11 research outputs found
Exploring the Milky Way Circumgalactic Medium in a Cosmological Context with a Semi-Analytic Model
We combine the Santa-Cruz Semi-Analytic Model (SAM) for galaxy formation and
evolution with the circumgalactic medium (CGM) model presented in Faerman et
al. (2020) to explore the CGM properties of galaxies. We use the SAM to
generate a sample of galaxies with halo masses similar to the Milky Way (MW)
halo, , and find that the CGM mass
and mean metallicity in the sample are correlated. We use the CGM masses and
metallicities of the SAM galaxies as inputs for the FSM20 model, and vary the
amount of non-thermal support. The density profiles in our models can be
approximated by power-law functions with slopes in the range of , with higher non-thermal pressure resulting in flatter distributions. We
explore how the gas pressure, dispersion measure, OVI-OVIII column densities,
and cooling rates behave with the gas distribution and total mass. We show that
for CGM masses below , photoionization has
a significant effect on the column densities of OVI and OVIII. The combination
of different MW CGM observations favors models with similar fractions in
thermal pressure, magnetic fields/cosmic rays, and turbulent support, and with
. The MW OVI column
requires , independent of the gas
distribution. The AGN jet-driven heating rates in the SAM are enough to offset
the CGM cooling, although exact balance is not required in star-forming
galaxies. We provide predictions for the columns densities of additional metal
ions - NV, NeVIII, and MgX.Comment: Submitted to ApJ. 19 pages, 15 figures (+ appendix
A Comprehensive Investigation of Metals in the Circumgalactic Medium of Nearby Dwarf Galaxies
Dwarf galaxies are found to have lost most of their metals via feedback
processes; however, there still lacks consistent assessment on the retention
rate of metals in their circumgalactic medium (CGM). Here we investigate the
metal content in the CGM of 45 isolated dwarf galaxies with
() using {\it
HST}/COS. While H I (Ly) is ubiquitously detected () within the
CGM, we find low detection rates () in C II, C IV, Si II, Si
III, and Si IV, largely consistent with literature values. Assuming these ions
form in the cool ( K) CGM with photoionization equilibrium, the
observed H I and metal column density profiles can be best explained by an
empirical model with low gas density and high volume filling factor. For a
typical galaxy with (median of the sample),
our model predicts a cool gas mass of ,
corresponding to of the galaxy's baryonic budget. Assuming a
metallicity of , we estimate that the dwarf galaxy's cool CGM
likely harbors of the metals ever produced, with the rest either in
more ionized states in the CGM or transported to the intergalactic medium. We
further examine the EAGLE simulation and show that H I and low ions may arise
from a dense cool medium, while C IV arises from a diffuse warmer medium. Our
work provides the community with a uniform dataset on dwarf galaxies' CGM that
combines our recent observations, additional archival data and literature
compilation, which can be used to test various theoretical models of dwarf
galaxies.Comment: Finalized version. Accepted for publication in Ap
The Cool Circumgalactic Medium of Low-redshift Star-forming Galaxies. I. Empirical Model and Mean Properties
We present an analytic model for the cool, T ∼ 10 ^4 K, circumgalactic medium (CGM), describing the gas distribution, and thermal and ionization states. Our model assumes (total) pressure equilibrium with the ambient warm/hot CGM, photoionization by the metagalactic radiation, and allows for nonthermal pressure support, parameterized by the ratio of thermal pressures, η = P _hot,th / P _cool,th . We apply the model to the COS-Halos measurements and find that a nominal model with η = 3, gas distribution out to r ≈ 0.6 R _vir , and M _cool = 3 × 10 ^9 M _⊙ , corresponding to a volume filling fraction of f _V,cool ≈ 1%, reproduces the H i and low/intermediate metal ions (C ii , C iii , Si ii , Si iii , and Mg ii ) mean column densities. Variation of ±0.5 dex in η or M _cool encompasses ∼2/3 of the scatter between objects. Our nominal model underproduces the measured C iv and Si iv columns, and these can be reproduced with (i) a cool phase with M _cool ∼ 10 ^10 M _⊙ and η ≈ 5, or (ii) cooling or mixing gas at intermediate temperatures, with M ∼ 1.5 × 10 ^10 M _⊙ and occupying ∼1/2 of the total CGM volume. For cool gas with f _V,cool ≈ 1%, we estimate an upper limit on the cloud sizes, R _cl ≲ 0.5 kpc. Our results suggest that for the average galaxy CGM, the mass and nonthermal support in the cool phase are lower than previously estimated, and extreme scenarios are not necessary. We estimate the rates of cool gas depletion and replenishment, and find accretion onto the galaxy can be offset, allowing over long timescales
A Comprehensive Investigation of Metals in the Circumgalactic Medium of Nearby Dwarf Galaxies
