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Discovery of a variable energy-dependent X-ray polarization in the accreting neutron star GX 5−1

Fabiani S; Capitanio F; Iaria R; Poutanen J; Gnarini A; Ursini F; Farinelli R; Bobrikova A; Steiner JF; Svoboda J; Anitra A; Baglio MC; Carotenuto F; Del Santo M; Ferrigno C; Lewis F; Russell DM; Russell TD; Eijnden J; Cocchi M; Di Marco A; La Monaca F; Liu K; Rankin J; Weisskopf MC; Xie F; Bianchi S; Burderi L; Di Salvo T; Egron E; Illiano G; Kaaret P; Matt G; Mikušincová R; Muleri F; Papitto A; Agudo I; Antonelli LA; Bachetti M; Baldini L; Baumgartner WH; Bellazzini R; Bongiorno SD; Bonino R; Brez A; Bucciantini N; Castellano S; Cavazzuti E; Chen C; Ciprini S; Costa E; De Rosa A; Del Monte E; Di Gesu L; Di Lalla N; Donnarumma I; Doroshenko V; Dovčiak M; Ehlert SR; Enoto T; Evangelista Y; Ferrazzoli R; Garcia JA; Gunji S; Hayashida K; Heyl J; Iwakiri W; Jorstad SG; Karas V; Kislat F; Kitaguchi T; Kolodziejczak JJ; Krawczynski H; Latronico L; Liodakis I; Maldera S; Manfreda A; Marin F; Marinucci A; Marscher AP; Marshall HL; Massaro F; 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; Pilia M; Possenti A; Puccetti S; Ramsey BD; Ratheesh A; Roberts OJ; Romani RW; Sgrò C; Slane P; Soffitta 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; Zane S

Discovery of a variable energy-dependent X-ray polarization in the accreting neutron star GX 5−1

Fabiani S
Capitanio F
Iaria R
Poutanen J
Gnarini A
Ursini F
Farinelli R
Bobrikova A
Steiner JF
Svoboda J
Anitra A
Baglio MC
Carotenuto F
Del Santo M
Ferrigno C
Lewis F
Russell DM
Russell TD
Eijnden J
Cocchi M
Di Marco A
La Monaca F
Liu K
Rankin J
Weisskopf MC
Xie F
Bianchi S
Burderi L
Di Salvo T
Egron E
Illiano G
Kaaret P
Matt G
Mikušincová R
Muleri F
Papitto A
Agudo I
Antonelli LA
Bachetti M
Baldini L
Baumgartner WH
Bellazzini R
Bongiorno SD
Bonino R
Brez A
Bucciantini N
Castellano S
Cavazzuti E
Chen C
Ciprini S
Costa E
De Rosa A
Del Monte E
Di Gesu L
Di Lalla N
Donnarumma I
Doroshenko V
Dovčiak M
Ehlert SR
Enoto T
Evangelista Y
Ferrazzoli R
Garcia JA
Gunji S
Hayashida K
Heyl J
Iwakiri W
Jorstad SG
Karas V
Kislat F
Kitaguchi T
Kolodziejczak JJ
Krawczynski H
Latronico L
Liodakis I
Maldera S
Manfreda A
Marin F
Marinucci A
Marscher AP
Marshall HL
Massaro F
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
Pilia M
Possenti A
Puccetti S
Ramsey BD
Ratheesh A
Roberts OJ
Romani RW
Sgrò C
Slane P
Soffitta 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
Zane S
Katso/Avaa
aa47374-23.pdf (7.378Mb)
Lataukset: 

EDP Sciences
doi:10.1051/0004-6361/202347374
URI
https://doi.org/10.1051/0004-6361/202347374
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Julkaisun pysyvä osoite on:
https://urn.fi/URN:NBN:fi-fe2025082791099
Tiivistelmä

We report on the coordinated observations of the neutron star low-mass X-ray binary (NS-LMXB) GX 5−1 in X-rays (IXPE, NICER, NuSTAR, and INTEGRAL), optical (REM and LCO), near-infrared (REM), mid-infrared (VLT VISIR), and radio (ATCA). This Z-source was observed by IXPE twice in March–April 2023 (Obs. 1 and 2). In the radio band the source was detected, but only upper limits to the linear polarization were obtained at a 3σ level of 6.1% at 5.5 GHz and 5.9% at 9 GHz in Obs. 1 and 12.5% at 5.5 GHz and 20% at 9 GHz in Obs. 2. The mid-IR, near-IR, and optical observations suggest the presence of a compact jet that peaks in the mid- or far-IR. The X-ray polarization degree was found to be 3.7%±0.4% (at 90% confidence level) during Obs. 1 when the source was in the horizontal branch of the Z-track and 1.8%±0.4% during Obs. 2 when the source was in the normal-flaring branch. These results confirm the variation in polarization degree as a function of the position of the source in the color-color diagram, as for previously observed Z-track sources (Cyg X-2 and XTE 1701−462). Evidence of a variation in the polarization angle of ∼20° with energy is found in both observations, likely related to the different, nonorthogonal polarization angles of the disk and Comptonization components, which peak at different energies.

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