2000ApJ...532.1150Z


Query : 2000ApJ...532.1150Z

2000ApJ...532.1150Z - Astrophys. J., 532, 1150-1171 (2000/April-1)

Full polar cap cascade scenario: gamma-ray and X-ray luminosities from spin-powered pulsars.

ZHANG B. and HARDING A.K.

Abstract (from CDS):

Canonical polar cap cascade models involve curvature radiation (CR) or inverse Compton scattering (ICS) of the primary particles and synchrotron radiation (SR) of the higher generation pairs. Here we modify such a cascade picture to include the ICS of the higher generation pairs. In such a ``full-cascade'' scenario, not only the perpendicular portion of the energy of the pairs goes to high-energy radiation via SR, but the parallel portion of the energy of the pairs can also contribute to high-energy emission via ICS with the soft thermal photons from either the full neutron star surface or the hot polar cap. The efficiency of converting particles' kinetic energy to radiation by ICS is very high if the scatterings occur in the ``resonant'' regime. As a result, almost 100% of the energy input from the pulsar inner accelerators could be converted to high-energy emission. An important output of such a scenario is that the soft tail of the ICS spectrum can naturally result in a nonthermal X-ray component that can contribute to the luminosities observed by ROSAT and ASCA. Here we present an analytic description of such a full polar cap cascade scenario using the recursion relationships between adjacent generations following the approach first proposed by Lu et al., but we develop it to be able to delineate the complex full-cascade process. The acceleration model we adopted is the space-charge-limited flow model proposed by Harding & Muslimov. We present the theoretical predictions of the γ-ray luminosities, the thermal and nonthermal X-ray luminosities for the known spin-powered X-ray pulsars (eight of them are also γ-ray pulsars) and compare them with the observations from CGRO, ROSAT, and ASCA. We estimate the nonthermal X-ray luminosity by including all the possible ICS branches contributing to a certain energy band and estimate both the full surface and hot polar cap thermal X-ray luminosities by adopting a standard neutron star cooling scenario, and by treating self-consistent polar cap heating in the Harding & Muslimov model, respectively. Our results show that the observed different dependences of the high-energy luminosities on the pulsar spin-down luminosities, i.e., Lγ∝(Lsd)1/2 and LX∼10–3Lsd, are well reproduced. We found that, for normal pulsars, both the hard (ASCA band) and the soft (ROSAT band) X-ray luminosities are dominated by the nonthermal X-rays of ICS origin, although for some pulsars, thermal components due to either neutron star cooling or polar cap heating can have comparable luminosities so that they are detectable. For the millisecond pulsars, our predicted upper limits of the thermal luminosities due to polar cap heating are usually higher than the ICS-origin nonthermal components if there are no strong multipolar magnetic field components near the neutron star surface; thus, the pulsed soft X-rays in the ROSAT band from most of the millisecond pulsars might be of thermal origin.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays: Theory - Stars: Pulsars: General - Radiation Mechanisms: Nonthermal - X-Rays: Stars

Simbad objects: 35

goto Full paper

goto View the references in ADS

Number of rows : 35
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 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
2 PSR B0355+54 Psr 03 58 53.7165 +54 13 13.727           ~ 465 1
3 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
4 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
5 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
6 PSR J0538+2813 Psr 05 38 25.06 +28 17 11.0           ~ 224 1
7 PSR B0540-69 Psr 05 40 11.2000490438 -69 19 54.198559829           ~ 976 3
8 PSR J0633+1746 Psr 06 33 54.153 +17 46 12.91           ~ 1308 0
9 PSR B0656+14 Psr 06 59 48.18800 +14 14 19.2000   24.85 24.90     ~ 943 1
10 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
11 PSR B0823+26 Psr 08 26 51.5068 +26 37 21.297           ~ 541 1
12 NAME Vela Pulsar Psr 08 35 20.65525 -45 10 35.1545     15.10     ~ 2446 1
13 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
14 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
15 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
16 PSR B1046-58 Psr 10 48 13.10000 -58 32 03.0000           ~ 293 0
17 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
18 PSR J1105-6107 Psr 11 05 26.1400 -61 07 48.940           ~ 129 0
19 CPD-63 2495 HXB 13 02 47.6544015048 -63 50 08.626970292 10.34 10.72 9.98 10.03   O9.5Ve 852 0
20 PSR B1509-58 Psr 15 13 47.6 -59 07 54     13.06     ~ 879 1
21 PSR J1614-5048 Psr 16 14 11.29 -50 48 03.5           ~ 128 0
22 PSR J1617-5055 Psr 16 17 29.35 -50 55 12.8           ~ 128 1
23 PSR B1706-44 Psr 17 09 42.62000 -44 29 12.0000     13.30     ~ 670 1
24 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
25 PSR B1800-21 Psr 18 03 51.40000 -21 37 07.0000           ~ 278 1
26 PSR J1811-1926 Psr 18 11 29.15 -19 25 25.4           ~ 136 1
27 PSR J1824-2452A Psr 18 24 32.009 -24 52 11.10           ~ 529 2
28 PSR B1823-13 Psr 18 26 13.06 -13 34 48.1           ~ 460 1
29 PSR B1853+01 Psr 18 56 10.65 +01 13 21.3           ~ 211 1
30 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 801 0
31 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
32 PSR B1951+32 Psr 19 52 58.181 +32 52 40.98           ~ 615 2
33 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 854 3
34 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
35 PSR B2334+61 Psr 23 37 05.779 +61 51 01.69           ~ 206 1

To bookmark this query, right click on this link: simbad:objects in 2000ApJ...532.1150Z and select 'bookmark this link' or equivalent in the popup menu