Dwarf galaxies are found to have lost most of their metals via feedback processes; however, there still lacks consistent assessment on the retention rate of metals in their circumgalactic medium (CGM). Here we investigate the metal content in the CGM of 45 isolated dwarf galaxies with M _* = 10 ^6.5–9.5 M _⊙ ( M _200m = 10 ^10.0–11.5 M _⊙ ) using the Hubble Space Telescope/Cosmic Origins Spectrograph. While H i (Ly α ) is ubiquitously detected (89%) within the CGM, we find low detection rates (≈5%–22%) in C ii , C iv , Si ii , Si iii , and Si iv , largely consistent with literature values. Assuming these ions form in the cool ( T ≈ 10 ^4 K) CGM with photoionization equilibrium, the observed H i and metal column density profiles can be best explained by an empirical model with low gas density and high volume filling factor. For a typical galaxy with M _200m = 10 ^10.9 M _⊙ (median of the sample), our model predicts a cool gas mass of M _CGM,cool ∼ 10 ^8.4 M _⊙ , corresponding to ∼2% of the galaxy’s baryonic budget. Assuming a metallicity of 0.3 Z _⊙ , we estimate that the dwarf galaxy’s cool CGM likely harbors ∼10% of the metals ever produced, with the rest either in more ionized states in the CGM or transported to the intergalactic medium. We further examine the EAGLE simulation and show that H i and low ions may arise from a dense cool medium, while C iv arises from a diffuse warmer medium. Our work provides the community with a uniform data set on dwarf galaxies’ CGM that combines our recent observations, additional archival data and literature compilation, which can be used to test various theoretical models of dwarf galaxies
WSRT HI imaging of ultra-compact high velocity clouds: gas-bearing dark matter minihalos?
A long standing problem in cosmology is the mismatch between the number of low mass dark matter halos predicted by simulations and the number of low mass galaxies observed in the Local Volume. We recently presented a set of isolated ultra-compact high velocity clouds (UCHVCs) identified within the dataset of the Arecibo Legacy Fast ALFA (ALFALFA) HI line survey that are consistent with representing low-mass gas-bearing dark matter halos within the Local Volume (Adams+ 2013). At distances of ~1 Mpc, the UCHVCs have HI masses of ~10^5 Msun and indicative dynamical masses of 10^7-10^8 Msun. The HI diameters of the UCHVCs range from 4' to 20', or 1 to 6 kpc at a distance of 1 Mpc.We have selected the most compact and isolated UCHVCs with the highest average column densities as representing the best galaxy candidates. These systems have been observed with the Westerbork Synthesis Radio Telescope (WSRT) to enable higher spatial resolution (~60") studies of the HI distribution. The HI morphology revealed by the WSRT data offers clues to the environment and origin of the UCHVCs, the kinematics of the HI allow the underlying mass distribution to be constrained, and the combination of spatial and spectral resolution allow the detection of a cold neutral medium component to the HI. The WSRT HI observations discriminate among the selected galaxy candidates for those objects that are most likely gas-bearing dark matter halos.One UCHVC, AGC198606, is of particular interest as it is located 16 km/s and 1.2 degrees from Leo T and has similar HI properties within the ALFALFA dataset. The WSRT HI observations reveal a smooth HI morphology and a velocity gradient along the HI major axis of the system consistent with rotation. These properties are consistent with the hypothesis that this object is a gas-bearing low-mass dark matter halo
Braving the Storm: Quantifying Disk-wide Ionized Outflows in the Large Magellanic Cloud with ULLYSES
The Large Magellanic Cloud (LMC) is home to many H ii regions, which may lead to significant outflows. We examine the LMC’s multiphase gas (T∼104-5 K) in H i, S ii, Si iv, and C iv using 110 stellar sight lines from the Hubble Space Telescope’s Ultraviolet Legacy Library of Young Stars as Essential Standards program. We develop a continuum fitting algorithm based on the concept of Gaussian process regression and identify reliable LMC interstellar absorption over v helio = 175–375 km s−1. Our analyses show disk-wide ionized outflows in Si iv and C iv across the LMC with bulk velocities of ∣v out, bulk∣ ∼ 20–60 km s−1, which indicates that most of the outflowing mass is gravitationally bound. The outflows’ column densities correlate with the LMC’s star formation rate surface densities (ΣSFR), and the outflows with higher ΣSFR tend to be more ionized. Considering outflows from both sides of the LMC as traced by C iv, we conservatively estimate a total outflow rate of Ṁout≳0.03M⊙ yr−1 and a mass-loading factor of η ≳ 0.15. We compare the LMC’s outflows with those detected in starburst galaxies and simulation predictions, and find a universal scaling relation of ∣vout, bulk∣∝ΣSFR0.23 over a wide range of star-forming conditions (ΣSFR ∼ 10−4.5–102 M ⊙ yr−1 kpc−2). Lastly, we find that the outflows are corotating with the LMC’s young stellar disk and the velocity field does not seem to be significantly impacted by external forces; we thus speculate on the existence of a bow shock leading the LMC, which may have shielded the outflows from ram pressure as the LMC orbits the Milky Way