Non-equilibrium temperature evolution of ionization fronts during the
Epoch of Reionization
C. Zeng, and C. Hirata. (2020)cite arxiv:2007.02940Comment: 9 pages, 6 figures.
Abstract
The epoch of reionization (EoR) marks the end of the Cosmic Dawn and the
beginning of large-scale structure formation in the universe. The impulsive
ionization fronts (I-fronts) heat and ionize the gas within the reionization
bubbles in the intergalactic medium (IGM). The temperature during this process
is a key yet uncertain ingredient in current models. Typically, reionization
simulations assume that all baryonic species are in instantaneous thermal
equilibrium with each other during the passage of an I-front. Here we present a
new model of the temperature evolution for the ionization front by studying
non-equilibrium effects. In particular, we include the energy transfer between
major baryon species ($e^-$, \HI, \HII, \HeI, and \HeII) and investigate
their impacts on the post-ionization front temperature $T_re$. For a
better step-size control when solving the stiff equations, we implement an
implicit method and construct an energy transfer rate matrix. We find that the
assumption of equilibration is valid for a low-speed ionization front
($łessapprox\ 10^9~cm/s$), but deviations from equilibrium
occur for faster fronts. The post-front temperature $T_re$ is lower
by up to 19.7\% (at $310^9$ cm/s) or 30.8\% (at $10^10$ cm/s) relative
to the equilibrium case.
Description
Non-equilibrium temperature evolution of ionization fronts during the Epoch of Reionization
%0 Generic
%1 zeng2020nonequilibrium
%A Zeng, Chenxiao
%A Hirata, Christopher M.
%D 2020
%K library
%T Non-equilibrium temperature evolution of ionization fronts during the
Epoch of Reionization
%U http://arxiv.org/abs/2007.02940
%X The epoch of reionization (EoR) marks the end of the Cosmic Dawn and the
beginning of large-scale structure formation in the universe. The impulsive
ionization fronts (I-fronts) heat and ionize the gas within the reionization
bubbles in the intergalactic medium (IGM). The temperature during this process
is a key yet uncertain ingredient in current models. Typically, reionization
simulations assume that all baryonic species are in instantaneous thermal
equilibrium with each other during the passage of an I-front. Here we present a
new model of the temperature evolution for the ionization front by studying
non-equilibrium effects. In particular, we include the energy transfer between
major baryon species ($e^-$, \HI, \HII, \HeI, and \HeII) and investigate
their impacts on the post-ionization front temperature $T_re$. For a
better step-size control when solving the stiff equations, we implement an
implicit method and construct an energy transfer rate matrix. We find that the
assumption of equilibration is valid for a low-speed ionization front
($łessapprox\ 10^9~cm/s$), but deviations from equilibrium
occur for faster fronts. The post-front temperature $T_re$ is lower
by up to 19.7\% (at $310^9$ cm/s) or 30.8\% (at $10^10$ cm/s) relative
to the equilibrium case.
@misc{zeng2020nonequilibrium,
abstract = {The epoch of reionization (EoR) marks the end of the Cosmic Dawn and the
beginning of large-scale structure formation in the universe. The impulsive
ionization fronts (I-fronts) heat and ionize the gas within the reionization
bubbles in the intergalactic medium (IGM). The temperature during this process
is a key yet uncertain ingredient in current models. Typically, reionization
simulations assume that all baryonic species are in instantaneous thermal
equilibrium with each other during the passage of an I-front. Here we present a
new model of the temperature evolution for the ionization front by studying
non-equilibrium effects. In particular, we include the energy transfer between
major baryon species ($e^{-}$, \HI, \HII, \HeI, and \HeII) and investigate
their impacts on the post-ionization front temperature $T_{\mathrm{re}}$. For a
better step-size control when solving the stiff equations, we implement an
implicit method and construct an energy transfer rate matrix. We find that the
assumption of equilibration is valid for a low-speed ionization front
($\lessapprox\ 10^9~\mathrm{cm}/\mathrm{s}$), but deviations from equilibrium
occur for faster fronts. The post-front temperature $T_{\mathrm{re}}$ is lower
by up to 19.7\% (at $3\times 10^9$ cm/s) or 30.8\% (at $10^{10}$ cm/s) relative
to the equilibrium case.},
added-at = {2020-07-08T07:26:17.000+0200},
author = {Zeng, Chenxiao and Hirata, Christopher M.},
biburl = {https://www.bibsonomy.org/bibtex/261180ce7f23888e3ccdffd1b108a1f84/gpkulkarni},
description = {Non-equilibrium temperature evolution of ionization fronts during the Epoch of Reionization},
interhash = {942381d66867e062acf9700b0a93686c},
intrahash = {61180ce7f23888e3ccdffd1b108a1f84},
keywords = {library},
note = {cite arxiv:2007.02940Comment: 9 pages, 6 figures},
timestamp = {2020-07-08T07:26:17.000+0200},
title = {Non-equilibrium temperature evolution of ionization fronts during the
Epoch of Reionization},
url = {http://arxiv.org/abs/2007.02940},
year = 2020
}