Highly Significant Detection of X-Ray Polarization from the Brightest Accreting Neutron Star Sco X-1
Monaca FL; Marco AD; Poutanen J; Bachetti M; Motta SE; Papitto A; Pilia M; Xie F; Bianchi S; Bobrikova A; Costa E; Deng W; Ge M; Illiano G; Jia S; Krawczynski H; Lai EV; Liu K; Mastroserio G; Muleri F; Rankin J; Soffitta P; Veledina A; Ambrosino F; Santo MD; Chen W; Garcia JA; Kaaret P; Russell TD; Wei W; Zhang S; Zuo C; Arzoumanian Z; Cocchi M; Gnarini A; Farinelli R; Gendreau K; Ursini F; Weisskopf MC; Zane S; Agudo I; Antonelli LA; Baldini L; Baumgartner WH; Bellazzini R; Bongiorno SD; Bonino R; Brez A; Bucciantini N; Capitanio F; Castellano S; Cavazzuti E; Chen C; Ciprini S; Rosa AD; Monte ED; Gesu LD; Lalla ND; Donnarumma I; Doroshenko V; Dovčiak M; Ehlert SR; Enoto T; Evangelista Y; Fabiani S; Ferrazzoli R; Gunji S; Hayashida K; Heyl J; Iwakiri W; Jorstad SG; Karas V; Kislat F; Kitaguchi T; Kolodziejczak JJ; Latronico L; Liodakis I; Maldera S; Manfreda A; Marin F; Marinucci A; Marscher AP; Marshall HL; Massaro F; Matt G; Mitsuishi I; Mizuno T; Negro M; Ng C; O’Dell SL; Omodei N; Oppedisano C; Pavlov GG; Peirson AL; Perri M; Pesce-Rollins M; Petrucci P; Possenti A; Puccetti S; Ramsey BD; Ratheesh A; Roberts OJ; Romani RW; Sgrò C; Slane P; Spandre G; Swartz DA; Tamagawa T; Tavecchio F; Taverna R; Tawara Y; Tennant AF; Thomas NE; Tombesi F; Trois A; Tsygankov SS; Turolla R; Vink J; Wu K; IXPE Collaboration
Highly Significant Detection of X-Ray Polarization from the Brightest Accreting Neutron Star Sco X-1
Monaca FL
Marco AD
Poutanen J
Bachetti M
Motta SE
Papitto A
Pilia M
Xie F
Bianchi S
Bobrikova A
Costa E
Deng W
Ge M
Illiano G
Jia S
Krawczynski H
Lai EV
Liu K
Mastroserio G
Muleri F
Rankin J
Soffitta P
Veledina A
Ambrosino F
Santo MD
Chen W
Garcia JA
Kaaret P
Russell TD
Wei W
Zhang S
Zuo C
Arzoumanian Z
Cocchi M
Gnarini A
Farinelli R
Gendreau K
Ursini F
Weisskopf MC
Zane S
Agudo I
Antonelli LA
Baldini L
Baumgartner WH
Bellazzini R
Bongiorno SD
Bonino R
Brez A
Bucciantini N
Capitanio F
Castellano S
Cavazzuti E
Chen C
Ciprini S
Rosa AD
Monte ED
Gesu LD
Lalla ND
Donnarumma I
Doroshenko V
Dovčiak M
Ehlert SR
Enoto T
Evangelista Y
Fabiani S
Ferrazzoli R
Gunji S
Hayashida K
Heyl J
Iwakiri W
Jorstad SG
Karas V
Kislat F
Kitaguchi T
Kolodziejczak JJ
Latronico L
Liodakis I
Maldera S
Manfreda A
Marin F
Marinucci A
Marscher AP
Marshall HL
Massaro F
Matt G
Mitsuishi I
Mizuno T
Negro M
Ng C
O’Dell SL
Omodei N
Oppedisano C
Pavlov GG
Peirson AL
Perri M
Pesce-Rollins M
Petrucci P
Possenti A
Puccetti S
Ramsey BD
Ratheesh A
Roberts OJ
Romani RW
Sgrò C
Slane P
Spandre G
Swartz DA
Tamagawa T
Tavecchio F
Taverna R
Tawara Y
Tennant AF
Thomas NE
Tombesi F
Trois A
Tsygankov SS
Turolla R
Vink J
Wu K
IXPE Collaboration
Institute of Physics Publishing
Julkaisun pysyvä osoite on:
https://urn.fi/URN:NBN:fi-fe2025082788773
https://urn.fi/URN:NBN:fi-fe2025082788773
Tiivistelmä
The Imaging X-ray Polarimetry Explorer measured with high significance the X-ray polarization of the brightest Z-source, Sco X-1, resulting in the nominal 2–8 keV energy band in a polarization degree of 1.0% ± 0.2% and a polarization angle of 8° ± 6° at a 90% confidence level. This observation was strictly simultaneous with observations performed by NICER, NuSTAR, and Insight-HXMT, which allowed for a precise characterization of its broadband spectrum from soft to hard X-rays. The source has been observed mainly in its soft state, with short periods of flaring. We also observed low-frequency quasiperiodic oscillations. From a spectropolarimetric analysis, we associate a polarization to the accretion disk at <3.2% at 90% confidence level, compatible with expectations for an electron scattering dominated optically thick atmosphere at the Sco X-1 inclination of ∼44°; for the higher-energy Comptonized component, we obtain a polarization of 1.3% ± 0.4%, in agreement with expectations for a slab of Thomson optical depth of ∼7 and an electron temperature of ∼3 keV. A polarization rotation with respect to previous observations by OSO-8 and PolarLight, and also with respect to the radio-jet position angle, is observed. This result may indicate a variation of the polarization with the source state that can be related to relativistic precession or a change in the corona geometry with the accretion flow.
Kokoelmat
- Rinnakkaistallenteet [29337]
