2010MNRAS.405.1888S


Query : 2010MNRAS.405.1888S

2010MNRAS.405.1888S - Mon. Not. R. Astron. Soc., 405, 1888-1900 (2010/July-1)

Detection of 21-cm, H2 and deuterium absorption at z > 3 along the line of sight to J1337+3152.

SRIANAND R., GUPTA N., PETITJEAN P., NOTERDAEME P. and LEDOUX C.

Abstract (from CDS):

We report the detection of 21-cm and molecular hydrogen absorption lines in the same damped Lyman α system (DLA; with log N(Hi) = 21.36±0.10) at zabs= 3.17447 towards SDSS J133724.69+315254.5 (zem∼ 3.174). We estimate the spin temperature of the gas to be TS= 600+222–159K, intermediate between the expected values for cold and warm neutral media. This suggests that the Hi absorption originates from a mixture of different phases. The total molecular fraction is low, , and H2 rotational level populations are not in equilibrium. The average abundance of the α-elements is [S/H] = -1.45±0.22. Nitrogen and iron are found underabundant with respect to α-elements by ∼1.0 and ∼0.5dex, respectively. Using photoionization models we conclude that the gas, of mean density nH∼ 2/cm3, is located more than 270kpc away from the quasi-stellar object. While the position of the 21-cm absorption line coincides with the H2 velocity profile, its centroid is shifted by ∼ 2.7±1.0 km/s^ with respect to the redshift measured from the H2lines. However, the position of the strongest metal absorption component matches the position of the 21-cm absorption line within 0.5 km/s. From this, we constrain the variation of the combination of fundamental constants x = α2 Gp/µ, Δ x/x = - (1.7±1.7)x10–6. This system is unique as we can at the same time have an independent constraint on µ using H2lines. However, as the H2 column density is low, only Werner band absorption lines are seen and, unfortunately, the range of sensitivity coefficients is too narrow to provide a stringent constraint: Δµ/µ ≤ 4.0x10–4. The Ultraviolet and Visual Echelle Spectrograph spectrum reveals another DLA at zabs= 3.16768 with log N(Hi) = 20.41 ±0.15 and low metallicity, [Si/H] = -2.68±0.11, in which [O/C] ∼0.18 ±0.18 and [O/Si] ∼ 0. This shows that even in the very early stages of chemical evolution, the carbon or silicon to oxygen ratios can be close to solar. Using Voigt profile fitting we derive log(N(Di)/N(Hi)) = -(4.93±0.15) in this system. This is a factor of 2 smaller than the value expected from the best-fitting value of Ωb from the Wilkinson Microwave Anisotropy Probe 5-yr data. This confirms the presence of astration of deuterium even at very low metallicity.

Abstract Copyright: © 2010 The Authors. Journal compilation © 2010 RAS

Journal keyword(s): galaxies: abundances - quasars: absorption lines - quasars: individual: SDSS J133724.69+315254.5

Simbad objects: 13

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Number of rows : 13
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 QSO B0027-1836 QSO 00 30 23.6259434280 -18 19 56.117225244   18.2 17.9     ~ 56 0
2 QSO B0347-383 QSO 03 49 43.6603590912 -38 10 30.825444900     17.3     ~ 196 0
3 QSO B0438-43 Bla 04 40 17.17997576 -43 33 08.6043290   19.31 19.5 18.2   ~ 302 2
4 QSO B0528-2505 Bla 05 30 07.9627395840 -25 03 29.900044512   18.17 17.34 17.7   ~ 429 1
5 CSO 38 QSO 10 11 55.5947671920 +29 41 41.595330804   16.28 16.05     ~ 117 0
6 LBQS 1232+0815 QSO 12 34 37.5514444464 +07 58 43.367750796     18.4     ~ 128 0
7 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
8 QSO B1331+170 Bla 13 33 35.7827544072 +16 49 04.013500728   16.84 16.71 16.41   ~ 469 1
9 QSO J1337+3152 QSO 13 37 24.6964232832 +31 52 54.575696928   19.40 19.01     ~ 58 1
10 QSO J1439+1117 BLL 14 39 12.0427245720 +11 17 40.563764052   19.27 18.92     ~ 77 1
11 QSO B1937-1009 BLL 19 39 57.2566747152 -10 02 41.522299692   18.800 19.0 17.188   ~ 207 1
12 LBQS 2206-1958A QSO 22 08 52.0729138920 -19 43 59.866776948   17.49 17.33     ~ 223 0
13 QSO J2340-0053 QSO 23 40 23.6700032496 -00 53 27.001299696   18.26 17.93     ~ 109 1

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