1998ApJ...506....1W


Query : 1998ApJ...506....1W

1998ApJ...506....1W - Astrophys. J., 506, 1-18 (1998/October-2)

The Hubble space telescope quasar absorption line key project. XIV. The evolution of Lyα absorption lines in the redshift interval z = 0-1.5.

WEYMANN R.J., JANNUZI B.T., LU L., BAHCALL J.N., BERGERON J., BOKSENBERG A., HARTIG G.F., KIRHAKOS S., SARGENT W.L.W., SAVAGE B.D., SCHNEIDER D.P., TURNSHEK D.A. and WOLFE A.M.

Abstract (from CDS):

We present the results of an analysis of the rate of evolution of the Lyα absorption lines in the redshift interval 0.0 to ∼1.5 based upon a sample of 987 Lyα absorption lines identified in the spectra of 63 QSOs obtained with the Faint Object Spectrograph (FOS) of the Hubble Space Telescope (HST). These spectra were obtained as part of the QSO Absorption Line Survey, an HST Key Project during the first four years of observations with the telescope. Fits to the evolution of the number of absorbers per unit redshift (dN/dz) of the form dN/dz = Ax(1 + z)γ continue to yield values of γ in the range 0.1-0.3, decidedly flatter than results from ground-based data pertaining to the redshift range z > 1.7. These results are consistent with our previous results based on a much smaller sample of lines, but the uncertainties in the fit have been greatly reduced. The combination of the HST and ground-based data suggest a marked transition in the rate of evolution of the Lyα lines at a redshift of about 1.7. The 19 Lyα lines from an additional higher redshift QSO from our sample for which tentative line identifications are available (UM 18; zem = 1.89) support the suggestion of a rapid increase at around this redshift. We derive the cumulative distribution of the full sample of Lyα lines and show that the distribution in redshift can indeed be well represented by a power law of the form (1 + z)γ. For this same sample, the distribution of equivalent widths of the Lyα absorbers above a rest equivalent width of 0.1 Å is fit quite well by an exponential. Comparing samples of Lyα lines, one set of which has redshifts the same as, or very near to, the redshifts of ions from heavy elements and another set in which no ions from heavy elements have been identified, we find that the Lyα systems with heavy element detections have a much steeper slope than the high rest equivalent width portion of the Lyman-only sample. We argue that this result is not likely to be due to either line misidentification or incomplete spectral coverage. Considering the insensitivity of the equivalent width to large changes in the column density for saturated lines, we suggest that this result is probably attributable to rapid evolution of the very highest column density systems, rather than real differences in metallicity. We find evidence that the rate of evolution increases with increasing equivalent width. We compare our results for the variation of line density with redshift to recent numerical simulations of Lyα absorbers, in particular, to those of Riediger, Petitjean, & Mucket, which extend to zero redshift. We find fairly good agreement between these simulations and our results, though the rapid evolution we find in the Lyα systems containing heavy element ions is not predicted in their models. We speculate that these heavy element-containing Lyα systems involve those clouds closely associated with galaxies, whose column densities are too high and whose sizes are too small to be included in the Riediger et al. simulations. Our results for Lyα lines at the high end of our equivalent width distribution are compatible with the recent analysis of the absorber-galaxy correlation by Chen et al. For the weaker lines, however, our results suggest that whatever association exists between absorbers and galaxies is different from that for the stronger lines. We conclude with some suggestions for further observations.

Abstract Copyright:

Journal keyword(s): Cosmology: Observations - Galaxies: Intergalactic Medium - Galaxies: Quasars: Absorption Lines

