2,065 research outputs found

    Keck Spectroscopy of the Gravitational Lens System PG 1115+080: Redshifts of the Lensing Galaxies

    Get PDF
    The quadruple system PG 1115+080 is the second gravitational lens with a reported measurement of the Hubble constant. In addition to the primary lens, three nearby galaxies are believed to contribute significantly to the lensing potential. In this paper we report accurate redshifts for all four galaxies and show that they belong to a single group at z_d = 0.311. This group has very similar properties to Hickson's compact groups of galaxies found at lower redshifts. We briefly discuss implications for the existing lens models and derive H_0 = 52 +/- 14 km/s/Mpc.Comment: revised to use the updated model of Keeton & Kochanek (astro-ph/9611216) and to correct the velocity dispersion of the group; 10 pages including 2 eps figures and 2 tables. Submitted to the Astronomical Journa

    Angular Power Spectrum of the Microwave Background Anisotropy seen by the COBE Differential Microwave Radiometer

    Full text link
    The angular power spectrum estimator developed by Peebles (1973) and Hauser & Peebles (1973) has been modified and applied to the 2 year maps produced by the COBE DMR. The power spectrum of the real sky has been compared to the power spectra of a large number of simulated random skies produced with noise equal to the observed noise and primordial density fluctuation power spectra of power law form, with P(k)knP(k) \propto k^n. Within the limited range of spatial scales covered by the COBE DMR, corresponding to spherical harmonic indices 3 \leq \ell \lsim 30, the best fitting value of the spectral index is n=1.250.45+0.4n = 1.25^{+0.4}_{-0.45} with the Harrison-Zeldovich value n=1n = 1 approximately 0.5σ\sigma below the best fit. For 3 \leq \ell \lsim 19, the best fit is n=1.460.44+0.39n = 1.46^{+0.39}_{-0.44}. Comparing the COBE DMR ΔT/T\Delta T/T at small \ell to the ΔT/T\Delta T/T at 50\ell \approx 50 from degree scale anisotropy experiments gives a smaller range of acceptable spectral indices which includes n=1n = 1.Comment: 22 pages of LaTex using aaspp.sty and epsf.sty with appended Postscript figures, COBE Preprint 94-0

    Relative Flux Calibration of Keck HIRES Echelle Spectra

    Full text link
    We describe a new method to calibrate the relative flux levels in spectra from the HIRES echelle spectrograph on the Keck-I telescope. Standard data reduction techniques that transfer the instrument response between HIRES integrations leave errors in the flux of 5 - 10%, because the effective response varies. The flux errors are most severe near the ends of each spectral order, where there can be discontinuous jumps. The source of these errors is uncertain, but may include changes in the vignetting connected to the optical alignment. Our new flux calibration method uses a calibrated reference spectrum of each target to calibrate individual HIRES integrations. We determine the instrument response independently for each integration, and hence we avoid the need to transfer the instrument response between HIRES integrations. The procedure can be applied to any HIRES spectrum, or any other spectrum. While the accuracy of the method depends upon many factors, we have been able to flux calibrate a HIRES spectrum to 1% over scales of 200 A that include order joins. We illustrate the method with spectra of Q1243+3047 towards which we have measured the deuterium to hydrogen abundance ratio.Comment: 24 pages, 17 figures, submitted to PAS

    The Dipole Observed in the COBE DMR Four-Year Data

    Get PDF
    The largest anisotropy in the cosmic microwave background (CMB) is the 3\approx 3 mK dipole assumed to be due to our velocity with respect to the CMB. Using the four year data set from all six channels of the COBE Differential Microwave Radiometers (DMR), we obtain a best-fit dipole amplitude 3.358±0.001±0.0233.358 \pm 0.001 \pm 0.023 mK in the direction (l,b)=(264deg.31±0deg.04±0deg.16,+48deg.05±0deg.02±0deg.09)(l,b)=(264\deg.31 \pm 0\deg.04 \pm 0\deg.16, +48\deg.05 \pm 0\deg.02 \pm 0\deg.09), where the first uncertainties are statistical and the second include calibration and combined systematic uncertainties. This measurement is consistent with previous DMR and FIRAS resultsComment: New and improved version; to be published in ApJ next mont
    corecore