2011MNRAS.414....2B


Query : 2011MNRAS.414....2B

2011MNRAS.414....2B - Mon. Not. R. Astron. Soc., 414, 2-27 (2011/June-2)

The VLT LBG redshift survey – I. Clustering and dynamics of ≈ 1000 galaxies at z ≈ 3.

BIELBY R.M., SHANKS T., WEILBACHER P.M., INFANTE L., CRIGHTON N.H.M., BORNANCINI C., BOUCHE N., HERAUDEAU P., LAMBAS D.G., LOWENTHAL J., MINNITI D., PADILLA N., PETITJEAN P. and THEUNS T.

Abstract (from CDS):

We present the initial imaging and spectroscopic data acquired as part of the Very Large Telescope (VLT) VIMOS Lyman-break galaxy Survey. UBR (or UBVI) imaging covers five ≈ 36 {x} 36 arcmin2 fields centred on bright z > 3 quasi-stellar objects (QSOs), allowing ≈ 21 000 2 < z < 3.5 galaxy candidates to be selected using the Lyman-break technique. We performed spectroscopic follow-up using VLT VIMOS, measuring redshifts for 1020 z > 2 Lyman-break galaxies and 10 z > 2 QSOs from a total of 19 VIMOS pointings. From the galaxy spectra, we observe a 625 ± 510 km/s velocity offset between the interstellar absorption and Lyman α emission-line redshifts, consistent with previous results. Using the photometric and spectroscopic catalogues, we have analysed the galaxy clustering at z ≈ 3. The angular correlation function, w(θ), is well fitted by a double power law with clustering scalelength, r0= 3.19+0.32–0.54h–1 Mpc and slope γ= 2.45 for r < 1 h–1 Mpc and r0= 4.37+0.43–0.55h–1 Mpc with γ= 1.61±0.15 at larger scales. Using the redshift sample we estimate the semiprojected correlation function, wp(σ), and, for a γ= 1.8 power law, find r0= 3.67+0.23–0.24h–1 Mpc for the VLT sample and r0= 3.98+0.14–0.15h–1 Mpc for a combined VLT+Keck sample. From ξ(s) and ξ(σ, π), and assuming the above ξ(r) models, we find that the combined VLT and Keck surveys require a galaxy pairwise velocity dispersion of ≈ 700 km/s, higher than ≈ 400 km/s assumed by previous authors. We also measure a value for the gravitational growth rate parameter of β(z= 3) = 0.48 ±0.17, again higher than that previously found and implying a low value for the bias of b= 2.06+1.1–0.5. This value is consistent with the galaxy clustering amplitude which gives b= 2.22±0.16, assuming the standard cosmology, implying that the evolution of the gravitational growth rate is also consistent with Einstein gravity. Finally, we have compared our Lyman-break galaxy clustering amplitudes with lower redshift measurements and find that the clustering strength is not inconsistent with that of low-redshift L* spirals for simple `long-lived' galaxy models.

Based on data obtained with the National Optical Astronomy Observatories (NOAO) Mayall 4-m Telescope at Kitt Peak National Observatory, USA (programme ID: 06A-0133), the NOAO Blanco 4-m Telescope at Cerro Tololo Inter-American Observatory, Chile (programme IDs: 03B-0162 and 04B-0022) and the European Southern Observatory (ESO) Very Large Telescope (VLT), Chile (programme IDs: 075.A-0683, 077.A-0612 and 079.A-0442). The VLT LBG Redshift Survey– II. Interactions between galaxies and the IGM at z∼ 3


Abstract Copyright: 2011 The Authors Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): intergalactic medium - galaxies: kinematics and dynamics - cosmology: observations - large-scale structure of Universe

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME Herschel Deep Field reg 00 22 33 +00 19.6           ~ 36 0
2 LBQS 0042-2627 QSO 00 44 33.9605081160 -26 11 19.711610520     17.67 18.5   ~ 54 0
3 QSO J0124+0044 QSO 01 24 03.7793700432 +00 44 32.745561900   19.71 18.71 17.9   ~ 101 0
4 QSO B0940-1050 QSO 09 42 53.5078384704 -11 04 25.931336376   16.96 16.6 16.6   ~ 102 0
5 QSO J1201+0116 QSO 12 01 44.3649782736 +01 16 11.740001304   18.09 17.74 17.4   ~ 66 2
6 QSO B2126-15 Bla 21 29 12.17589329 -15 38 41.0419083   17.61 17.3 17.3   ~ 521 1

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