2016MNRAS.456L..79B


Query : 2016MNRAS.456L..79B

2016MNRAS.456L..79B - Mon. Not. R. Astron. Soc., 456, L79-L83 (2016/February-2)

Constraining the temperature-density relation of the intergalactic medium with the Lyman α and β forests.

BOERA E., MURPHY M.T., BECKER G.D. and BOLTON J.S.

Abstract (from CDS):

The post-reionization thermal state of the intergalactic medium is characterized by a power-law relationship between temperature and density, with a slope determined by the parameter γ. We describe a new method to measure γ using the ratio of flux curvature in the Lyman α and β forests. At a given redshift, this curvature ratio incorporates information from the different gas densities traced by Lyman α and β absorption. It is relatively simple and fast to compute and appears robust against several observational uncertainties. We apply this technique to a sample of 27 high-resolution quasar spectra from the Very Large Telescope. While promising statistical errors on γ appear to be achievable with these spectra, to reach its full potential, the dependence of the curvature ratio on the thermal state of the gas in the foreground Lyman α forest will require further, detailed forward modelling.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

Journal keyword(s): intergalactic medium - quasars: absorption lines - cosmology: observations

Simbad objects: 27

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Number of rows : 27
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 J0003-2323 QSO 00 03 44.9144535192 -23 23 55.073021280     16.7     ~ 79 0
2 QSO B0055-26 QSO 00 57 58.0253990928 -26 43 14.750912928   17.90 17.47 17.99   ~ 152 1
3 QSO B0103-260 QSO 01 06 04.4059842336 -25 46 51.327250896   18.82 18.31   18.6 ~ 33 0
4 QSO B0109-353 QSO 01 11 43.6321128912 -35 03 00.587535660   16.6 16.9     ~ 79 0
5 QSO B0122-379 QSO 01 24 17.3720154480 -37 44 22.919854020     17.1     ~ 121 0
6 QSO J0140-0839 QSO 01 40 49.1830961952 -08 39 42.462483840   19.62 18.57     ~ 57 0
7 QSO J0142+0023 QSO 01 42 14.7480666240 +00 23 24.293809176   19.30 18.70     ~ 53 0
8 QSO J0153-4311 QSO 01 53 27.1920203376 -43 11 38.095833120     16.80     ~ 51 0
9 QSO B0237-2322 QSO 02 40 08.1743783856 -23 09 15.729012036   16.78 16.63     ~ 516 1
10 QSO B0329-385 QSO 03 31 06.3780612048 -38 24 04.653443772   17.63 16.92     ~ 85 1
11 QSO J0407-4410 QSO 04 07 18.0880236912 -44 10 13.983623724   17.6 17.6     ~ 103 1
12 QSO J0422-3844 BLL 04 22 14.7829521792 -38 44 52.826059032   17.70 16.92 16.3   ~ 203 2
13 QSO J0453-1305 QSO 04 53 13.5744238944 -13 05 55.085318988   13.2 16.5     ~ 94 2
14 QSO B0940-1050 QSO 09 42 53.5078384704 -11 04 25.931336376   16.96 16.6 16.6   ~ 102 0
15 QSO B1036-2257 QSO 10 39 09.5068714968 -23 13 26.396602392   18.0 18.0     ~ 46 0
16 PG 1101-264 QSO 11 03 25.2993421704 -26 45 15.808554720   16.08 16.02     ~ 247 1
17 QSO B1122-168 QSO 11 24 42.8658917592 -17 05 17.389038732   16.5 16.5 16.1   ~ 132 1
18 QSO B1142+1015 QSO 11 44 36.6559665072 +09 59 04.870692816   19.25 18.86     ~ 54 0
19 QSO J1155+0530 QSO 11 55 38.6022229320 +05 30 50.687047944   19.57 18.78     ~ 59 0
20 QSO B1158-1842 QSO 12 00 44.9451160128 -18 59 44.479378320   17.22 16.93     ~ 59 0
21 QSO B1448-232 QSO 14 51 02.5093156224 -23 29 31.107548184   17.13 16.96     ~ 135 2
22 SDSS J212329.46-005052.9 QSO 21 23 29.4639412848 -00 50 52.916363736   16.91 16.62     ~ 131 0
23 QSO B2126-15 Bla 21 29 12.17589329 -15 38 41.0419083   17.61 17.3 17.3   ~ 521 1
24 QSO J2220-2803 QSO 22 20 06.7591541688 -28 03 23.467479516     16.0 16.10   ~ 100 0
25 QSO B2332-094 QSO 23 34 46.4045250120 -09 08 12.250650732   19.21 18.62 18.07   ~ 89 1
26 QSO B2343+125 QSO 23 46 28.200 +12 49 00.00     17.5     ~ 143 2
27 QSO B2347-4342 QSO 23 50 34.2593744544 -43 25 59.683985652   16.3 16.3     ~ 172 0

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