40,959 research outputs found

    Ultraviolet/X-ray variability and the extended X-ray emission of the radio-loud broad absorption line quasar PG 1004+130

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    We present the results of recent Chandra, XMM-Newton, and Hubble Space Telescope observations of the radio-loud (RL), broad absorption line (BAL) quasar PG 1004+130. We compare our new observations to archival X-ray and UV data, creating the most comprehensive, high signal-to-noise, multi-epoch, spectral monitoring campaign of a RL BAL quasar to date. We probe for variability of the X-ray absorption, the UV BAL, and the X-ray jet, on month-year timescales. The X-ray absorber has a low column density of NH=8×10204×1021N_{H}=8\times10^{20}-4\times10^{21} cm2^{-2} when it is assumed to be fully covering the X-ray emitting region, and its properties do not vary significantly between the 4 observations. This suggests the observed absorption is not related to the typical "shielding gas" commonly invoked in BAL quasar models, but is likely due to material further from the central black hole. In contrast, the CIV BAL shows strong variability. The equivalent width (EW) in 2014 is EW=11.24±\pm0.56 \AA, showing a fractional increase of ΔEW/EW\Delta EW / \langle EW \rangle=1.16±\pm0.11 from the 2003 observation, 3183 days earlier in the rest-frame. This places PG 1004+130 among the most highly variable BAL quasars. By combining Chandra observations we create an exposure 2.5 times deeper than studied previously, with which to investigate the nature of the X-ray jet and extended diffuse X-ray emission. An X-ray knot, likely with a synchrotron origin, is detected in the radio jet ~8 arcsec (30 kpc) from the central X-ray source with a spatial extent of ~4 arcsec (15 kpc). No similar X-ray counterpart to the counterjet is detected. Asymmetric, non-thermal diffuse X-ray emission, likely due to inverse Compton scattering of Cosmic Microwave Background photons, is also detected.Comment: 15 pages, 7 figures, 3 tables. Accepted for publication in Ap

    Dynamic Monte Carlo Study of the Two-Dimensional Quantum XY Model

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    We present a dynamic Monte Carlo study of the Kosterlitz-Thouless phase transition for the spin-1/2 quantum XY model in two dimensions. The short-time dynamic scaling behaviour is found and the dynamical exponent θ\theta, zz and the static exponent η\eta are determined at the transition temperature.Comment: 6 pages with 3 figure

    X-ray Insights into the Nature of Quasars with Redshifted Broad Absorption Lines

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    We present ChandraChandra observations of seven broad absorption line (BAL) quasars at z=0.863z=0.863-2.516 with redshifted BAL troughs (RSBALs). Five of our seven targets were detected by ChandraChandra in 4-13 ks exposures with ACIS-S. The αox\alpha_{\rm ox} values, Δαox\Delta\alpha_{\rm ox} values, and spectral energy distributions of our targets demonstrate they are all X-ray weak relative to expectations for non-BAL quasars, and the degree of X-ray weakness is consistent with that of appropriately-matched BAL quasars generally. Furthermore, our five detected targets show evidence for hard X-ray spectral shapes with a stacked effective power-law photon index of Γeff=0.50.4+0.5\Gamma_{\rm eff}=0.5^{+0.5}_{-0.4}. These findings support the presence of heavy X-ray absorption (NH2×1023N_{\rm H}\approx 2 \times 10^{23} cm2^{-2}) in RSBAL quasars, likely by the shielding gas found to be common in BAL quasars more generally. We use these X-ray measurements to assess models for the nature of RSBAL quasars, finding that a rotationally-dominated outflow model is favored while an infall model also remains plausible with some stipulations. The X-ray data disfavor a binary quasar model for RSBAL quasars in general.Comment: 11 pages, 5 figures, and 3 table

    Dynamic Approach to the Fully Frustrated XY Model

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    Using Monte Carlo simulations, we systematically investigate the non-equilibrium dynamics of the chiral degree of freedom in the two-dimensional fully frustrated XY model. The critical initial increase of the staggered chiral magnetization is observed. By means of the short-time dynamics approach, we estimate the second order phase transition temperature TcT_{c} and all the dynamic and static critical exponents θ\theta, z, β\beta and ν\nu.Comment: 5 pages with 6 figures include
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