243 research outputs found

    Spectral Statistics and Luminosity Function of a Hard X-ray Complete Sample of Brightest AGNs

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    We investigated the statistics of the X-ray spectral properties of a complete flux-limited sample of bright AGNs from HEAO-1 all-sky catalogs to provide the bright end constraint of the evolution of AGN hard X-ray luminosity function (HXLF) and the AGN population synthesis model of the X-ray background. Spectral studies have been made using ASCA and XMM-Newton observation data for almost all AGNs in this sample.Comment: PTPTex v0.88, 2 pages with 4 figures, Proceedings of the "Stellar-Mass, Intermediate -Masss, and Supermassive Black Holes" in Kyoto, Japa

    X-Ray Study of the Outer Region of Abell 2142 with Suzaku

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    We observed outer regions of a bright cluster of galaxies A2142 with Suzaku. Temperature and brightness structures were measured out to the virial radius (r200r_{200}) with good sensitivity. We confirmed the temperature drop from 9 keV around the cluster center to about 3.5 keV at r200r_{200}, with the density profile well approximated by the β\beta model with β=0.85\beta = 0.85. Within 0.4\r_{200}, the entropy profile agrees with r1.1r^{1.1}, as predicted by the accretion shock model. The entropy slope becomes flatter in the outer region and negative around r200r_{200}. These features suggest that the intracluster medium in the outer region is out of thermal equilibrium. Since the relaxation timescale of electron-ion Coulomb collision is expected to be longer than the elapsed time after shock heating at r200r_{200}, one plausible reason of the low entropy is the low electron temperature compared to that of ions. Other possible explanations would be gas clumpiness, turbulence and bulk motions of ICM\@. We also searched for a warm-hot intergalactic medium around r200r_{200} and set an upper limit on the oxygen line intensity. Assuming a line-of-sight depth of 2 Mpc and oxygen abundance of 0.1 solar, the upper limit of an overdensity is calculated to be 280 or 380, depending on the foreground assumption.Comment: 14 pages, 8 figure

    Metallicity of the Fossil Group NGC 1550 Observed with Suzaku

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    We studied the temperature and metal abundance distributions of the intra-cluster medium (ICM) in a group of galaxies NGC 1550 observed with Suzaku. The NGC 1550 is classified as a fossil group, which have few bright member galaxies except for the central galaxy. Thus, such a type of galaxy is important to investigate how the metals are enriched to the ICM. With the Suzaku XIS instruments, we directly measured not only Si, S, and Fe lines but also O and Mg lines and obtained those abundances to an outer region of ~0.5 r_180 for the first time, and confirmed that the metals in the ICM of such a fossil group are indeed extending to a large radius. We found steeper gradients for Mg, Si, S, and Fe abundances, while O showed almost flat abundance distribution. Abundance ratios of alpha-elements to Fe were similar to those of the other groups and poor clusters. We calculated the number ratio of type II to type Ia supernovae for the ICM enrichment to be 2.9 +- 0.5 within 0.1 r_180, and the value was consistent with those for the other groups and poor clusters observed with Suzaku. We also calculated metal mass-to-light ratios (MLRs) for Fe, O and Mg with B-band and K-band luminosities of the member galaxies of NGC 1550. The derived MLRs were comparable to those of NGC 5044 group in the r<0.1 r_180 region, while those of NGC 1550 are slightly higher than those of NGC 5044 in the outer region.Comment: 11 pages, 7 figures, accepted for publication in PAS

    Detection of Excess Hard X-ray Emission from the Group of Galaxies HCG62

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    From the group of galaxies HCG62, we detected an excess hard X-ray emission in energies above 4\sim 4 keV with \A SCA. The excess emission is spatially extended up to 10\sim10' from the group center, and somewhat enhanced toward north. Its spectrum can be represented by either a power-law of photon index 0.8-2.7, or a Bremsstrahlung of temperature >6.3>6.3 keV. In the 2-10 keV range, the observed hard X-ray flux, (1.0±0.3)×1012(1.0\pm0.3)\times10^{-12} erg cm2^{-2} s1^{-1}, implies a luminosity of (8.0±2.0)×1041(8.0\pm2.0)\times10^{41} erg s1^{-1} for a Hubble constant of 50 km s1^{-1} Mpc1^{-1}. The emission is thus too luminous to be attributed to X-ray binaries in the memb er galaxies. We discuss possible origin of the hard X-ray emission.Comment: 6 pages, 3 Postscript figures, uses emulateapj.sty. Accepted for publication in the Astrophysical Journal Letter

    Properties of the cosmological filament between two clusters: A possible detection of a large-scale accretion shock by SuzakuSuzaku

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    We report on the results of a SuzakuSuzaku observation of the plasma in the filament located between the two massive clusters of galaxies Abell 399 and Abell 401. Abell 399 (zz=0.0724) and Abell 401 (zz=0.0737) are expected to be in the initial phase of a cluster merger. In the region between the two clusters, we find a clear enhancement in the temperature of the filament plasma from 4 keV (expected value from a typical cluster temperature profile) to kTkT\sim6.5 keV. Our analysis also shows that filament plasma is present out to a radial distance of 15' (1.3 Mpc) from a line connecting the two clusters. The temperature profile is characterized by an almost flat radial shape with kTkT\sim6-7 keV within 10' or \sim0.8 Mpc. Across rr=8'~from the axis, the temperature of the filament plasma shows a drop from 6.3 keV to 5.1 keV, indicating the presence of a shock front. The Mach number based on the temperature drop is estimated to be M{\cal M}\sim1.3. We also successfully determined the abundance profile up to 15' (1.3 Mpc), showing an almost constant value (ZZ=0.3 solar) at the cluster outskirt. We estimated the Compton yy-parameter to be \sim14.5±1.3×106\pm1.3\times10^{-6}, which is in agreement with PlanckPlanck's results (14-17×106\times10^{-6} on the filament). The line of sight depth of the filament is ll\sim1.1 Mpc, indicating that the geometry of filament is likely a pancake shape rather than cylindrical. The total mass of the filamentary structure is \sim7.7×1013 M\times10^{13}~\rm M_{\odot}. We discuss a possible interpretation of the drop of X-ray emission at the rim of the filament, which was pushed out by the merging activity and formed by the accretion flow induced by the gravitational force of the filament.Comment: 8 pages, 8 figures, accepted for publication in A&
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