2009MNRAS.396..385K


Query : 2009MNRAS.396..385K

2009MNRAS.396..385K - Mon. Not. R. Astron. Soc., 396, 385-401 (2009/June-2)

A search for HI 21cm absorption in strong Mg II absorbers in the redshift desert.

KANEKAR N., PROCHASKA J.X., ELLISON S.L. and CHENGALUR J.N.

Abstract (from CDS):

We report results from a deep search for redshifted Hi 21cm absorption in 55 strong Mgiiλ2796 absorbers (having Wλ27960 > 0.5Å) at intermediate redshifts, 0.58 < zabs< 1.70, with the Green Bank Telescope (GBT) and the Giant Metrewave Radio Telescope (GMRT). Nine detections of Hi 21cm absorption were obtained, all at 1.17 < zabs < 1.68, including three systems reported earlier by Gupta et al. (2007). Absorption was not detected at >3σ significance in 32 other Mgii absorbers, with 26 of these providing strong upper limits to the Hi 21cm optical depth, τ< 0.013 per ∼10km/s. For the latter 26 systems, the spin temperature Ts of the absorber must be >[800 xf] K (where f is the covering factor), if the Hi column density is ≥2x1020/cm2, i.e. if the absorber is a damped Lyman α system (DLA). Data on the remaining 13 systems of the sample were affected by radio frequency interference and were hence not useful.

Two of the Mgii absorbers, at zabs∼ 1.4106 towards 2003-025 and at zabs∼ 0.9115 towards 2149+212, are known DLAs. We detect Hi 21cm absorption towards 2003-025 with the GMRT and estimate the spin temperature of the DLA to be Ts = [(905±380)xf] K. Conversely, the GBT observations of 2149+212 resulted in a non-detection of Hi 21cm absorption, yielding the 3σ limit Ts> [2700xf] K.

Excluding `associated' systems (within 3000km/s of the quasar redshift), the detection rate of Hi 21cm absorption in strong Mgiiλ2796 absorbers is per cent, at a 3σ optical depth sensitivity of ∼0.013 per 10km/s. Comparing the detection rates of Hi 21cm and damped Lyman α absorption in strong Mgii absorber samples yields a detection rate of Hi 21cm absorption in DLAs of per cent, consistent with the detection rate in low-z DLAs. Since Hi 21cm absorption arises in cold neutral gas, this indicates that most gas-rich galaxies contain significant fractions of cold Hi by z ∼ 1.

Finally, we use the observed detection rate of Hi 21cm absorption in Mgii absorbers to infer the cosmological mass density of neutral gas in DLAs, assuming that (1) the average Hi column density in our Hi 21cm absorber sample is the same as that measured by Rao, Turnshek & Nestor in their DLA sample and (2) the detection rate of Hi 21cm absorption in the DLAs of our Mgii sample is the same as that in known DLAs at 0.09 < zabs< 3.45. We obtain ΩGAS∼ (0.55+0.42–0.22) x10–3, at, slightly lower than, but consistent with, the value obtained by Rao, Turnshek & Nestor from their DLA survey at similar redshifts.


