Source | d | P | ![]() |
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[kpc] | [ms] | [ky] | [erg/s] | [erg/cm2 s] | [erg/cm2 s] | [erg/s] | [erg/s] | |||
B0531+21 | 2.0 | 29.7 | 1.3 | 4.4E+38 |
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6.2E-3 |
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1.4E-3![]() |
B1509-58 | 5.8 | 151.5 | 1.6 | 1.7E+37 |
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3.5E-2 |
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1.2E-2c |
J0205+6449 | 3.2 | 65.7 | 5.4 | 2.7E+37 |
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1.7E-4 |
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3.0E-3![]() |
B0833-045 | 0.287 | 89.3 | 11.4 | 6.9E+36 |
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1.3E-5 |
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1.1E-2![]() |
Notes. The luminosities of the pulsed emission L are calculated as
with values for the distance d taken from the table, and the beaming fraction
set to 1. F represent the pulsed flux.
(a) Luminosities, fluxes, and efficiencies labeled with x are evaluated for the 2-100 keV band.
(b) Luminosities, fluxes, and efficiencies labeled with
are evaluated for the 0.1-10 GeV band. (c) The
-ray
energy flux of PSR B1509-58 in the 0.1-10 GeV band has been
derived from the (total) photon flux values for the 100-300 and
300-1000 MeV bands as given in Kuiper et al. (1999)
assuming a power-law shape with photon index of 2.5, and should be
considered as an upper-limit to the pulsed flux of PSR B1509-58 in the
0.1-10 GeV band.
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