RX J0142.0+2131.I.The Galaxy Content of an X-Ray-luminous Galaxy Cluster at z=0.28

The Astronomical Journal 130 (2005) 445-474

Authors:

RL Davies, Jordi Barr, Inger Jorgensen, Marcel Bergmann

The obscuration by dust of most of the growth of supermassive black holes

Nature 436 (2005) 666-669

Authors:

SG Rawlings, Alejo Martinez-Sansigre, Mark Lacy, Dario Fada

Formation of Structure in Molecular Clouds: A Case Study

ArXiv astro-ph/0507567 (2005)

Authors:

F Heitsch, A Burkert, L Hartmann, AD Slyz, JEG Devriendt

Abstract:

Molecular clouds (MCs) are highly structured and ``turbulent''. Colliding gas streams of atomic hydrogen have been suggested as a possible source of MCs, imprinting the filamentary structure as a consequence of dynamical and thermal instabilities. We present a 2D numerical analysis of MC formation via converging HI flows. Even with modest flow speeds and completely uniform inflows, non-linear density perturbations as possible precursors of MCs arise. Thus, we suggest that MCs are inevitably formed with substantial structure, e.g., strong density and velocity fluctuations, which provide the initial conditions for subsequent gravitational collapse and star formation in a variety of galactic and extragalactic environments.

Formation of Structure in Molecular Clouds: A Case Study

(2005)

Authors:

F Heitsch, A Burkert, L Hartmann, AD Slyz, JEG Devriendt

The 2dF QSO redshift survey-XV. Correlation analysis of redshift-space distortions

Monthly Notices of the Royal Astronomical Society 360:3 (2005) 1040-1054

Authors:

J Da Ângela, PJ Outram, T Shanks, BJ Boyle, SM Croom, NS Loaring, L Miller, RJ Smith

Abstract:

We analyse the redshift-space (z-space) distortions of quasi-stellar object (QSO) clustering in the 2-degree field instrument (2dF) QSO Redshift Survey (2QZ). To interpret the z-space correlation function, ξ(σ, π), we require an accurate model for the QSO real-space correlation function, ξ(r). Although a single power-law ξ(r) ξ r-γ model fits the projected correlation function [wp(σ)] at small scales, it implies somewhat too shallow a slope for both wp(σ) and the z-space correlation function, ξ(s), at larger scales (≳20 h-1 Mpc). Motivated by the form for ξ(r) seen in the 2dF Galaxy Redshift Survey (2dFGRS) and in standard A cold dark matter (COM) predictions, we use a double power-law model for ξ(r), which gives a good fit to ξ(s) and w p(σ). The model is parametrized by a slope of γ = 1.45 for 1 < r < 10 h-1 Mpc and γ = 2.30 for 10 < r < 40 h-1 Mpc. As found for the 2dFGRS, the value of β determined from the ratio of ξ(s)/ξ(r) depends sensitively on the form of ξ(r) assumed. With our double power-law form for ξ(r), we measure β(z = 1.4) = 0.32-0.11+0.09. Assuming the same model for ξ(r), we then analyse the z-space distortions in the 2QZ ξ(σ, π) and put constraints on the values of Ωm0 and β(z = 1.4), using an improved version of the method of Hoyle et al. The constraints we derive are Ωm0 = 0.35-0.13+0.19, β(z = 1.4) = 0.50-0.15+0.13 in agreement with our ξ(s)/ξ(r) results at the ∼1σ level. © 2005 RAS.