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X-ray polarimetry of X-ray pulsar X Persei: another orthogonal rotator?

Mushtukov AA; Tsygankov SS; Poutanen J; Doroshenko V; Salganik A; Costa E; Di Marco A; Heyl J; La Monaca F; Lutovinov AA; Mereminsky IA; Papitto A; Semena AN; Shtykovsky AE; Suleimanov VF; Forsblom SV; Gonzalez-Caniulef D; Malacaria C; Sunyaev RA; Agudo I; Antonelli LA; Bachetti M; Baldini L; Baumgartner WH; Bellazzini R; Bianchi S; Bongiorno SD; Bonino R; Brez A; Bucciantini N; Capitanio F; Castellano S; Cavazzuti E; Chen CT; Ciprini S; De Rosa A; Del Monte E; Di Gesu L; Di Lalla N; Donnarumma I; Dovciak M; Ehlert SR; Enoto T; Evangelista Y; Fabiani S; Ferrazzoli R; Garcia JA; Gunji S; Hayashida K; Iwakiri W; Jorstad SG; Kaaret P; Karas V; Kislat F; Kitaguchi T; Kolodziejczak JJ; Krawczynski H; Latronico L; Liodakis I; Maldera S; Manfreda A; Marin F; Marscher AP; Marshall HL; Massaro F; Matt G; Mitsuishi I; Mizuno T; Muleri F; Negro M; Ng CY; O'Dell SL; Omodei N; Oppedisano C; Pavlov GG; Peirson AL; Perri M; Pesce-Rollins M; Petrucci PO; Pilia M; Possenti A; Puccetti S; Ramsey BD; Rankin J; Ratheesh A; Roberts OJ; Romani RW; Sgro 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; Turolla R; Vink J; Weisskopf MC; Wu K; Xie F; Zane S

X-ray polarimetry of X-ray pulsar X Persei: another orthogonal rotator?

Mushtukov AA
Tsygankov SS
Poutanen J
Doroshenko V
Salganik A
Costa E
Di Marco A
Heyl J
La Monaca F
Lutovinov AA
Mereminsky IA
Papitto A
Semena AN
Shtykovsky AE
Suleimanov VF
Forsblom SV
Gonzalez-Caniulef D
Malacaria C
Sunyaev RA
Agudo I
Antonelli LA
Bachetti M
Baldini L
Baumgartner WH
Bellazzini R
Bianchi S
Bongiorno SD
Bonino R
Brez A
Bucciantini N
Capitanio F
Castellano S
Cavazzuti E
Chen CT
Ciprini S
De Rosa A
Del Monte E
Di Gesu L
Di Lalla N
Donnarumma I
Dovciak M
Ehlert SR
Enoto T
Evangelista Y
Fabiani S
Ferrazzoli R
Garcia JA
Gunji S
Hayashida K
Iwakiri W
Jorstad SG
Kaaret P
Karas V
Kislat F
Kitaguchi T
Kolodziejczak JJ
Krawczynski H
Latronico L
Liodakis I
Maldera S
Manfreda A
Marin F
Marscher AP
Marshall HL
Massaro F
Matt G
Mitsuishi I
Mizuno T
Muleri F
Negro M
Ng CY
O'Dell SL
Omodei N
Oppedisano C
Pavlov GG
Peirson AL
Perri M
Pesce-Rollins M
Petrucci PO
Pilia M
Possenti A
Puccetti S
Ramsey BD
Rankin J
Ratheesh A
Roberts OJ
Romani RW
Sgro 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
Turolla R
Vink J
Weisskopf MC
Wu K
Xie F
Zane S
Katso/Avaa
X-ray polarimetry of X-ray pulsar X Persei another orthogonal rotator.pdf (2.096Mb)
Lataukset: 

OXFORD UNIV PRESS
doi:10.1093/mnras/stad1961
URI
https://academic.oup.com/mnras/article/524/2/2004/7210538
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Julkaisun pysyvä osoite on:
https://urn.fi/URN:NBN:fi-fe2025082789785
Tiivistelmä

X Persei is a persistent low-luminosity X-ray pulsar of period of ≈ 835 s in a Be binary system. The field strength at the neutron star surface is not known precisely, but indirect signs indicate a magnetic field above 1013 G, which makes the object one of the most magnetized known X-ray pulsars. Here we present the results of observations X Persei performed with the Imaging X-ray Polarimetry Explorer (IXPE). The X-ray polarization signal was found to be strongly dependent on the spin phase of the pulsar. The energy-averaged polarization degree in 3–8 keV band varied from several to ∼20 per cent over the pulse with a phase dependence resembling the pulse profile. The polarization angle shows significant variation and makes two complete revolutions during the pulse period, resulting in nearly nil pulse-phase averaged polarization. Applying the rotating vector model to the IXPE data we obtain the estimates for the rotation axis inclination and its position angle on the sky, as well as for the magnetic obliquity. The derived inclination is close to the orbital inclination, reported earlier for X Persei. The polarimetric data imply a large angle between the rotation and magnetic dipole axes, which is similar to the result reported recently for the X-ray pulsar GRO J1008−57. After eliminating the effect of polarization angle rotation over the pulsar phase using the best-fitting rotating vector model, the strong dependence of the polarization degree with energy was discovered, with its value increasing from 0 at ∼2 keV to 30per cent at 8 keV.

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