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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, C bgd = C ¯ bgd ± σ C bgd $ C_{\mathrm{bgd}}=\overline{C}_{\mathrm{bgd}}\pm\sigma_{C_{\mathrm{bgd}}} $, C ¯ bgd $ \overline{C}_{\mathrm{bgd}} $ and σCbgd are the mean and standard deviation of background measurements. Cs is the net source count rate; its error is estimated as [ ( σ C bgd 2 + C s t exp 1 g 1 ] 1 / 2 $ [(\sigma_{C\mathrm{bgd}}^2 + C_{s} t_{\mathrm{exp}}^{-1} g^{-1}]^{1/2} $, 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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