2024MNRAS.52712109B


Query : 2024MNRAS.52712109B

2024MNRAS.52712109B - Mon. Not. R. Astron. Soc., 527, 12109-12119 (2024/February-1)

Neutral carbon in diffuse interstellar medium: abundance matching with H2 for damped Lyman alpha systems at high redshifts.

BALASHEV S.A. and KOSENKO D.N.

Abstract (from CDS):

We present a study of C I/H2 relative abundance in the diffuse cold neutral medium (CNM). Using the chemical and thermal balance model, we calculate the dependence of C I/H2 on the main parameters of the medium: hydrogen number density, metallicity, strength of the UV field, and cosmic ray ionization rate (CRIR). We show that the observed relative C I and H2 column densities in damped Lyman alpha systems (DLAs) at high redshifts can be reproduced within our model assuming the typically expected conditions in the diffuse CNM. Using additional observed information on metallicity, H I column density, and excitation of C I fine-structure levels, as well as temperature, we estimated for a wide range metallicities in the CNM at high redshifts that CRIRs are in the range from ∼10–16 to a $\rm few \times 10^{-15}\, \rm s^{-1}$, hydrogen number densities are in the range ∼10-103 cm–3, and the UV field is in the range from 10–2 to a $\rm few \times 10^2$ of the Mathis field. We argue that because the observed quantities used in this work are quite homogeneous and much less affected by radiative transfer effects (in comparison with, for example, the dissociation of HD and UV pumping of H2 rotational levels), our estimates are quite robust against the assumption of the exact geometrical model of the cloud and local sources of the UV field.

Abstract Copyright: © 2024 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): ISM: abundances - ISM: cosmic rays - Cosmology: observations

Simbad objects: 19

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Number of rows : 19
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 SDSS J000015.17+004833.2 QSO 00 00 15.1760866776 +00 48 33.306387012           ~ 29 0
2 QSO B0027-1836 QSO 00 30 23.6259434280 -18 19 56.117225244   18.2 17.9     ~ 56 0
3 QSO J0812+32 QSO 08 12 40.6859242632 +32 08 08.579336496   18.16 17.75     ~ 106 0
4 SDSS J081634.38+144612.4 QSO 08 16 34.3904979384 +14 46 12.491066712   21.91 20.39     ~ 46 0
5 SDSS J084312.72+022117.2 QSO 08 43 12.7165734816 +02 21 17.341452360           ~ 24 0
6 SDSS J090609.45+054818.7 QSO 09 06 09.4577833464 +05 48 18.767115360           ~ 11 0
7 SDSS J094649.47+121628.4 QSO 09 46 49.4736287328 +12 16 28.460820144           ~ 10 0
8 SDSS J114638.95+074311.2 QSO 11 46 38.9522084352 +07 43 11.280833832           ~ 11 0
9 LBQS 1232+0815 QSO 12 34 37.5514444464 +07 58 43.367750796     18.4     ~ 128 0
10 SDSS J123714.60+064759.5 QSO 12 37 14.6105371632 +06 47 59.612187624   19.66 19.15     ~ 63 0
11 SDSS J131129.10+222552.5 QSO 13 11 29.1083707728 +22 25 52.585583628   20.62 20.03     ~ 20 0
12 QSO J1439+1117 BLL 14 39 12.0427245720 +11 17 40.563764052   19.27 18.92     ~ 77 1
13 [VV2006] J151349.5+035211 QSO 15 13 49.5187990104 +03 52 11.713951128   21.51 20.98     ~ 31 0
14 QSO J2100-0641 QSO 21 00 25.0301694552 -06 41 45.968177220   19.02 18.54     ~ 60 0
15 SDSS J212329.46-005052.9 QSO 21 23 29.4639412848 -00 50 52.916363736   16.91 16.62     ~ 131 0
16 SDSS J214043.02-032139.2 QSO 21 40 43.0124617776 -03 21 39.253768020           ~ 24 0
17 QSO B2318-1107 QSO 23 21 28.6902031608 -10 51 22.515901344           ~ 21 0
18 QSO J2340-0053 QSO 23 40 23.6700032496 -00 53 27.001299696   18.26 17.93     ~ 109 1
19 SDSS J234730.76-005131.5 QSO 23 47 30.7646955384 -00 51 31.590454572       20.1   ~ 18 0

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