Abstract
The thermal history of cosmic gas in the Dark Ages remains largely unknown.
It is important to quantify the impact of relevant physics on the IGM
temperature between $z=10$ and $z 30$, in order to interpret recent and
oncoming observations, including results reported by EDGES. We revisit the gas
heating due to structure formation shocks in this era, using a set of fixed
grid cosmological hydrodynamical simulations performed by three different
codes. In all our simulations, the cosmic gas is predicted to be in multiphase
state since $z>30$. The gas surrounding high density peaks gradually develops a
relation more sharp than $T \rho^2/3$, approximately $T \propto
\rho^2$, from $z=30$ to $z=11$, might due to shock heating. Meanwhile, the
gas in void region tends to have a large local mach number, and their thermal
state varies significantly from code to code. In the redshift range $11-20$,
the mass fraction of gas shock heated above the CMB temperature in our
simulations is larger than previous semi-analytical results by a factor of 2 to
8. At $z=15$, the fraction varies from $19\%$ to $52 \%$ among different
codes. Between $z=11$ and $z=20$, the gas temperature $<1/T_K>_M^-1$
is predicted to be $10-20$ K by two codes, much higher than the adiabatic
cooling model and some previous works. However, in our simulations performed by
RAMSES, $<1/T_K>_M^-1$ is predicted to be even below the temperature
required to explain result of the EDGES. Given the fact that different codes
give different predictions, currently, it seems a challenge to make solid
prediction on the temperature of gas at $z 17$ in simulations.
Users
Please
log in to take part in the discussion (add own reviews or comments).