Star formation in a multi-phase interstellar medium

Astrophysics and Space Science 284:2 (2003) 833-836

Authors:

A Slyz, J Devriendt, G Bryan, J Silk

Abstract:

This contribution reports on our first efforts to simulate a multiphase interstellar medium on a kiloparsec scale in three dimensions with the stars and gas modeled self-consistently. Starting from inhomogenous initial conditions, our closed box simulations follow the gas as it cools and collapses under its own self-gravity to form stars which eventually return material and energy back through supernovae explosions and winds.

Photometry and Spectroscopy of GRB 030329 and Its Associated Supernova 2003dh: The First Two Months

The Astrophysical Journal American Astronomical Society 599:1 (2003) 394-407

Authors:

T Matheson, PM Garnavich, KZ Stanek, D Bersier, ST Holland, K Krisciunas, N Caldwell, P Berlind, JS Bloom, M Bolte, AZ Bonanos, MJI Brown, WR Brown, ML Calkins, P Challis, R Chornock, L Echevarria, DJ Eisenstein, ME Everett, AV Filippenko, K Flint, RJ Foley, DL Freedman, Mario Hamuy, P Harding, NP Hathi, M Hicken, C Hoopes, C Impey, BT Jannuzi, RA Jansen, S Jha, J Kaluzny, S Kannappan, RP Kirshner, DW Latham, JC Lee, DC Leonard, W Li, KL Luhman, P Martini, H Mathis, J Maza, ST Megeath, LR Miller, D Minniti, EW Olszewski, M Papenkova, MM Phillips, B Pindor, DD Sasselov, R Schild, H Schweiker, T Spahr, J Thomas-Osip, I Thompson, D Weisz, R Windhorst, D Zaritsky

Top-down fragmentation of a warm dark matter filament

Monthly Notices of the Royal Astronomical Society 345:4 (2003) 1285-1290

Authors:

A Knebe, JEG Devriendt, BK Gibson, J Silk

Abstract:

We present the first high-resolution N-body simulations of the fragmentation of dark matter filaments. Such fragmentation occurs in top-down scenarios of structure formation, when the dark matter is warm instead of cold. In a previous paper, we showed that warm dark matter (WDM) differs from the standard cold dark matter (CDM) mainly in the formation history and large-scale distribution of low-mass haloes, which form later and tend to be more clustered in WDM than in CDM universes, tracing the filamentary structures of the cosmic web more closely. Therefore, we focus our computational effort in this paper on one particular filament extracted from a WDM cosmological simulation and compare in detail its evolution to that of the same CDM filament. We find that the mass distribution of the haloes forming via fragmentation within the filament is broadly peaked around a Jeans mass of a few 109 M ⊙, corresponding to a gravitational instability of smooth regions with an overdensity contrast around 10 at these redshifts. Our results confirm that WDM filaments fragment and form gravitationally bound haloes in a top-down fashion, whereas CDM filaments are built bottom-up, thus demonstrating the impact of the nature of the dark matter on dwarf galaxy properties.

The 2dF QSO Redshift Survey - XIII. A Measurement of Lambda from the QSO Power Spectrum

ArXiv astro-ph/0310873 (2003)

Authors:

PJ Outram, T Shanks, BJ Boyle, SM Croom, Fiona Hoyle, NS Loaring, L Miller, RJ Smith

Abstract:

We report on measurements of the cosmological constant, Lambda, and the redshift space distortion parameter beta=Omega_m^0.6/b, based on an analysis of the QSO power spectrum parallel and perpendicular to the observer's line of sight, from the final catalogue of the 2dF QSO Redshift Survey. We derive a joint Lambda - beta constraint from the geometric and redshift-space distortions in the power spectrum. By combining this result with a second constraint based on mass clustering evolution, we break this degeneracy and obtain strong constraints on both parameters. Assuming a flat cosmology and a Lambda cosmology r(z) function to convert from redshift into comoving distance, we find best fit values of Omega_Lambda=0.71^{+0.09}_{-0.17} and beta(z~1.4)=0.45^{+0.09}_{-0.11}. Assuming instead an EdS cosmology r(z) we find that the best fit model obtained, with Omega_Lambda=0.64^{+0.11}_{-0.16} and beta(z~1.4)=0.40^{+0.09}_{-0.09}, is consistent with the Lambda r(z) results, and inconsistent with a Lambda=0 flat cosmology at over 95 per cent confidence.

AGN Physics from QSO Clustering

ArXiv astro-ph/0310533 (2003)

Authors:

Scott Croom, Brian Boyle, Tom Shanks, Phil Outram, Robert Smith, Lance Miller, Nicola Loaring, Suzanne Kenyon, Warrick Couch

Abstract:

We review the current status of QSO clustering measurements, particular with respect to their relevance in understanding AGN physics. Measurements based on the 2dF QSO Redshift Survey (2QZ) find a scale length for QSO clustering of s_0=5.76(+0.17-0.27) h-1 Mpc at a redshift ~1.5, very similar to low redshift galaxies. There is no evidence of evolution in the clustering of QSOs from z~0.5 to z~2.2. This lack of evolution and low clustering amplitude suggests a short life time for AGN activity of the order ~10^6-10^7 years. Large surveys such at the 2QZ and SDSS also allow the the study of QSO environments in 3D for the first time (at least at low redshift), early results from this work seem to show no difference between the environments of QSOs and normal galaxies. Future studies e.g. measuring clustering as a function of black hole mass, and deep QSO surveys should provide further insight into the formation and evolution of AGN.