A short mean free path at \$z=6\$ favors late and rapid reionization by faint galaxies. Cain, C., D'Aloisio, A., Gangolli, N., & Becker, G. D. arXiv e-prints, 2105:arXiv:2105.10511, May, 2021.
A short mean free path at \$z=6\$ favors late and rapid reionization by faint galaxies [link]Paper  abstract   bibtex   
Recent measurements of the ionizing photon mean free path (\${\textbackslash}lambda_\{912\}{\textasciicircum}\{{\textbackslash}rm mfp\}\$) at \$5 {\textless} z {\textless} 6\$ suggest that the IGM was rapidly evolving at those times. We use radiative transfer simulations to explore the implications for reionization, with a focus on the short value of \${\textbackslash}lambda_\{912\}{\textasciicircum}\{{\textbackslash}rm mfp\} = 3.57{\textasciicircum}\{+3.09\}_\{-2.14\}\$ cMpc/\$h\$ at \$z=6\$. We introduce a model for sub-resolution ionizing photon sinks based on radiative hydrodynamics simulations of small-scale IGM clumping. We argue that the rapid evolution in \${\textbackslash}lambda_\{912\}{\textasciicircum}\{p̌hantom{\}}{\textbackslash}rm mfpp̌hantom{\{}\}\$ at \$z=5-6\$, together with constraints on the metagalactic ionizing background, favors a late reionization process in which the neutral fraction evolved rapidly in the latter half. We also argue that the short \${\textbackslash}lambda_\{912\}{\textasciicircum}\{{\textbackslash}rm mfp\}(z=6)\$ points to faint galaxies as the primary drivers of reionizaton. Our preferred model, with \${\textbackslash}lambda_\{912\}{\textasciicircum}\{{\textbackslash}rm mfp\}(z=6) = 6.5\$ Mpc/\$h\$, has a midpoint of \$z= 7.1\$ and ends at \$z= 5.1\$. It requires 3 ionizing photons per H atom to complete reionization and a LyC photon production efficiency of \${\textbackslash}log(f{\textasciicircum}\{{\textbackslash}rm eff\}_\{{\textbackslash}rm esc\} {\textbackslash}xi_\{{\textbackslash}rm ion\}/[{\textbackslash}mathrm\{erg\}{\textasciicircum}\{-1\} {\textbackslash}mathrm\{Hz\}]) = 24.8\$ at \$z{\textgreater}6\$. Recovering \${\textbackslash}lambda_\{912\}{\textasciicircum}\{p̌hantom{\}}{\textbackslash}rm mfpp̌hantom{\{}\}(z=6)\$ as low as the measured central value may require an increase in IGM clumpiness beyond predictions from simulations, with a commensurate increase in the photon budget.
@article{cain_short_2021,
	title = {A short mean free path at \$z=6\$ favors late and rapid reionization by faint galaxies},
	volume = {2105},
	url = {http://adsabs.harvard.edu/abs/2021arXiv210510511C},
	abstract = {Recent measurements of the ionizing photon mean free path 
(\${\textbackslash}lambda\_\{912\}{\textasciicircum}\{{\textbackslash}rm mfp\}\$) at \$5 {\textless} z {\textless} 6\$ suggest that the IGM
was rapidly evolving at those times. We use radiative transfer
simulations to explore the implications for reionization, with a focus
on the short value of \${\textbackslash}lambda\_\{912\}{\textasciicircum}\{{\textbackslash}rm mfp\} = 3.57{\textasciicircum}\{+3.09\}\_\{-2.14\}\$
cMpc/\$h\$ at \$z=6\$. We introduce a model for sub-resolution ionizing
photon sinks based on radiative hydrodynamics simulations of small-scale
IGM clumping. We argue that the rapid evolution in \${\textbackslash}lambda\_\{912\}{\textasciicircum}\{\vphantom{\}}{\textbackslash}rm
mfp\vphantom{\{}\}\$ at \$z=5-6\$, together with constraints on the metagalactic ionizing
background, favors a late reionization process in which the neutral
fraction evolved rapidly in the latter half. We also argue that the
short \${\textbackslash}lambda\_\{912\}{\textasciicircum}\{{\textbackslash}rm mfp\}(z=6)\$ points to faint galaxies as the
primary drivers of reionizaton. Our preferred model, with
\${\textbackslash}lambda\_\{912\}{\textasciicircum}\{{\textbackslash}rm mfp\}(z=6) = 6.5\$ Mpc/\$h\$, has a midpoint of \$z= 7.1\$
and ends at \$z= 5.1\$. It requires 3 ionizing photons per H atom to
complete reionization and a LyC photon production efficiency of
\${\textbackslash}log(f{\textasciicircum}\{{\textbackslash}rm eff\}\_\{{\textbackslash}rm esc\} {\textbackslash}xi\_\{{\textbackslash}rm ion\}/[{\textbackslash}mathrm\{erg\}{\textasciicircum}\{-1\}
{\textbackslash}mathrm\{Hz\}]) = 24.8\$ at \$z{\textgreater}6\$. Recovering \${\textbackslash}lambda\_\{912\}{\textasciicircum}\{\vphantom{\}}{\textbackslash}rm
mfp\vphantom{\{}\}(z=6)\$ as low as the measured central value may require an increase
in IGM clumpiness beyond predictions from simulations, with a
commensurate increase in the photon budget.},
	urldate = {2021-06-04},
	journal = {arXiv e-prints},
	author = {Cain, Christopher and D'Aloisio, Anson and Gangolli, Nakul and Becker, George D.},
	month = may,
	year = {2021},
	keywords = {Astrophysics - Cosmology and Nongalactic Astrophysics},
	pages = {arXiv:2105.10511},
}

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