thomas N.E.; Tombesi F.; Trois A.; Tsygankov S.; Turolla R.; Wu K.; Xie F.
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