Table 1.
Pulsar photometry.
Filter | λp | Weff | texp | rextr | ϕ | Ctot | Cbgd | Cs | 𝒫ν | ⟨fν⟩ |
---|---|---|---|---|---|---|---|---|---|---|
Å | Å | s | arcsec | % | cnts/ks | cnts/ks | cnts/ks | nJy ks/cnts | nJy | |
F125LP | 1426 | 340 | 1830 | 0.2 | 62 | 103.8 | 23.1,3.7 | 80.7,7.6 | 0.875 | 113,11 |
F140LP | 1519 | 259 | 566 | 0.25 | 67 | 77.0 | 17.7,6.6 | 59.3,12.2 | 1.668 | 148,30 |
bhigh | 4360 | 952 | 4680 | 0.38 | 70 | 71200 | 69420,370 | 1780,370 | ... | 85,18 |
vhigh | 5524 | 1187 | 5400 | 0.25 | 51 | 97970 | 94560,920 | 3410,920 | ... | 163,44 |
Notes. λp and Weff = [∫T(λ)dλ][Max(T(λ))]−1 are the pivot wavelength and the effective width of the filter, ϕ is the fraction of source counts in the aperture with radius rextr, Ctot is the total count rate in the source aperture, ,
and σCbgd are the mean and standard deviation of background measurements. Cs is the net source count rate; its error is estimated as
, where g is the gain, ⟨fν⟩ = Cs𝒫ν/ϕ is the mean flux density; and 𝒫ν is the count rate-to-flux conversion factor.
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