1,924 research outputs found

    Jet-Disc coupling in the accreting black hole XTEJ1118+480

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    We interpret the rapid correlated UV/optical/ X-ray variability of XTEJ1118+480 as a signature of the coupling between the X-ray corona and a jet emitting synchrotron radiation in the optical band.We propose a scenario in which the jet and the X-ray corona are fed by the same energy reservoir where large amounts of accretion power are stored before being channelled into either the jet or the high energy radiation. This time dependent model reproduces the main features of the rapid multi-wavelength variability of XTEJ1118+480. A strong requirement of the model is that the total jet power should be at least a few times larger than the observed X-ray luminosity. This would be consistent with the overall low radiative efficiency of the source. We present independent arguments showing that the jet probably dominates the energetic output of all accreting black holes in the low-hard state.Comment: 8 pages, 1 figure, to appear in the proceedings of "From X-ray binaries to quasars: Black hole accretion on all mass scales, (Amsterdam, July 2004)", Eds. T. Maccarone, R. Fender, L. H

    Implications of very rapid TeV variability in blazars

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    We discuss the implications of rapid (few-minute) variability in the TeV flux of blazars, which has been observed recently with the HESS and MAGIC telescopes. The variability timescales seen in PKS 2155-304 and Mrk 501 are much shorter than inferred light-crossing times at the black hole horizon, suggesting that the variability involves enhanced emission in a small region within an outflowing jet. The enhancement could be triggered by dissipation in part of the black hole's magnetosphere at the base of the outflow, or else by instabilities in the jet itself. By considering the energetics of the observed flares, along with the requirement that TeV photons escape without producing pairs, we deduce that the bulk Lorentz factors in the jets must be >50. The distance of the emission region from the central black hole is less well-constrained. We discuss possible consequences for multi-wavelength observations.Comment: 5 pages, no figures, accepted for publication in Monthly Notices of the Royal Astronomical Society Letter

    X-ray observations of the galaxy cluster PKS 0745-191: To the virial radius, and beyond

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    We measure X-ray emission from the outskirts of the cluster of galaxies PKS 0745-191 with Suzaku, determining radial profiles of density, temperature, entropy, gas fraction, and mass. These measurements extend beyond the virial radius for the first time, providing new information about cluster assembly and the diffuse intracluster medium out to ~1.5 r_200, (r_200 ~ 1.7 Mpc ~ 15'). The temperature is found to decrease by roughly 70 per cent from 0.3-1 r_200. We also see a flattening of the entropy profile near the virial radius and consider the implications this has for the assumption of hydrostatic equilibrium when deriving mass estimates. We place these observations in the context of simulations and analytical models to develop a better understanding of non-gravitational physics in the outskirts of the cluster.Comment: 10 pages, 11 figures, accepted to MNRAS; expanded discussion of analysis and uncertainties, results qualitatively unchange

    Allan Variance Analysis as Useful Tool to Determine Noise in Various Single-Molecule Setups

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    One limitation on the performance of optical traps is the noise inherently present in every setup. Therefore, it is the desire of most experimentalists to minimize and possibly eliminate noise from their optical trapping experiments. A step in this direction is to quantify the actual noise in the system and to evaluate how much each particular component contributes to the overall noise. For this purpose we present Allan variance analysis as a straightforward method. In particular, it allows for judging the impact of drift which gives rise to low-frequency noise, which is extremely difficult to pinpoint by other methods. We show how to determine the optimal sampling time for calibration, the optimal number of data points for a desired experiment, and we provide measurements of how much accuracy is gained by acquiring additional data points. Allan variances of both micrometer-sized spheres and asymmetric nanometer-sized rods are considered.Comment: 14 pages, 6 figures, presented at SPIE Optics+Photonics 2009 in San Diego, CA, US

    The Ultra-Fast Outflow of WKK 4438: Suzaku and NuSTAR X-ray Spectral Analysis

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    Previous X-ray spectral analysis has revealed an increasing number of AGNs with high accretion rates where an outflow with a mildly relativistic velocity originates from the inner accretion disk. Here we report the detection of a new ultra-fast outflow (UFO) with a velocity of vout=0.319βˆ’0.008+0.005cv_{\rm out}=0.319^{+0.005}_{-0.008}c in addition to a relativistic disk reflection component in a poorly studied NLS1 WKK~4438, based on archival \nustar and \suzaku observations. The spectra of both \suzaku and \nustar observations show an Fe~\textsc{xxvi} absorption feature and the \suzaku data also show evidence for an Ar~\textsc{xviii} with the same blueshift. A super-solar argon abundance (ZArβ€²>6ZβŠ™Z^{\prime}_{\rm Ar}>6Z_{\odot}) and a slight iron over-abundance (ZFeβ€²=2.6βˆ’2.0+1.9ZβŠ™Z^{\prime}_{\rm Fe}=2.6^{+1.9}_{-2.0}Z_{\odot}) are found in our spectral modelling. Based on Monte-Carlo simulations, the detection of the UFO is estimated to be around at 3Οƒ\sigma significance. The fast wind most likely arises from a radius of β‰₯20rg\geq20r_g away from the central black hole. The disk is accreting at a high Eddington ratio (Lbol=0.4βˆ’0.7LEddL_{\rm bol}=0.4-0.7L_{\rm Edd}). The mass outflow rate of the UFO is comparable with the disk mass inflow rate (MΛ™out>30%MΛ™in\dot M_{\rm out}>30\%\dot M_{\rm in}), assuming a maximum covering factor. The kinetic power of the wind might not be high enough to have influence in AGN feedback (EΛ™wind/Lbolβ‰ˆ3βˆ’5%\dot E_{\rm wind}/L_{\rm bol}\approx 3-5\%) due to a relatively small column density (12βˆ’4+9Γ—102212^{+9}_{-4}\times10^{22}~cmβˆ’2^{-2}). However note that both the inferred velocity and the column density could be lower limits owing to the low viewing angle (i=23βˆ’2+3i=23^{+3}_{-2}∘^{\circ}).Comment: 7 pages, 3 figures, accepted by MNRA
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