Galactic star formation in parsec-scale resolution simulations

(2010)

Authors:

Leila C Powell, Frederic Bournaud, Damien Chapon, Julien Devriendt, Adrianne Slyz, Romain Teyssier

The C-Band All-Sky Survey: Instrument design, status, and first-look data

Proceedings of SPIE - The International Society for Optical Engineering 7741 (2010)

Authors:

OG King, C Copley, R Davies, R Davis, C Dickinson, YA Hafez, C Holler, JJ John, JL Jonas, ME Jones, JP Leahy, SJC Muchovej, TJ Pearson, ACS Readhead, MA Stevenson, AC Taylor

Abstract:

The C-Band All-Sky Survey (C-BASS) aims to produce sensitive, all-sky maps of diffuse Galactic emission at 5 GHz in total intensity and linear polarization. These maps will be used (with other surveys) to separate the several astrophysical components contributing to microwave emission, and in particular will allow an accurate map of synchrotron emission to be produced for the subtraction of foregrounds from measurements of the polarized Cosmic Microwave Background. We describe the design of the analog instrument, the optics of our 6.1 m dish at the Owens Valley Radio Observatory, the status of observations, and first-look data. © 2010 SPIE.

The Origin and Evolution of the Mass-Metallicity Relation using GalICS

ArXiv 1008.4158 (2010)

Authors:

Jeremy Sakstein, Antonio Pipino, Julien Devriendt, Roberto Maiolino

Abstract:

The GalICS (Galaxies in Cosmological Simulations) semi-analytical model of hierar- chical galaxy formation is used to investigate the effects of different galactic properties, including star formation rate (SFR) and outflows, on the shape of the mass metallic- ity relation and to predict the relation for galaxies at redshift z=2.27 and z=3.54. Our version of GalICS has the chemical evolution implemented in great detail and is less heavily reliant on approximations such as instantaneous recycling. We vary the model parameters controlling both the efficiency and redshift dependence of the SFR as well as the efficiency of supernova feedback. We find that the factors controlling the SFR influence the relation significantly at all redshifts and require a strong redshift dependence, proportional to 1+z, in order to reproduce the observed relation at the low mass end. Indeed, at any redshift, the predicted relation flattens out at the high mass end resulting in a poorer agreement with observations in this regime. We also find that variation of the parameters associated with outflows has a minimal effect on the relation at high redshift but does serve to alter its shape in the more recent past. We thus conclude that the relation is one between SFR and mass and that outflows are only important in shaping the relation at late times. When the relation is stratified by SFR it is apparent that the predicted galaxies with increasing stellar masses have higher SFRs, supporting the view that galaxy downsizing is the origin of the relation. Attempting to reproduce the observed relation, we vary the parameters controlling the efficiency of star formation and its redshift dependence and compare the predicted relations with Erb et al. (2006) at z=2.27 and Maiolino et al. (2008) at z=3.54 in order to find the best-fitting parameters. (Abridged)

The Origin and Evolution of the Mass-Metallicity Relation using GalICS

(2010)

Authors:

Jeremy Sakstein, Antonio Pipino, Julien Devriendt, Roberto Maiolino

Measuring the low mass end of the M - σ relation

AIP Conference Proceedings 1240 (2010) 215-218

Authors:

D Krajnović, RM McDermid, M Cappellari, RL Davies

Abstract:

We show that high quality laser guide star (LGS) adaptive optics (AO) observations of nearby early-type galaxies are possible when the tip-tilt correction is done by guiding on nuclei while the focus compensation due to the changing distance to the sodium layer is made 'open loop'. We achieve corrections such that 40% of flux comes from R<0.2 arcsec. To measure a black hole mass (M•) one needs integral field observations of both high spatial resolution and large field of view. With these data it is possible to determine the lower limit to M• even if the spatial resolution of the observations are up to a few times larger than the sphere of influence of the black hole. © 2010 American Institute of Physics.