2006ApJ...645..556K


Query : 2006ApJ...645..556K

2006ApJ...645..556K - Astrophys. J., 645, 556-575 (2006/July-1)

Discovery of luminous pulsed hard X-ray emission from anomalous X-ray pulsars 1RXS J1708-4009, 4U 0142+61, and 1E 2259+586 by INTEGRAL and RXTE.

KUIPER L., HERMSEN W., DEN HARTOG P.R. and COLLMAR W.

Abstract (from CDS):

We investigated the time-averaged high-energy spectral characteristics of the persistent anomalous X-ray pulsars (AXPs) 1RXS J1708-4009, 4U 0142+61, 1E 2259+586, and 1E 1048.1-5937, using RXTE PCA (2-60 keV), RXTE HEXTE (15-250 keV), and INTEGRAL IBIS ISGRI (20-300 keV) data. We discovered hard spectral tails for energies above 10 keV in the total and pulsed spectra of AXPs 1RXS J1708-4009, 4U 0142+4009, and 1E 2259+586, but 1E 1048.1-5937 appeared to be too weak to be detected. Improved hard X-ray spectral information for AXP 1E 1841-045 is also presented. The pulsed and total spectra above 10 keV have power-law shapes, and there is so far no significant evidence for spectral breaks or bends up to ∼150 keV. The pulsed spectra above 10 keV are exceptionally hard with indices for four AXPs in the range -1.0 to 1.0. Below 10 keV these indices were in the range 2.0-4.3, indicating the very drastic spectral changes in a narrow energy interval around 10 keV. The best-fit power-law models to the total spectra between ∼10 and 150 keV are significantly softer, with indices measured for 1E 1841-045, 1RXS J1708-4009, and 4U 0142+61 in the range 1.0-1.4. For the latter AXPs the pulsed fractions are consistent with 100% around 100 keV but are different at 10 keV: ∼10% for 4U 0142+61, ∼25% for 1E 1841-045, and consistent with 100% for 1RXS J1708-4009. The luminosities of these total and pulsed spectral tails (10-150 keV) largely exceed the total available spin-down powers by factors ranging from ∼100 to ∼600. We also reanalyzed archival CGRO COMPTEL (0.75-30 MeV) data: no AXP detections can be claimed, and the obtained upper limits indicate for 1RXS J1708-4009, 4U 0142+61, and 1E 1841-045 that strong breaks or bends must occur somewhere between ∼150 and 750 keV. We discuss predictions from first attempts to model our hard X-ray and soft gamma-ray spectra in the context of the magnetar model.

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Journal keyword(s): Stars: Pulsars: Individual: Alphanumeric: 1E 1048.1-5937 - Stars: Pulsars: Individual: Alphanumeric: 1E 1841-045 - Stars: Pulsars: Individual: Alphanumeric: 1E 2259+586 - Stars: Pulsars: Individual: Alphanumeric: 1RXS J1708-4009 (read: 1RXS J170849.0-400910) - Stars: Pulsars: Individual: Alphanumeric: 4U 0142+61 - X-Rays: Stars

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* V1037 Cas LXB 00 29 03.06 +59 34 19.0           ~ 283 1
2 V* V635 Cas HXB 01 18 31.9704955824 +63 44 33.072603144 17.05 16.64 15.19 14.34 13.22 B0.2Ve 791 0
3 PSR J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
4 EM* GGA 104 HXB 01 47 00.2124077208 +61 21 23.663788056 11.76 12.09 11.366 11.00 10.52 B1IIIe 205 0
5 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
6 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
7 PSR B0540-69 Psr 05 40 11.2000490438 -69 19 54.198559829           ~ 976 3
8 NAME Vela Pulsar Psr 08 35 20.65525 -45 10 35.1545     15.10     ~ 2446 1
9 * eta Car s*b 10 45 03.545808 -59 41 03.95124 6.37 7.03 6.48 6.123 4.41 LBV 2543 0
10 2E 2336 HXB 10 50 08.93 -59 53 19.9           Be 419 0
11 PSR B1509-58 Psr 15 13 47.6 -59 07 54     13.06     ~ 879 1
12 2MASS J17004888-4139214 HXB 17 00 48.884 -41 39 21.46           Ofpe/WN9 272 0
13 HD 153919 HXB 17 03 56.7725629224 -37 50 38.913331452 6.06 6.78 6.51 6.08 5.90 O6Iafcp 851 0
14 PSR J1708-4008 Psr 17 08 46.1 -40 08 56           ~ 315 0
15 PSR J1718-3718 Psr 17 18 10.16 -37 18 53.8           ~ 73 0
16 PSR J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1316 2
17 SNR G027.3+00.0 SNR 18 41 17.8 -04 56 12           ~ 345 3
18 PSR J1841-0456 Psr 18 41 19.29 -04 56 11.4           ~ 296 1
19 PSR J1847-0130 Psr 18 47 35.2 -01 30 46           ~ 44 0
20 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 673 1
21 SNR G109.1-01.0 SNR 23 01 35 +58 53.0           ~ 362 0

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