146 research outputs found

    Gemini Planet Imager Observational Calibrations VI: Photometric and Spectroscopic Calibration for the Integral Field Spectrograph

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    The Gemini Planet Imager (GPI) is a new facility instrument for the Gemini Observatory designed to provide direct detection and characterization of planets and debris disks around stars in the solar neighborhood. In addition to its extreme adaptive optics and corona graphic systems which give access to high angular resolution and high-contrast imaging capabilities, GPI contains an integral field spectrograph providing low resolution spectroscopy across five bands between 0.95 and 2.5 μ\mum. This paper describes the sequence of processing steps required for the spectro-photometric calibration of GPI science data, and the necessary calibration files. Based on calibration observations of the white dwarf HD 8049B we estimate that the systematic error in spectra extracted from GPI observations is less than 5%. The flux ratio of the occulted star and fiducial satellite spots within coronagraphic GPI observations, required to estimate the magnitude difference between a target and any resolved companions, was measured in the HH-band to be Δm=9.23±0.06\Delta m = 9.23\pm0.06 in laboratory measurements and Δm=9.39±0.11\Delta m = 9.39\pm 0.11 using on-sky observations. Laboratory measurements for the YY, JJ, K1K1 and K2K2 filters are also presented. The total throughput of GPI, Gemini South and the atmosphere of the Earth was also measured in each photometric passband, with a typical throughput in HH-band of 18% in the non-coronagraphic mode, with some variation observed over the six-month period for which observations were available. We also report ongoing development and improvement of the data cube extraction algorithm.Comment: 15 pages, 6 figures. Proceedings of the SPIE, 9147-30

    Accretion onto a Supermassive Black Hole Binary Before Merger

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    While supermassive binary black holes (SMBBHs) inspiral toward merger they may also accrete significant amounts of matter. To study the dynamics of such a system requires simultaneously describing the evolving spacetime and the dynamics of magnetized plasma. Here we present the first relativistic calculation simulating two equal-mass, non-spinning black holes as they inspiral from an initial separation of 20M20M (G=c=1G=c=1) almost to merger, ≃9M\simeq 9M, while accreting gas from a surrounding disk, where MM is the total binary mass. We find that the accretion rate M˙\dot M onto the black holes first decreases during this period and then reaches a plateau, dropping by only a factor of ∼3\sim 3 despite its rapid inspiral. An estimated bolometric light curve follows the same profile. The minidisks through which the accretion reaches the black holes are very non-standard. Reynolds, not Maxwell, stresses dominate, and they oscillate between two distinct structural states. In one part of the cycle, ``sloshing" streams transfer mass from one minidisk to the other through the L1 point at a rate ∼0.1×\sim 0.1\times the accretion rate, carrying kinetic energy at a rate that can be as large as the peak minidisk bolometric luminosity. We also discover that the minidisks have time-varying tilts with respect to the orbital plane similar in magnitude to the circumbinary disk's aspect ratio. The unsigned poloidal flux on the black hole event horizon is roughly constant at a dimensionless level ϕ∼2−3\phi\sim 2-3, but doubles just before merger; if the black holes had significant spin, this flux could support jets whose power could approach the radiated luminosity. This simulation is the first to employ our multipatch infrastructure \pwmhd, decreasing computational expense per physical time to ∼3%\sim 3\% of similar runs using conventional single-grid methods.Comment: Comments welcom
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