CO-dark molecular gas at high redshift: very large H\$_2\$ content and high pressure in a low metallicity damped Lyman-alpha system. Balashev, S. A., Noterdaeme, P., Rahmani, H., Klimenko, V. V., Ledoux, C., Petitjean, P., Srianand, R., Ivanchik, A. V., & Varshalovich, D. A. arXiv:1705.10283 [astro-ph], May, 2017. arXiv: 1705.10283
CO-dark molecular gas at high redshift: very large H\$_2\$ content and high pressure in a low metallicity damped Lyman-alpha system [link]Paper  abstract   bibtex   
We present a detailed analysis of a H\$_2\$-rich, extremely strong intervening Damped Ly-\${\textbackslash}alpha\$ Absorption system (DLA) at \$z_\{{\textbackslash}rm abs\}=2.786\$ towards the quasar J\${\textbackslash},\$0843+0221, observed with the Ultraviolet and Visual Echelle Spectrograph on the Very Large Telescope. The total column density of molecular (resp. atomic) hydrogen is \${\textbackslash}log N\$(H\$_2\$)=\$21.21{\textbackslash}pm0.02\$ (resp. \${\textbackslash}log N\$(H\${\textbackslash},\$I)=\$21.82{\textbackslash}pm0.11\$), making it to be the first case in quasar absorption lines studies with H\$_2\$ column density as high as what is seen in \${\textasciicircum}\{13\}\$CO-selected clouds in the Milky-Way. We find that this system has one of the lowest metallicity detected among H\$_2\$-bearing DLAs, with \${\textbackslash}rm [Zn/H]=-1.52{\textasciicircum}\{+0.08\}_\{-0.10\}\$. This can be the reason for the marked differences compared to systems with similar H\$_2\$ column densities in the local Universe: \$(i)\$ the kinetic temperature, \$T{\textbackslash}sim\$120\textasciitildeK, derived from the \$J=0,1\$ H\$_2\$ rotational levels is at least twice higher than expected; \$(ii)\$ there is little dust extinction with A\$_V {\textless} 0.1\$; \$(iii)\$ no CO molecules are detected, putting a constraint on the \$X_\{{\textbackslash}rm CO\}\$ factor \$X_\{{\textbackslash}rm CO\}{\textgreater} 2{\textbackslash}times 10{\textasciicircum}\{23\} \$ cm\${\textasciicircum}\{-2\}\$/(km/s\textbackslash,K), in the very low metallicity gas. Low CO and high H\$_2\$ contents indicate that this system represents "CO-dark/faint" gas. We investigate the physical conditions in the H\$_2\$-bearing gas using the fine-structure levels of C\${\textbackslash},\$I, C\${\textbackslash},\$II, Si\${\textbackslash},\$II and the rotational levels of HD and H\$_2\$. We find the number density to be about \$n {\textbackslash}sim 260-380{\textbackslash},\$cm\${\textasciicircum}\{-3\}\$, implying a high thermal pressure of \$(3-5) {\textbackslash}times 10{\textasciicircum}4{\textbackslash},\$cm\${\textasciicircum}\{-3\}{\textbackslash},\$K. We further identify a trend of increasing pressure with increasing total hydrogen column density. This independently supports the suggestion that extremely strong DLAs (with \${\textbackslash}log{\textbackslash},\$N(H) \${\textbackslash}sim 22\$) probe high-z galaxies at low impact parameters.
@article{balashev_co-dark_2017,
	title = {{CO}-dark molecular gas at high redshift: very large {H}\$\_2\$ content and high pressure in a low metallicity damped {Lyman}-alpha system},
	shorttitle = {{CO}-dark molecular gas at high redshift},
	url = {http://arxiv.org/abs/1705.10283},
	abstract = {We present a detailed analysis of a H\$\_2\$-rich, extremely strong intervening Damped Ly-\${\textbackslash}alpha\$ Absorption system (DLA) at \$z\_\{{\textbackslash}rm abs\}=2.786\$ towards the quasar J\${\textbackslash},\$0843+0221, observed with the Ultraviolet and Visual Echelle Spectrograph on the Very Large Telescope. The total column density of molecular (resp. atomic) hydrogen is \${\textbackslash}log N\$(H\$\_2\$)=\$21.21{\textbackslash}pm0.02\$ (resp. \${\textbackslash}log N\$(H\${\textbackslash},\$I)=\$21.82{\textbackslash}pm0.11\$), making it to be the first case in quasar absorption lines studies with H\$\_2\$ column density as high as what is seen in \${\textasciicircum}\{13\}\$CO-selected clouds in the Milky-Way. We find that this system has one of the lowest metallicity detected among H\$\_2\$-bearing DLAs, with \${\textbackslash}rm [Zn/H]=-1.52{\textasciicircum}\{+0.08\}\_\{-0.10\}\$. This can be the reason for the marked differences compared to systems with similar H\$\_2\$ column densities in the local Universe: \$(i)\$ the kinetic temperature, \$T{\textbackslash}sim\$120{\textasciitilde}K, derived from the \$J=0,1\$ H\$\_2\$ rotational levels is at least twice higher than expected; \$(ii)\$ there is little dust extinction with A\$\_V {\textless} 0.1\$; \$(iii)\$ no CO molecules are detected, putting a constraint on the \$X\_\{{\textbackslash}rm CO\}\$ factor \$X\_\{{\textbackslash}rm CO\}{\textgreater} 2{\textbackslash}times 10{\textasciicircum}\{23\} \$ cm\${\textasciicircum}\{-2\}\$/(km/s{\textbackslash},K), in the very low metallicity gas. Low CO and high H\$\_2\$ contents indicate that this system represents "CO-dark/faint" gas. We investigate the physical conditions in the H\$\_2\$-bearing gas using the fine-structure levels of C\${\textbackslash},\$I, C\${\textbackslash},\$II, Si\${\textbackslash},\$II and the rotational levels of HD and H\$\_2\$. We find the number density to be about \$n {\textbackslash}sim 260-380{\textbackslash},\$cm\${\textasciicircum}\{-3\}\$, implying a high thermal pressure of \$(3-5) {\textbackslash}times 10{\textasciicircum}4{\textbackslash},\$cm\${\textasciicircum}\{-3\}{\textbackslash},\$K. We further identify a trend of increasing pressure with increasing total hydrogen column density. This independently supports the suggestion that extremely strong DLAs (with \${\textbackslash}log{\textbackslash},\$N(H) \${\textbackslash}sim 22\$) probe high-z galaxies at low impact parameters.},
	journal = {arXiv:1705.10283 [astro-ph]},
	author = {Balashev, S. A. and Noterdaeme, P. and Rahmani, H. and Klimenko, V. V. and Ledoux, C. and Petitjean, P. and Srianand, R. and Ivanchik, A. V. and Varshalovich, D. A.},
	month = may,
	year = {2017},
	note = {arXiv: 1705.10283},
	keywords = {Astrophysics - Astrophysics of Galaxies},
}

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