Abstract

We construct a new X-ray (2--10 keV) luminosity function of Compton-thin active galactic nuclei (AGNs) in the local universe, using the first MAXI/GSC source catalog surveyed in the 4--10 keV band. The sample consists of 37 non-blazar AGNs at z=0.002−0.2z=0.002-0.2, whose identification is highly (>97>97%) complete. We confirm the trend that the fraction of absorbed AGNs with NH>1022N_{\rm H} > 10^{22} cm−2^{-2} rapidly decreases against luminosity (LXL_{\rm X}), from 0.73±\pm0.25 at LX=1042−43.5L_{\rm X} = 10^{42-43.5} erg s−1^{-1} to 0.12±0.09\pm0.09 at LX=1043.5−45.5L_{\rm X} = 10^{43.5-45.5} erg s−1^{-1}. The obtained luminosity function is well fitted with a smoothly connected double power-law model whose indices are γ1=0.84γ_1 = 0.84 (fixed) and γ2=2.0±0.2γ_2 = 2.0\pm0.2 below and above the break luminosity, L∗=1043.3±0.4L_{*} = 10^{43.3\pm0.4} ergs s−1^{-1}, respectively. While the result of the MAXI/GSC agrees well with that of HEAO-1 at $L_{\rm X} \gtsim 10^{43.5}$ erg s−1^{-1}, it gives a larger number density at the lower luminosity range. Comparison between our luminosity function in the 2--10 keV band and that in the 14--195 keV band obtained from the Swift/BAT survey indicates that the averaged broad band spectra in the 2--200 keV band should depend on luminosity, approximated by Γ∼1.7Γ\sim1.7 for $L_{\rm X} \ltsim 10^{44}$ erg s−1^{-1} while Γ∼2.0Γ\sim 2.0 for $L_{\rm X} \gtsim 10^{44}$ erg s−1^{-1}. This trend is confirmed by the correlation between the luminosities in the 2--10 keV and 14--195 keV bands in our sample. We argue that there is no contradiction in the luminosity functions between above and below 10 keV once this effect is taken into account.

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