AEGIS: Infrared Spectroscopy of An Infrared Luminous Lyman Break Galaxy at z=3.01

(2006)

Authors:

J-S Huang, D Rigopoulou, C Papovich, MLN Ashby, SP Willner, R Ivison, ES Laird, T Webb, G Wilson, P Barmby, S Chapman, C Conselice, B Mcleod, CG Shu, HA Smith, E Le Floc'h, E Egami, CAN Willmer, G Fazio

The rapid formation of a large rotating disk galaxy three billion years after the Big Bang

Nature 442:7104 (2006) 786-789

Authors:

R Genzel, LJ Tacconi, F Eisenhauer, NM Förster Schreiber, A Cimatti, E Daddi, N Bouché, R Davies, MD Lehnert, D Lutz, N Nesvadba, A Verma, R Abuter, K Shapiro, A Sternberg, A Renzini, X Kong, N Arimoto, M Mignoli

Abstract:

Observations and theoretical simulations have established a framework for galaxy formation and evolution in the young Universe. Galaxies formed as baryonic gas cooled at the centres of collapsing dark-matter haloes; mergers of haloes and galaxies then led to the hierarchical build-up of galaxy mass. It remains unclear, however, over what timescales galaxies were assembled and when and how bulges and disks - the primary components of present-day galaxies - were formed. It is also puzzling that the most massive galaxies were more abundant and were forming stars more rapidly at early epochs than expected from models. Here we report high-angular-resolution observations of a representative luminous star-forming galaxy when the Universe was only 20% of its current age. A large and massive rotating protodisk is channelling gas towards a growing central stellar bulge hosting an accreting massive black hole. The high surface densities of gas, the high rate of star formation and the moderately young stellar ages suggest rapid assembly, fragmentation and conversion to stars of an initially very gas-rich protodisk, with no obvious evidence for a major merger. © 2006 Nature Publishing Group.

Star formation and figure rotation in the early-type galaxy NGC2974

(2006)

Authors:

Hyunjin Jeong, Martin Bureau, Sukyoung Ken Yi, Davor Krajnovic, Roger L Davies

New constraints on the co-moving star formation rate in the redshift interval 6<z<10

Proceedings of the International Astronomical Union 2:14 (2006) 251

Authors:

RS Ellis, DP Stark, J Richard, AJ Bunker, EE Egami, JP Kneib

Abstract:

Recent progress in measuring the optical depth of neutral hydrogen in distant quasars and that of electron scattering of microwave background photons suggests that most of the sources responsible for cosmic re-ionisation probably lie in the redshift interval 6 to 10. We present two new observational results which, together, provide valuable constraints on the contribution from star-forming sources in this redshift interval. First, using a large sample of v-band dropouts with unconfused Spitzer-IRAC detections, we determine the integrated stellar mass density at z = 5. This provides a valuable integral constraint on past star formation. It seems difficult to reconcile the observed stellar mass at z = 5 with the low abundance of luminous i-z- and J-band dropouts in deep Hubble Space Telescope data. Accordingly, we explore whether less luminous star-forming sources in the redshift interval 6 to 10 might be the dominant cause of cosmic re-ionization. In the second component of our research, we report on the results of two surveys for weak Lyman emitters and z- and J-band dropouts highly-magnified by foreground lensing clusters. Although some promising z = 89 candidates are found, it seems unlikely that low luminosity sources in this redshift interval can dominate cosmic reionization. If our work is substantiated by more extensive and precise surveys, the bulk of the re-ionizing photons may come from yet earlier sources lying at redshifts z>10. © 2007 International Astronomical Union.

Non-Standard Structure Formation Scenarios

Astrophysics and Space Science Kluwer Academic Publishers 284 (2006) 335-340

Authors:

A Knebe, B Little, R Islam, J Devriendt, A Mahmood, J Silk

Abstract:

Observations on galactic scales seem to be in contradiction with recent high resolution N-body simulations. This so-called cold dark matter (CDM) crisis has been addressed in several ways, ranging from a change in fundamental physics by introducing self-interacting cold dark matter particles to a tuning of complex astrophysical processes such as global and/or local feedback. All these efforts attempt to soften density profiles and reduce the abundance of satellites in simulated galaxy halos. In this contribution we are exploring the differences between a Warm Dark Matter model and a CDM model where the power on a certain scale is reduced by introducing a narrow negative feature (''dip''). This dip is placed in a way so as to mimic the loss of power in the WDM model: both models have the same integrated power out to the scale where the power of the Dip model rises to the level of the unperturbed CDM spectrum again. Using N-body simulations we show that that the new Dip model appears to be a viable alternative to WDM while being based on different physics: where WDM requires the introduction of a new particle species the Dip stems from a non-standard inflationary period. If we are looking for an alternative to the currently challenged standard LCDM structure formation scenario, neither the LWDM nor the new Dip model can be ruled out with respect to the analysis presented in this contribution. They both make very similar predictions and the degeneracy between them can only be broken with observations yet to come.