10,580 research outputs found
The origin of scatter in the star formation rate - stellar mass relation
Observations have revealed that the star formation rate (SFR) and stellar
mass (M) of star-forming galaxies follow a tight relation known as
the galaxy main sequence. However, what physical information is encoded in this
relation is under debate. Here, we use the EAGLE cosmological hydrodynamical
simulation to study the mass dependence, evolution and origin of scatter in the
SFR-M relation. At , we find that the scatter decreases
slightly with stellar mass from 0.35 dex at M
M to 0.30 dex at M M. The
scatter decreases from to by 0.05 dex at M M and by 0.15 dex for lower masses. We show that the scatter
at originates from a combination of fluctuations on short time-scales
(ranging from 0.2-2 Gyr) that are presumably associated with self-regulation
from cooling, star formation and outflows, but is dominated by long time-scale
( Gyr) variations related to differences in halo formation times.
Shorter time-scale fluctuations are relatively more important for lower-mass
galaxies. At high masses, differences in black hole formation efficiency cause
additional scatter, but also diminish the scatter caused by different halo
formation times. While individual galaxies cross the main sequence multiple
times during their evolution, they fluctuate around tracks associated with
their halo properties, i.e. galaxies above/below the main sequence at
tend to have been above/below the main sequence for Gyr.Comment: Accepted for publication in MNRAS. Updated comparison to
observations. More detailed investigation of the relative importance of
SFH-fluctuation time-scales on the SFR(Mstar) scatter (S 4.3, Figs. 6 & 7
The mean free path of hydrogen ionizing photons during the epoch of reionization
We use the Aurora radiation-hydrodynamical simulations to study the mean free
path (MFP) for hydrogen ionizing photons during the epoch of reionization. We
directly measure the MFP by averaging the distance 1 Ry photons travel before
reaching an optical depth of unity along random lines-of-sight. During
reionization the free paths tend to end in neutral gas with densities near the
cosmic mean, while after reionizaton the end points tend to be overdense but
highly ionized. Despite the increasing importance of discrete, over-dense
systems, the cumulative contribution of systems with suffices to drive the MFP at , while at
earlier times higher column densities are more important. After reionization
the typical size of HI systems is close to the local Jeans length, but during
reionization it is much larger. The mean free path for photons originating
close to galaxies, , is much smaller than the cosmic MFP. After
reionization this enhancement can remain significant up to starting distances
of comoving Mpc. During reionization, however, for
distances comoving kpc typically exceeds the cosmic MFP.
These findings have important consequences for models that interpret the
intergalactic MFP as the distance escaped ionizing photons can travel from
galaxies before being absorbed and may cause them to under-estimate the
required escape fraction from galaxies, and/or the required emissivity of
ionizing photons after reionization.Comment: 13 pages, 9 figures, 1 table; submitted to MNRA
Predictions for the relation between strong HI absorbers and galaxies at redshift 3
We combine cosmological, hydrodynamical simulations with accurate radiative
transfer corrections to investigate the relation between strong HI absorbers
(N_HI >~ 10^17 /cm^2) and galaxies at redshift z = 3. We find a strong
anti-correlation between the column density and the impact parameter that
connects the absorber to the nearest galaxy. The median impact parameters for
Lyman Limit (LL) and Damped Lyman-{\alpha} (DLA) systems are ~10 and ~1 proper
kpc, respectively. If normalized to the size of the halo of the nearest central
galaxy, the median impact parameters for LL and DLA systems become ~1 and
~10^-1 virial radii, respectively. At a given HI column density, the impact
parameter increases with the mass of the closest galaxy, in agreement with
observations. We predict most strong HI absorbers to be most closely associated
with extremely low-mass galaxies, M_star < 10^8 M_sun and star formation rate
<10^-1 M_sun/yr. We also find a correlation between the column density of
absorbers and the mass of the nearest galaxy. This correlation is most
pronounced for DLAs with N_HI > 10^21 /cm^2 which are typically close to
galaxies with M_star >~ 10^9 M_sun. Similar correlations exist between column
density and other properties of the associated galaxies such as their star
formation rates, halo masses and HI content. The galaxies nearest to HI
absorbers are typically far too faint to be detectable with current
instrumentation, which is consistent with the high rate of (often unpublished)
non-detections in observational searches for the galaxy counterparts of strong
HI absorbers. Moreover, we predict that the detected nearby galaxies are
typically not the galaxies that are most closely associated with the absorbers,
thus causing the impact parameters, star formation rates and stellar masses of
the observed counterparts to be biased high.Comment: 21 pages, 14 figures; Accepted for publication in MNRA
Star-forming galaxies are predicted to lie on a fundamental plane of mass, star formation rate and \alpha-enhancement
Observations show that star-forming galaxies reside on a tight
three-dimensional plane between mass, gas-phase metallicity and star formation
rate (SFR), which can be explained by the interplay between metal-poor gas
inflows, SFR and outflows. However, different metals are released on different
time-scales, which may affect the slope of this relation. Here, we use central,
star-forming galaxies with M M from the
EAGLE hydrodynamical simulation to examine three-dimensional relations between
mass, SFR and chemical enrichment using absolute and relative C, N, O and Fe
abundances. We show that the scatter is smaller when gas-phase
-enhancement is used rather than metallicity. A similar plane also
exists for stellar -enhancement, implying that present-day specific
SFRs are correlated with long time-scale star formation histories. Between
and 1, the -enhancement plane is even more insensitive to
redshift than the plane using metallicity. However, it evolves at due to
lagging iron yields. At fixed mass, galaxies with higher SFRs have star
formation histories shifted toward late times, are more -enhanced and
this -enhancement increases with redshift as observed. These findings
suggest that relations between physical properties inferred from observations
may be affected by systematic variations in -enhancements.Comment: 6 pages, 4 figures; Accepted for publication in MNRAS Letter
An evaluation of performance information procurement system (PIPS)
Since procurement is seen as crucial for project success, many\ud
methods have been developed and papers written about this issue. A remarkable\ud
contribution in this field comes from Dean Kashiwagi (Arizona State University,\ud
USA) who underpins his support for the Performance Information Procurement\ud
System (PiPS) with claims of high project performance and client satisfaction.\ud
Kashiwagi’s explanation for PiPS’s effects is based upon a theoretical\ud
framework that relates to staff members’ ability to deal appropriately with\ud
information by making sound decisions based not just on implicit expectation\ud
and tacit experience. This is not, however, a satisfactory explanation. This paper\ud
provides an overview of New Institutional Economics perspectives which are\ud
better able to explain the effects of PiPS. The linking of these theories to\ud
innovative PiPS elements clears the path to effectively select and apply PiPS\ud
elements within suitable projects in the Dutch construction industry. This will\ud
enhance industry performance and is of interest to all stakeholders
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