Abstract Copyright: © 2009 The Authors. Journal compilation © 2009 RAS

Journal keyword(s): galaxies: evolution - galaxies: ISM - radio lines: galaxies

Simbad objects: 57

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Number of rows : 57
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 6C 001403+811827 BLL 00 17 08.47489694 +81 35 08.1365094   17.60 16.52 15.95   ~ 389 1
2 2C 26 BLL 00 20 25.2231670656 +15 40 54.774271884   17.92 17.62     ~ 342 1
3 QSO B0039-407 QSO 00 42 01.2251121648 -40 30 39.739745232   18.5 18.5 19.3   ~ 30 0
4 4C -01.06 QSO 01 08 26.8423531848 -00 37 24.164003640   18.11 17.82     ~ 135 1
5 4C 17.09 QSO 01 11 49.8456722808 +17 53 51.069035508     18.0     ~ 72 1
6 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2815 2
7 QSO B0237-2322 QSO 02 40 08.1743783856 -23 09 15.729012036   16.78 16.63     ~ 505 0
8 QSO B0240-060 QSO 02 43 12.46947413 -05 50 55.2953784   18.2 19.0 19.11   ~ 63 1
9 QSO B0244-128 BLL 02 46 58.4699862120 -12 36 30.796050528   18.5 18.4 18.28   ~ 60 1
10 3C 82 QSO 03 14 43.6 +43 14 05     21.0     ~ 51 2
11 [VV2006] J041149.7-042415 QSO 04 11 49.6935145848 -04 24 15.048820908   19.93 19.76     ~ 26 1
12 4C 09.17 QSO 04 48 21.73843453 +09 50 51.4600564   20.2 19.55     ~ 82 1
13 4C -02.19 QSO 05 01 12.80988538 -01 59 14.2564557   19.1 18.06 19.04   ~ 585 1
14 ICRF J054236.1+495107 Sy1 05 42 36.13789710 +49 51 07.2337139   18.45 17.80 17.210   ~ 1493 1
15 7C 064253.00+445430.00 QSO 06 46 32.02599653 +44 51 16.5901185   19.57 18.49 18.64   ~ 348 1
16 7C 074143.50+292721.00 Bla 07 44 51.3643230792 +29 20 06.038217348   17.20 16.97 16.4   ~ 54 1
17 4C 30.13 QSO 08 04 42.2368690344 +30 12 37.030825404   18.56 18.17     ~ 81 1
18 7C 080458.39+495918.00 QSO 08 08 39.66628970 +49 50 36.5304041   19.55 19.18 18.34   ~ 362 2
19 3C 196 Sy1 08 13 36.0561170112 +48 13 02.644966020   18.36 17.79     ~ 551 2
20 7C 081224.00+331441.00 QSO 08 15 34.1618573256 +33 05 29.012497692   19.55 19.25     ~ 57 1
21 4C 39.23A Bla 08 24 55.48385834 +39 16 41.9040476   18.55 18.21 17.20   ~ 213 1
22 7C 082926.39+423515.00 QSO 08 32 48.4358591616 +42 24 58.906002744   19.34 18.99     ~ 40 1
23 QSO J0850+5159 QSO 08 50 42.2440214784 +51 59 11.650187472   19.92 19.41     ~ 47 1
24 QSO J0852+3435 QSO 08 52 44.7398043240 +34 35 40.525493604   20.42 19.70     ~ 38 1
25 US 1139 QSO 09 58 19.67164698 +47 25 07.8424065   18.78 18.62 18.39   ~ 240 1
26 4C 00.34 QSO 10 00 17.6727030648 +00 05 23.704002492   19.61 19.41     ~ 149 1
27 8C 0958+561 QSO 10 01 20.6918953728 +55 53 55.593949272   17.16 16.95     ~ 735 3
28 QSO B1005-333 BLL 10 07 31.38745248 -33 33 06.7169760   20.18 18.0 19.80   ~ 51 1
29 4C 28.25 QSO 10 14 35.6898933624 +27 49 03.438825240   18.72 18.43     ~ 68 1
30 4C 02.30 QSO 10 15 15.6398810616 +01 58 53.226956424   17.75 17.40     ~ 66 1
31 4C 12.39 Bla 11 18 57.30143432 +12 34 41.7179609   19.39 19.25 19.10   ~ 258 1
32 7C 113623.30+404933.00 QSO 11 39 02.73424186 +40 32 54.8414557   20.42 20.25     ~ 45 1
33 4C 05.52 QSO 11 45 21.31516115 +04 55 26.6880160   19.69 19.26 18.67   ~ 94 1
34 QSO B1200+0651 QSO 12 03 01.01264266 +06 34 41.5375798   20.32 19.67     ~ 52 1
35 6C 120402+395719 QSO 12 06 37.0532372328 +39 41 03.748793640   19.10 18.71     ~ 57 1
36 4C 13.46 QSO 12 13 32.1707286888 +13 07 20.905849740   18.87 18.53 18   ~ 136 1
37 6C 122223+435147 BLL 12 24 51.50530154 +43 35 19.2873713   21.12 20.66 20.2   ~ 79 3
38 LBQS 1226+1035 QSO 12 28 36.8792519112 +10 18 41.954083020   19.33 19.12     ~ 102 1
39 QSO B1318-263 QSO 13 21 14.03692236 -26 36 10.4646221   21.10   21.4   ~ 38 1
40 QSO B1324-047 QSO 13 26 54.61394860 -05 00 58.9732821     19.00 19.67   ~ 35 1
41 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4341 2
42 4C 38.37 QSO 13 45 36.9420854112 +38 23 12.500014308     18.5     ~ 94 1
43 7C 1354+2552 QSO 13 57 06.5354509152 +25 37 24.494694024   19.13 18.93     ~ 100 1
44 QSO B1402-012 BLL 14 04 45.89545125 -01 30 21.9471571   18.70 18.45 17.9   ~ 169 1
45 QSO B1430-178 QSO 14 32 57.69062795 -18 01 35.2488081   17.8 19.5 18.4   ~ 90 1
46 2MASX J16045246+2402423 Sy1 16 04 52.4589508560 +24 02 41.678729304   17.1       ~ 30 0
47 6C 161147+342017 QSO 16 13 41.06424322 +34 12 47.9088535   17.98 17.46 17.07   ~ 642 1
48 4C 23.43 Sy1 16 24 39.0838297968 +23 45 12.223370412   17.91 17.47     ~ 339 1
49 SDSS J162733.42+260602.1 QSO 16 27 33.4214524416 +26 06 02.195284284   18.79 18.59     ~ 23 1
50 4C 12.59 QSO 16 31 45.1708807968 +11 56 03.203387592   18.38 18.40     ~ 122 1
51 [VV2006] J163638.1+211255 QSO 16 36 38.1837507672 +21 12 55.597804020   19.86 19.69 18.70   ~ 64 1
52 7C 1701+5919 QSO 17 02 20.0625479448 +59 15 38.655742284   20.14 19.70     ~ 35 1
53 4C -02.79 QSO 20 06 08.4469088568 -02 23 34.972947204     19     ~ 55 1
54 4C 21.59 QSO 21 51 45.8862336840 +21 30 13.743231624     19     ~ 67 1
55 QSO B2149-306 Bla 21 51 55.52396937 -30 27 53.6980880   17.95 18.0 17.48   ~ 260 1
56 QSO J2340-0053 QSO 23 40 23.6700032496 -00 53 27.001299696   18.26 17.93     ~ 103 0
57 QSO J2358-1020 QSO 23 58 10.88239662 -10 20 08.6114174   19.16 18.91 18.00   ~ 153 0

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