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Theoretical physicists working at a blackboard collaboration pod in the Beecroft building.
Credit: Jack Hobhouse

Professor James Binney FRS

Emeritus Professor

Sub department

  • Rudolf Peierls Centre for Theoretical Physics

Research groups

  • Theoretical astrophysics and plasma physics at RPC
James.Binney@physics.ox.ac.uk
Telephone: 01865 (2)73979
Rudolf Peierls Centre for Theoretical Physics, room 50.3
  • About
  • Publications

Is there really a Black Hole at the center of NGC 4041? - Constraints from gas kinematics

ArXiv astro-ph/0211650 (2002)

Authors:

A Marconi, DJ Axon, A Capetti, W Maciejewski, J Atkinson, D Batcheldor, J Binney, M Carollo, L Dressel, H Ford, J Gerssen, MA Hughes, D Macchetto, MR Merrifield, C Scarlata, W Sparks, M Stiavelli, Z Tsvetanov, RP van der Marel

Abstract:

We present HST/STIS spectra of the Sbc spiral galaxy NGC 4041 which were used to map the velocity field of the gas in its nuclear region. We detect the presence of a compact (r~0.4" ~40 pc), high surface brightness, rotating nuclear disk co-spatial with a nuclear star cluster. The disk is characterized by a rotation curve with a peak to peak amplitude of ~40 km/s and is systematically blueshifted by 10 - 20 km/s with respect to the galaxy systemic velocity. With the standard assumption of constant mass-to-light ratio and with the nuclear disk inclination taken from the outer disk, we find that a dark point mass of 1(-0.7;+0.6) 10^7 Msun is needed to reproduce the observed rotation curve. However the observed blueshift suggests the possibility that the nuclear disk could be dynamically decoupled. Following this line of reasoning we relax the standard assumptions and find that the kinematical data can be accounted for by the stellar mass provided that either the central mass-to-light ratio is increased by a factor of ~2 or that the inclination is allowed to vary. This model results in a 3 sigma upper limit of 6 10^6 Msun on the mass of any nuclear black hole. Overall, our analysis only allows us to set an upper limit of 2 10^7 Msun on the mass of the nuclear black hole. If this upper limit is taken in conjunction with an estimated bulge B magnitude of -17.7 and with a central stellar velocity dispersion of 95 km/s, then these results are not inconsistent with both the MBH-Lsph and the MBH-sigma correlations. Constraints on black hole masses in spiral galaxies of types as late as Sbc are still very scarce and therefore the present result adds an important new datapoint to our understanding of black hole demography.

Radial mixing in galactic discs

Monthly Notices of the Royal Astronomical Society 336 (2002) 785-796

Authors:

JJ Binney, J.A. Sellwood

AGN as cosmic thermostats

ArXiv astro-ph/0210569 (2002)

Authors:

Christian R Kaiser, Marcus Brueggen, James J Binney

Abstract:

We present a simple analytical model and the results of numerical simulations supporting the idea of periodical heating of cluster gas by AGN outflows. We show why, under this assumption, we are extremely unlikely to observe clusters containing gas with a temperature below about 1 keV. We review the results from numerical hydro-simulations studying the mechanisms by which AGN outflows heat the cluster gas.

Two-body relaxation in cosmological simulations

Monthly Notices of the Royal Astronomical Society 333:2 (2002) 378-382

Authors:

J Binney, A Knebe

Abstract:

It is logically possible that early two-body relaxation in simulations of cosmological clustering influences the final structure of massive clusters. Convergence studies in which mass and spatial resolution are simultaneously increased cannot eliminate this possibility. We test the importance of two-body relaxation in cosmological simulations with simulations in which there are two species of particles. The cases of two mass ratios, √2:1 and 4:1, are investigated. Simulations are run with both a spatially fixed softening length and adaptive softening using the publicly available codes GADGET and MLAPM, respectively. The effects of two-body relaxation are detected in both the density profiles of haloes and the mass function of haloes. The effects are more pronounced with a fixed softening length, but even in this case they are not so large as to suggest that results obtained with one mass species are significantly affected by two-body relaxation. The simulations that use adaptive softening are less affected by two-body relaxation and produce slightly higher central densities in the largest haloes. They run about three times faster than the simulations that use a fixed softening length.

Observable consequences of cold clouds as dark matter

Monthly Notices of the Royal Astronomical Society 332:2 (2002) L29-L33

Authors:

E Kerins, J Binney, J Silk

Abstract:

Cold, dense clouds of gas have been proposed to explain the dark matter in Galactic haloes, and have also been invoked in the Galactic disc as an explanation for the excess faint submillimetre sources detected by SCUBA. Even if their dust-to-gas ratio is only a small percentage of that in conventional gas clouds, these dense systems would be opaque to visible radiation. We examine the possibility that the data sets of microlensing experiments searching for massive compact halo objects can also be used to search for occultation signatures by such clouds. We compute the rate and time-scale distribution of stellar transits by clouds in the Galactic disc and halo. We find that, for cloud parameters typically advocated by theoretical models, thousands of transit events should already exist within microlensing survey data sets. We examine the seasonal modulation in the rate caused by the Earth's orbital motion and find it provides an excellent probe of whether detected clouds are of disc or halo origin.

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