Simbad objects: 65

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Number of rows : 65
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 QSO B0002+0507 BLL 00 05 20.2155845040 +05 24 10.802758572   16.56 16.21 16.26   ~ 183 1
2 ICRF J000559.2+160949 Sy1 00 05 59.2378545384 +16 09 49.021968096   16.51 16.40     ~ 290 1
3 QSO J0027+2241 QSO 00 27 15.3715301928 +22 41 58.067953764   16.90 16.57 15.60   ~ 89 1
4 QSO B0043+0354 Sy1 00 45 47.2231233240 +04 10 23.386759392   15.88 16.00     ~ 156 0
5 87GB 004432.0+030343 Sy1 00 47 05.9186531064 +03 19 54.784830324   16.2 16.37     ~ 146 2
6 QSO B0117+2118 QSO 01 20 17.2642359528 +21 33 46.197696168     16.1     ~ 127 0
7 QSO J0125-0006 Bla 01 25 28.8438355224 -00 05 55.930595964   16.92 16.64 16.30   ~ 294 1
8 ICRF J020157.1-113233 Sy1 02 01 57.1794759192 -11 32 33.435766068   16.54 16.40 16.073   ~ 215 1
9 4C -04.06 QSO 02 35 07.3418452008 -04 02 05.317096956   16.61 16.46 16.2   ~ 213 1
10 3C 95 Sy1 03 51 28.5673217616 -14 29 08.257870248 15.62 16.55 16.22     ~ 189 1
11 PKS 0405-123 Sy1 04 07 48.4309841856 -12 11 36.659928408   15.09 14.86 14.7   ~ 510 1
12 2E 962 Sy1 04 17 16.7842972416 -05 53 45.608035560   16.24 15.94 15.7   ~ 172 1
13 QSO J0441-4313 QSO 04 41 17.3385563928 -43 13 45.488722116   16.64 16.36 16.54 16.26 ~ 109 1
14 QSO B0624+6907 QSO 06 30 02.5051022520 +69 05 03.913837440   14.64 14.16     ~ 95 0
15 QSO J0635-7516 Bla 06 35 46.5079301472 -75 16 16.816418256   15.96 15.75 15.82   ~ 587 1
16 QSO J0743-6726 QSO 07 43 31.6117092000 -67 26 25.547011008   16.71 16.37     ~ 146 1
17 ICRF J074541.6+314256 Sy1 07 45 41.6715742128 +31 42 56.614217508   16.10 15.97     ~ 260 1
18 US 1867 Sy1 08 53 34.2440799000 +43 49 02.336647692   17.15 16.91     ~ 102 0
19 QSO B0916+512 QSO 09 19 57.6059812632 +51 06 09.542294028   16.47 16.41     ~ 65 0
20 PG 0953+414 Sy1 09 56 52.3931554992 +41 15 22.211247636 14.710 15.611 15.546 15.294 14.720 ~ 452 0
21 Ton 469 Sy1 09 58 20.9496221568 +32 24 02.208417372   15.88 15.78 15.51   ~ 425 1
22 ICRF J100306.7+681316 Sy1 10 03 06.7660298016 +68 13 16.811854896   16.28 15.92 15.3   ~ 66 1
23 Ton 28 Sy1 10 04 02.6102134920 +28 55 35.329310688   16.17 15.7     ~ 174 0
24 7C 100725.89+414711.00 Sy1 10 10 27.5274498072 +41 32 39.053861232   16.72 16.67     ~ 184 1
25 QSO B1008+1319 QSO 10 11 10.8547987008 +13 04 12.189722736   17.00 16.76     ~ 91 0
26 4C 06.41 BLL 10 41 17.16249940 +06 10 16.9237327   16.86 16.70 16.14   ~ 289 1
27 PG 1049-005 Sy1 10 51 51.4474066944 -00 51 17.707987476   15.98 15.78     ~ 179 0
28 [OKM2018] SWIFT J1104.8+7689 Sy1 11 04 13.8611496720 +76 58 58.194549084   15.70 15.72 15.40   ~ 543 1
29 ICRF J110715.0+162802 Sy1 11 07 15.0475336176 +16 28 02.244766584   15.91 15.70     ~ 166 1
30 Ton 1388 Sy1 11 19 08.6786220240 +21 19 17.987085948   14.91 14.80     ~ 466 0
31 QSO B1130+111 QSO 11 33 30.2985591648 +10 52 23.353505292   16.52 16.45     ~ 59 0
