Distinguishing local and global influences on galaxy morphology: A Hubble Space Telescope comparison of high and low X-ray luminosity clusters
Astrophysical Journal 566:1 I (2002) 123-136
Abstract:
We present a morphological analysis of 17 X-ray-selected clusters at z ∼ 0.25, imaged uniformly with the Hubble Space Telescope Wide Field Planetary Camera 2 (WFPC2). Eight of these clusters comprise a subsample selected for their low X-ray luminosities (≲1044 ergs s -1), called the low-Lx sample. The remaining nine clusters comprise a high-Lx subsample with Lx > 10 45 ergs s-1. The two subsamples differ in their mean X-ray luminosity by a factor of 30 and span a range of more than 300. The clusters cover a relatively small range in redshift (z = 0.17-0.3, σ z/Z ∼ 0.15), and the data are homogeneous in terms of depth, resolution (0″.17 = 1 h50-1 kpc at z = 0.25), and rest wavelength observed, minimizing differential corrections from cluster to cluster. We fit the two-dimensional surface brightness profiles of galaxies down to very faint absolute magnitudes, M702 ≤, -18.2 + 5 log h50 (roughly 0.01L*R) with parametric models, and quantify their morphologies using the fractional bulge luminosity (B/T). Within a single WFPC2 image, covering a field of ∼ 3′ (1h50-1 Mpc at z = 0.25) in the cluster center, we find that the low-Lx clusters are dominated by galaxies with low B/T (∼ 0), while the high-Lx clusters are dominated by galaxies with intermediate B/T (∼ 0.4). We test whether this difference could arise from a universal morphology-density relation due to differences in the typical galaxy densities in the two samples. We find that small differences in the B/T distributions of the two samples persist with marginal statistical significance (98% confidence based on a binned Χ2 test) even when we restrict the comparison to galaxies in environments with similar projected local galaxy densities. A related difference (also of low statistical significance) is seen between the bulge-luminosity functions of the two cluster samples, while no difference is seen between the disk luminosity functions. From the correlations between these quantities, we argue that the global environment affects the population of bulges, over and above trends seen with local density. On the basis of this result, we conclude that the destruction of disks through ram pressure stripping or harassment is not solely responsible for the morphology-density relation and that bulge formation is less efficient in low-mass clusters, perhaps reflecting a less rich merger history.Merger histories in warm dark matter structure formation scenarios
Monthly Notices of the Royal Astronomical Society 329:4 (2002) 813-828
Gemini-north multiobject spectrograph: Integral field unit
Proceedings of SPIE the International Society for Optical Engineering 4841:3 (2002) 1750-1759
Abstract:
The Gemini-North Multiobject Spectrograph (CMOS) includes a powerful capability for integral field spectroscopy - the first to be installed and used on an 8-10m telescope. CMOS is switched to this mode by the remote insertion of an integral field unit (IFU) into the focal plane in place of the masks used for multiobject spectroscopy. With 1500 lenslet-coupled fibres, it provides a total field of view exceeding 50 square arcseconds, including a separate field dedicated to background subtraction. We describe the design, construction and testing of the IFU and present performance results obtained during commissioning.Integral field spectroscopy with the Gemini multiobject spectrograph. I. Design, construction, and testing
Publications of the Astronomical Society of the Pacific 114:798 (2002) 892-912
Abstract:
The Gemini Multiobject Spectrograph (GMOS) installed on the Gemini-North telescope has a facility for integral field spectroscopy over the wavelength range 0.4-1.0 μm. GMOS is converted to this mode by the remote insertion of an integral field unit (IFU) into the beam in place of the masks used for the multiobject mode. With the IFU deployed, integral field spectroscopy is available over a fully filled contiguous field of 5″ × 7″ with a sampling of 0″.2. A separate field of half the area, but otherwise identical, is also provided to improve background subtraction. The IFU contains 1500 lenslet-coupled fibers and is the first facility of any type for integral field spectroscopy employed on an 8-10 m telescope. We describe the design, construction, and testing of the GMOS IFU and present measurements of the throughput both in the laboratory and at the telescope. We compare these with a theoretical prediction made before construction started. All are in good agreement with each other, with the on-telescope throughput exceeding 60% (averaged over wavelength). A second paper will verify the scientific performance by comparison with existing one- and two-dimensional data sets.MUSE, a second-generation integral-field spectrograph for the VLT
Proceedings of SPIE the International Society for Optical Engineering 4841:2 (2002) 1096-1107