2,887 research outputs found

    The Extreme Ultraviolet Spectra of Low Redshift Radio Loud Quasars

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    This paper reports on the extreme ultraviolet (EUV) spectrum of three low redshift (z0.6z \sim 0.6) radio loud quasars, 3C 95, 3C 57 and PKS 0405-123. The spectra were obtained with the Cosmic Origins Spectrograph (COS) of the Hubble Space Telescope. The bolometric thermal emission, LbolL_{bol}, associated with the accretion flow is a large fraction of the Eddington limit for all of these sources. We estimate the long term time averaged jet power, Q\overline{Q}, for the three sources. Q/Lbol\overline{Q}/L_{bol}, is shown to lie along the correlation of Q/Lbol\overline{Q}/L_{bol} and αEUV\alpha_{EUV} found in previous studies of the EUV continuum of intermediate and high redshift quasars, where the EUV continuum flux density between 1100 \AA\, and 700 \AA\, is defined by FνναEUVF_{\nu} \sim \nu^{-\alpha_{EUV}}. The high Eddington ratios of the three quasars extends the analysis into a wider parameter space. Selecting quasars with high Eddington ratios has accentuated the statistical significance of the partial correlation analysis of the data. Namely. the correlation of Q/Lbol\overline{Q}/L_{\mathrm{bol}} and αEUV\alpha_{EUV} is fundamental and the correlation of Q\overline{Q} and αEUV\alpha_{EUV} is spurious at a very high statistical significance level (99.8\%). This supports the regulating role of ram pressure of the accretion flow in magnetically arrested accretion models of jet production. In the process of this study, we use multi-frequency and multi-resolution Very Large Array radio observations to determine that one of the bipolar jets in 3C 57 is likely frustrated by galactic gas that keeps the jet from propagating outside the host galaxy.Comment: To appear in MNRA

    Response of graphene to femtosecond high-intensity laser irradiation

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    We study the response of graphene to high-intensity 10^11-10^12 Wcm^-2, 50-femtosecond laser pulse excitation. We establish that graphene has a fairly high (~3\times10^12Wcm^-2) single-shot damage threshold. Above this threshold, a single laser pulse cleanly ablates graphene, leaving microscopically defined edges. Below this threshold, we observe laser-induced defect formation that leads to degradation of the lattice over multiple exposures. We identify the lattice modification processes through in-situ Raman microscopy. The effective lifetime of CVD graphene under femtosecond near-IR irradiation and its dependence on laser intensity is determined. These results also define the limits of non-linear applications of graphene in femtosecond high-intensity regime.Comment: 4 pages, 3 figure

    Magnetic-Field Amplification in the Thin X-ray Rims of SN1006

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    Several young supernova remnants (SNRs), including SN1006, emit synchrotron X-rays in narrow filaments, hereafter thin rims, along their periphery. The widths of these rims imply 50 to 100 μ\muG fields in the region immediately behind the shock, far larger than expected for the interstellar medium compressed by unmodified shocks, assuming electron radiative losses limit rim widths. However, magnetic-field damping could also produce thin rims. Here we review the literature on rim width calculations, summarizing the case for magnetic-field amplification. We extend these calculations to include an arbitrary power-law dependence of the diffusion coefficient on energy, DEμD \propto E^{\mu}. Loss-limited rim widths should shrink with increasing photon energy, while magnetic-damping models predict widths almost independent of photon energy. We use these results to analyze Chandra observations of SN 1006, in particular the southwest limb. We parameterize the full widths at half maximum (FWHM) in terms of energy as FWHM EγmE\propto E^{m_E}_{\gamma}. Filament widths in SN1006 decrease with energy; mE0.3m_E \sim -0.3 to 0.8-0.8, implying magnetic field amplification by factors of 10 to 50, above the factor of 4 expected in strong unmodified shocks. For SN 1006, the rapid shrinkage rules out magnetic damping models. It also favors short mean free paths (small diffusion coefficients) and strong dependence of DD on energy (μ1\mu \ge 1).Comment: Accepted by ApJ, 49 pages, 10 figure
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