A BeppoSAX observation of KS 1731-260 in its quiescent state:: Constraints on the magnetic field of the neutron star

被引:18
作者
Burderi, L
Di Salvo, T
Stella, L
Fiore, F
Robba, NR
van der Klis, M
Iaria, R
Mendez, M
Menna, MT
Campana, S
Gennaro, G
Rebecchi, S
Burgay, M
机构
[1] Osserv Astron Roma, Sede Monteporzio Catone, I-00040 Rome, Italy
[2] Univ Amsterdam, Astron Inst Anton Pannekoek, NL-1098 SJ Amsterdam, Netherlands
[3] Univ Amsterdam, Ctr High Energy Astrophys, NL-1098 SJ Amsterdam, Netherlands
[4] Univ Palermo, Dipartimento Sci Fis & Astron, I-90123 Palermo, Italy
[5] SRON, Natl Inst Space Res, NL-3584 CA Utrecht, Netherlands
[6] Osserv Astron Brera, I-23807 Merate, Italy
[7] Telespazio Spa, Direz Gen, I-00156 Rome, Italy
[8] Agenzia Spaziale Italiana, Consorzio Interuniv Fis Spaziale, I-00198 Rome, Italy
[9] Univ Bologna, Dipartimento Astron, I-40127 Bologna, Italy
关键词
accretion; accretion disks; stars : individual (KS 1731-260); stars : neutron; X-rays : general; X-rays : stars;
D O I
10.1086/341058
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We report here the results of a 90 ks BeppoSAX observation of the low-mass X-ray binary and atoll source KS 1731-260 during a quiescent phase. From this observation we derive a source X-ray luminosity of similar to10(33) ergs s(-1) (for a source distance of 7 kpc). If the neutron star is spinning at a period of a few milliseconds, as inferred from the nearly coherent oscillations observed during type I X-ray bursts, the quiescent X-ray luminosity constrains the neutron star magnetic field strength. We consider all the mechanisms that have been proposed to explain the quiescent X-ray emission of neutron star X-ray transients and compare the corresponding expectations with the measured upper limit on the X-ray luminosity. We find that, in any case, the neutron star magnetic field is most probably less than similar to10(9) G. We have also observed KS 1731-260, still in its quiescent state, at 1.4 GHz with the Parkes radio telescope to search for radio pulses. We found that no radio signals with millisecond periods are present with an upper limit on the flux of 0.60 mJy using a 4 minute integration time (optimal for a close system with an orbital period smaller than a few hours) and of 0.21 mJy using a 35 minute integration time (optimal for a wide-orbit system).
引用
收藏
页码:930 / 936
页数:7
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