arXiv subjects

H. W. Rix

Publications and source records attributed to H. W. Rix.

23 records · Page 2Linked to original sources

arXiv2004

A comprehensive model for the Monoceros tidal stream

We have compiled an extensive dataset on potential parts of the Monoceros tidal stream and performed an exhaustive survey of dwarf galaxy semi-analytic orbits in order to constrain its orbital properties. The best-fit orbits are subsequently realized as self-consistent N-body simulations in order to reproduce the spatial and velocity distribution of satellite debris. We find that all kinematic and geometric constraints can be fit by a single stream allowing for multiple wraps. The orbital eccentricity and inclination of the progenitor are strongly constrained to be e = 0.10 \pm 0.05 and i = 25 \pm 5 deg. Ten new estimates of proper motions from the Sloan Digital Sky Survey (SDSS) clearly exclude all retrograde orbits. Particles lost by the satellite populate two, nearly concentric rings naturally explaining the detection of stream stars at both 6--8 kpc (Ibata et al. 2003, Newberg et al. 2003) and 12--18 kpc (the Tri/And stream; Rocha-Pinto et al. 2003) from the Sun. We have attempted to predict the present location of the Monoceros stream progenitor using different information: (i) the kinematical and spatial distribution of detections and (ii) the different mean metallicity in the innner and the outer rings. A current location at l ~ 245, b ~ -18., with a distance to the Sun r_s~15 kpc, reproduces the available constraints. The mass of the progenitor has been poorly determined due to the slow orbital decay. Similar fits have been obtained for masses (3-9)10^8 M_sun. Additionally, we have analyzed to possible common origin of the Canis Major dwarf and the Monoceros stream, unfortunately, without a conclusive result.

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arXiv2002

VLT observations of the z=6.28 quasar SDSS 1030+0524

We present new VLT spectroscopic observations of the most distant quasar known, SDSS J1030+0524 at z=6.28 which was recently discovered by the Sloan Digital Sky Survey. We confirm the presence of a complete Gunn-Peterson trough caused by neutral hydrogen in the intergalactic medium. There is no detectable flux over the wavelength range from 8450 to 8710 A. We set an improved limit on the drop of the flux level blueward of the Ly alpha line: a factor of > 200. Below 8450 A the spectrum shows a rise in flux, with a large fraction (> 60 %) of the total emission produced by few narrow features of transmitted flux. We discuss the obvious proximity effect around this quasar, with the presence of transmitted flux with many absorption features in a region of about 23h^{-1} comoving Mpc. If assuming the surrounding medium were completely neutral, the size of this region would imply a quasar lifetime of \~1.3x10^7 years. We also present near-IR spectroscopy of both SDSS J1030+0524 and of SDSS J1306+05, the second most distant quasar known at redshift 6.0. We combine measurements of the CIV line and limits on the HeII emission with the NV line measurements from the optical spectra to derive line ratios, and by implication the abundances of these early quasar environments. The results are indistinguishable from those of lower redshift quasars and indicate little or no evolution in the abundances from z ~ 6 to z ~ 2. The line ratios suggest supersolar metallicities, implying that the first stars around the quasars must have formed at least a few hundreds of Myrs prior to the observation, i.e. at redshift higher than 8.

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arXiv1997

Improved evidence for a black hole in M32 from HST/FOS spectra - II. Axisymmetric dynamical models

Axisymmetric dynamical models are constructed for the E3 galaxy M32 to interpret high spatial resolution stellar kinematical HST data. Models are studied with two-integral phase-space distribution functions, and with fully general three- integral distribution functions. The latter are built using a new extension of Schwarzschild's orbit superposition approach. Models are constructed for inclinations of 90 and 55 degrees. No model without a nuclear dark object can fit the combined ground-based and HST data, independent of the dynamical structure of M32. Models with a nuclear dark object of 3.4 x 10^6 solar masses do provide an excellent fit. The inclined models provide the best fit, but the inferred dark mass does not depend sensitively on the assumed inclination. The models that best fit the data are not two-integral models, but like two-integral models they are azimuthally anisotropic. An extended dark object can fit the data only if its half-mass radius is r_h < 0.08 arcsec (=0.26 pc), implying a central dark matter density exceeding 1 x 10^8 solar masses / pc^3. This density is high enough to rule out most plausible alternatives to a massive black hole. The dynamically inferred dark mass is identical to that suggested by existing adiabatic black hole growth models for HST photometry of M32. The low activity of M32 implies either that only a very small fraction of the gas that is shed by evolving stars is accreted onto the black hole, or that accretion proceeds at very low efficiency, e.g. in an advection-dominated mode. (shortened version)

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arXiv1997

Improved evidence for a black hole in M32 from HST/FOS spectra - I. Observations

We have obtained spectra through small apertures centered on the nuclear region and major axis of M32, with the HST/FOS. A detailed analysis and reduction of the data is presented, including: (i) new calibrations and modeling of the FOS aperture sizes, PSF and line-spread-functions; (ii) determination of the aperture positioning for each observation; and (iii) accurate wavelength calibration, template matching, and kinematical analysis of the spectra. This yields measurements of the stellar rotation velocities and velocity dispersions with five times higher spatial resolution than the best available ground-based data. The inferred velocities provide the highest angular resolution stellar kinematical data obtained to date for any stellar system. The observations show a steeper rotation curve and higher central velocity dispersion than ground-based data. The rotation velocity is observed to be 30 km/s at 0.1" from the nucleus; roughly twice the value measured from the ground at this distance. The nuclear dispersion measured through the smallest FOS aperture (0.068" square) is 156 +/- 10 km/s. The average of four independent dispersion measurements at various positions inside the central 0.1" is 126 km/s, with a RMS scatter of 21 km/s. The nuclear dispersion measured from the ground is only 85-95 km/s, whereas the dispersion outside the central arcsec is only 45-55 km/s. These results significantly strengthen previous arguments for the presence of a massive nuclear black hole in M32. Detailed dynamical models are presented in a series of companion papers.

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arXiv1997

New evidence for a massive black hole at the centre of the quiescent galaxy M32

Massive black holes are thought to reside at the centres of many galaxies, where they power quasars and active galactic nuclei. But most galaxies are quiescent, indicating that any central massive black hole present will be starved of fuel and therefore detectable only through its gravitational influence on the motions of the surrounding stars. M32 is a nearby, quiescent elliptical galaxy in which the presence of a black hole has been suspected; however, the limited resolution of the observational data and the restricted classes of models used to interpret this data have made it difficult to rule out alternative explanations, such as models with an anisotropic stellar velocity distribution and no dark mass or models with a central concentration of dark objects (for example, stellar remnants or brown dwarfs). Here we present high-resolution optical HST spectra of M32, which show that the stellar velocities near the centre of this galaxy exceed those inferred from previous ground-based observations. We use a range of general dynamical models to determine a central dark mass concentration of (3.4 +/- 1.6) x 10^6 solar masses, contained within a region only 0.3 pc across. This leaves a massive black hole as the most plausible explanation of the data, thereby strengthening the view that such black holes exist even in quiescent galaxies.

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