2012ApJS..201...37K


Query : 2012ApJS..201...37K

2012ApJS..201...37K - Astrophys. J., Suppl. Ser., 201, 37 (2012/August-0)

Chandra pulsar survey (ChaPS).

KARGALTSEV O., DURANT M., PAVLOV G.G. and GARMIRE G.

Abstract (from CDS):

Taking advantage of the high sensitivity of the Chandra X-ray Observatory's (CXO) Advanced CCD Imaging Spectrometer, we have conducted a snapshot survey of pulsars previously undetected in X-rays. We detected 12 pulsars and established deep flux limits for 11 pulsars. Using these new results, we revisit the relationship between the X-ray luminosity, L psrX, and spin-down power, {dot}E. We find that the obtained limits further increase the extremely large spread in the non-thermal X-ray efficiencies, ηpsrX= L psrX/{dot}E, with some of them being now below 10–5. Such a spread cannot be explained by poorly known distances or by beaming of pulsar radiation. We also find evidence of a break in the dependence of L psrX on {dot}E, such that pulsars become more X-ray efficient at {dot}E-1035 erg/s. We examine the relationship between the γ-ray luminosity, L psrγ, and {dot}E, which exhibits a smaller scatter compared to that in X-rays. This confirms that the very large spread in the X-ray efficiencies cannot be explained just by the beaming because the γ-ray emission is generally expected to be beamed stronger than the X-ray emission. Intriguingly, there is also an indication of a break in the L psrγ{dot}E dependence at {dot}E erg/s, with lower-{dot}E pulsars becoming less γ-ray efficient. We also examine the distance-independent L psrγ/L psrX ratio as a function of {dot}E for a sample of γ-ray pulsars observed by CXO and find that it peaks at {dot}E erg/s, showing that the breaks cannot originate from poorly measured distances. We discuss the implications of our findings for existing models of magnetospheric emission and venues for further exploration.

Abstract Copyright: ∼

Journal keyword(s): pulsars: general - X-rays: general

Simbad objects: 28

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Number of rows : 28
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 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
2 PSR B0540-69 Psr 05 40 11.2000490438 -69 19 54.198559829           ~ 976 3
3 PSR J0729-1448 Psr 07 29 16.45 -14 48 36.8           ~ 71 0
4 PSR B0906-49 Psr 09 08 35.46000 -49 13 05.0000           ~ 168 0
5 PSR J0940-5428 Psr 09 40 58.22 -54 28 40.6           ~ 61 0
6 PSR J1023-5746 Psr 10 23 02.84 -57 46 06.9           ~ 70 0
7 FGES J1023.3-5747 gam 10 23 15.18313 -57 46 34.7840           ~ 57 0
8 PSR J1028-5819 Psr 10 28 27.888 -58 19 06.14           ~ 122 1
9 PSR J1105-6107 Psr 11 05 26.1400 -61 07 48.940           ~ 129 0
10 PSR J1413-6205 Psr 14 13 30.135 -62 05 37.02           ~ 50 0
11 PSR J1524-5625 Psr 15 24 49.820 -56 25 24.07           ~ 36 0
12 PSR J1531-5610 Psr 15 31 27.91 -56 10 55.0           ~ 59 0
13 PSR J1648-4611 Psr 16 48 22.02 -46 11 16.0           ~ 73 0
14 PSR J1702-4310 Psr 17 02 26.94 -43 10 41.5           ~ 30 0
15 PSR J1702-4128 Psr 17 02 52.52 -41 28 48.2           ~ 72 0
16 PSR J1718-3825 Psr 17 18 13.558 -38 25 17.83           ~ 108 0
17 PSR B1727-33 Psr 17 30 32.559 -33 50 39.40           ~ 130 1
18 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
19 PSR B1822-14 Psr 18 25 02.927 -14 46 52.60           ~ 92 0
20 PSR J1835-1106 Psr 18 35 18.287 -11 06 15.10           ~ 75 0
21 PSR B1835-06.1 Psr 18 37 43.55 -06 04 49.0           ~ 77 0
22 PSR B1839-03.8 Psr 18 41 38.68 -03 48 42.6           ~ 44 0
23 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
24 PSR J1913+1011 Psr 19 13 20.341 +10 11 22.97           ~ 84 0
25 PSR J1928+1746 Psr 19 28 42.8 +17 46 27           ~ 62 0
26 PSR J1958+2846 Psr 19 58 40.1015582448 +28 45 54.108736344           ~ 81 0
27 PSR J2022+3842 Psr 20 22 21.689 +38 42 14.82           ~ 66 0
28 NAME Local Bubble ISM ~ ~           ~ 1059 0

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