Abstract
Observations reveal massive amounts of OVI around star-forming $L_*$
galaxies, with covering fractions of near unity extending to the host halo's
virial radius. This OVI absorption is typically kinematically centered upon
photoionized gas, with line widths that are suprathermal and kinematically
offset from the galaxy. We discuss various scenarios and whether they could
result in the observed phenomenology (cooling flows, boundary layers, shocks,
virialized gas, photoionized clouds in thermal equilibrium). If predominantly
collisionally ionized, as we argue is most probable, the OVI observations
require that the circumgalactic medium (CGM) of $L_*$ galaxies holds nearly all
the associated baryons within a virial radius ($10^11M_ødot$) and that
there is likely a cooling flow of
$\approx30nT/30\rm~cm^-3K~M_ødot~$yr$^-1$, which must be largely
prevented from accreting onto the host galaxy. Cooling and feedback energetics
considerations require $10 <nT\rangle<100\rm~cm^-3K$ for the warm
and hot halo gases. We argue that virialized gas, boundary layers, hot winds,
and shocks are unlikely to directly account for the bulk of the OVI.
Furthermore, we show that there is a robust constraint on the number density of
many of the photoionized $\sim10^4$K absorption systems that yields upper
bounds in the range $n<(0.1-3)\times10^-3(Z/0.3)$cm$^-3$, where $Z$ is the
metallicity, suggestive that the dominant pressure in some photoionized clouds
is nonthermal. This constraint, which requires minimal ionization modeling, is
in accord with the low densities inferred from more complex photoionization
modeling. The large inferred cooling flow could re-form these clouds in a
fraction of the halo dynamical time, as some arguments require, and it requires
much of the feedback energy available from supernovae and stellar winds to be
dissipated in the CGM.
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