32 NAME Crt A Sy1 11 39 10.7025556152 -13 50 43.639196064   16.38 16.17 16.4   ~ 271 1
33 ICRF J113957.0+654749 Sy1 11 39 57.0254367168 +65 47 49.483232880   16.50 16.32     ~ 518 1
34 PG 1216+069 Sy1 12 19 20.9318278680 +06 38 38.467059252   15.68 15.65     ~ 285 0
35 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 5798 1
36 QSO J1244+1721B QSO 12 44 10.8247089768 +17 21 04.508869464   16.40 16.09     ~ 152 1
37 QSO B1248+401 QSO 12 50 48.3268288080 +39 51 39.458894760   16.62 16.19     ~ 137 0
38 QSO B1252+119 Bla 12 54 38.25561478 +11 41 05.8950431   16.99 16.64 16.76   ~ 272 1
39 NVSS J125953+335653 Rad 12 59 54.0 +33 56 54   20.9       ~ 18 1
40 LB 2522 Sy1 13 01 12.9250750776 +59 02 06.693816732   16.04 15.89     ~ 281 0
41 ICRF J130533.0-103319 Sy1 13 05 33.0150535680 -10 33 19.430383680   15.18 15.23 14.46   ~ 577 1
42 Ton 153 QSO 13 19 56.2320886176 +27 28 08.186323080   16.12 15.98     ~ 153 0
43 PB 4007 Sy1 13 36 02.0092074528 +17 25 13.092799188   16.50 16.33     ~ 92 0
44 QSO J1341+4123 QSO 13 41 00.7893930432 +41 23 14.130152880   17.04 16.76     ~ 130 0
45 QSO B1352+0106 QSO 13 54 58.6806746304 +00 52 10.898450652     16.0     ~ 76 0
46 [OKM2018] SWIFT J1357.0+1929 Sy1 13 57 04.4366598768 +19 19 07.371837768   16.33 16.03 15.3   ~ 455 2
47 QSO J1409+2618 QSO 14 09 23.9085820008 +26 18 21.056458176   16.07 15.74     ~ 191 0
48 QSO J1427-1203 QSO 14 27 38.1268790904 -12 03 49.949292420   16.91 16.49 17.19   ~ 74 1
49 ICRF J151443.0+365050 Sy1 15 14 43.0683049560 +36 50 50.355436776   17.11 17.01 15.83   ~ 411 1
50 PG 1538+47 Sy1 15 39 34.8103136784 +47 35 31.263874908   16.01 15.81     ~ 98 1
51 2E 3648 Sy1 16 20 21.8185395384 +17 36 23.952361176   16.53 16.41 20.5   ~ 417 2
52 QSO B1634+7037 QSO 16 34 28.9917184368 +70 31 32.393436960   14.90 14.66     ~ 268 0
53 3C 351.0 Sy1 17 04 41.3742408840 +60 44 30.520617000   15.65 15.40 15.30   ~ 757 1
54 ClG 1821+64 ClG 18 21 56.7276 +64 20 55.841           ~ 504 1
55 7C 1821+6419 Sy1 18 21 57.2130271440 +64 20 36.221312076   14.23 14.24     ~ 601 1
56 QSO B2128-123 BLL 21 31 35.2617909696 -12 07 04.795364172   16.33 16.11 15.87   ~ 455 1
57 4C 06.69 Bla 21 48 05.45866779 +06 57 38.6041877   16.85 16.47 15.06   ~ 676 1
58 QSO J2246-1206 QSO 22 46 18.23197022 -12 06 51.2775983   16.63 16.45 15.99   ~ 283 1
59 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 2845 2
60 4C 11.72 BLL 22 54 10.4214226080 +11 36 38.748083760   16.02 15.82     ~ 341 1
61 ICRF J230343.5-680737 Sy1 23 03 43.56459610 -68 07 37.4431119   16.26 16.38 17.68   ~ 83 1
62 PB 5235 QSO 23 04 44.9534365920 +03 11 45.917366280   15.44 15.8     ~ 104 0
63 QSO B2340-0339 QSO 23 42 56.6002743864 -03 22 26.269675248   16.53 16.02 16.28   ~ 89 1
64 ICRF J234636.8+093045 Sy1 23 46 36.8384562240 +09 30 45.514903032   16.23 15.97 15.99   ~ 320 2
65 QSO J2355-3357 QSO 23 55 25.7961480408 -33 57 55.218632328   18.32 16.4 17.10   ~ 61 1

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