173 research outputs found
Nebular Emission from Star-Forming Galaxies
We present a new model for computing consistently the line and continuum
emission from galaxies, based on a combination of recent population synthesis
and photoionization codes. We use effective parameters to describe the HII
regions and the diffuse gas ionized by single stellar generations in a galaxy
[...]. We calibrate the nebular properties of our model using the observed
[OIII]/Hbeta, [OII]/[OIII], [SII]/Halpha, and [NII]/[SII] ratios of a
representative sample of nearby spiral and irregular, starburst, and HII
galaxies. To compute whole (line plus continuum) spectral energy distributions,
we include the absorption by dust in the neutral interstellar medium (ISM)
using a recent simple prescription, which is consistent with observations of
nearby starburst galaxies. Our model enables us to interpret quantitatively the
observed optical spectra of galaxies in terms of stars, gas, and dust
parameters. We find that the range of ionized-gas properties spanned by nearby
galaxies implies factors of 3.5 and 14 variations in the Halpha and [OII]
luminosities produced per unit star formation rate (SFR). When accounting for
stellar Halpha absorption and absorption by dust in the neutral ISM, the actual
uncertainties in SFR estimates based on the emergent Halpha and [OII]
luminosities are as high as several decades. We derive new estimators of the
SFR, the gas-phase oxygen abundance, and the effective absorption optical depth
of the dust in galaxies. We show that, with the help of other lines such as
[OII], Hbeta, [OIII], [NII], or [SII], the uncertainties in SFR estimates based
on Halpha can be reduced to a factor of only 2-3, even if the Halpha line is
blended with the adjacent [NII] lines. Without Halpha, however, the SFR is
difficult to estimate from the [OII], Hbeta, and [OIII] lines. (abridged)Comment: To appear in MNRAS; 17 pages with 10 embedded PS figures (mn.sty
Superdense and normal early-type galaxies at 1<z<2
We combined proprietary and archival HST observations to collect a sample of
62 early-type galaxies (ETGs) at 0.9<z<2 with spectroscopic confirmation of
their redshift and spectral type. The whole sample is covered by ACS or NICMOS
observations and partially by Spitzer and AKARI observations. We derived
morphological parameters by fitting their HST light profiles and physical
parameters by fitting their spectral energy distributions. The study of the
size-mass and the size-luminosity relations of these early-types shows that a
large fraction of them (~50) follows the local relations. These 'normal' ETGs
are not smaller than local counterparts with comparable mass. The remaining
half of the sample is composed of compact ETGs with sizes (densities) 2.5-3
(15-30) times smaller (higher) than local counterparts and, most importantly,
than the other normal ETGs at the same redshift and with the same stellar mass.
This suggests that normal and superdense ETGs at z~2 come from different
histories of mass assembly.Comment: 4 pages, 3 figures. To appear in "Hunting for the Dark: The Hidden
Side of Galaxy Formation", Malta, 19-23 Oct. 2009, eds. V.P. Debattista and
C.C. Popescu, AIP Conf. (in press
Star Formation History of Early-Type Galaxies in Low Density Environments V. Blue line-strength indices for the nuclear region
We analyze the star formation properties of a sample of 21 shell galaxies and
30 early-type galaxies members of interacting pairs, located in low density
environments (Longhetti et al 1998a, 1998b).
The study is based on new models developed to interpret the information
coming from `blue' H/FeI, H+K(CaII) and \D4000 line-strength indices
proposed by Rose (1984; 1985) and Hamilton (1985).
We find that the last star forming event that occurred in the nuclear region
of shell galaxies is statistically old (from 0.1 up to several Gyr) with
respect to the corresponding one in the sub-sample of pair galaxies (<0.1 Gyr
or even ongoing star formation).
If the stellar activity is somehow related to the formation of shells, as
predicted by several dynamical models of galaxy interaction, shells have to be
considered long lasting structures.
Since pair members show evidence of very recent star formation, we suggest
that either large reservoirs of gas have to be present to maintain active star
formation, if these galaxies are on periodic orbits, or most of the pair
members in the present sample are experiencing unbound encounters.Comment: 12 pages, including 7 figures - Accepted for publication in A&
The population of early-type galaxies: how it evolves with time and how it differs from passive and late-type galaxies
The aim of our analysis is twofold. On the one hand we are interested in
addressing whether a sample of ETGs morphologically selected differs from a
sample of passive galaxies in terms of galaxy statistics. On the other hand we
study how the relative abundance of galaxies, the number density and the
stellar mass density for different morphological types change over the redshift
range 0.6<z<2.5. From the 1302 galaxies brighter than Ks=22 selected from the
GOODS-MUSIC catalogue, we classified the ETGs on the basis of their morphology
and the passive galaxies on the basis of their sSFR. We proved how the
definition of passive galaxy depends on the IMF adopted in the models and on
the assumed sSFR threshold. We find that ETGs cannot be distinguished from the
other morphological classes on the basis of their low sSFR, irrespective of the
IMF adopted in the models. Using the sample of 1302 galaxies morphologically
classified into spheroidal galaxies (ETGs) and not spheroidal galaxies (LTGs),
we find that their fractions are constant over the redshift range 0.6<z<2.5
(20-30% ETGs vs 70-80% LTGs). However, at z<1 these fractions change among the
population of the most massive (M*>=10^(11) M_sol) galaxies, with the fraction
of massive ETGs rising up to 40% and the fraction of massive LTGs decreasing
down to 60%. Moreover, we find that the number density and the stellar mass
density of the whole population of massive galaxies increase almost by a factor
of ~10 between 0.6<z<2.5, with a faster increase of these densities for the
ETGs than for the LTGs. Finally, we find that the number density of the
highest-mass galaxies (M*>3-4x10^(11) M_sol) both ETGs and LTGs do not increase
since z~2.5, contrary to the lower mass galaxies. This suggests that the
population of the most massive galaxies formed at z>2.5-3 and that the assembly
of such high-mass galaxies is not effective at lower redshift.Comment: 15 pages, 14 figures. Published in A&
Lower mass normalization of the stellar initial mass function for dense massive early-type galaxies at z ~ 1.4
This paper aims at understanding if the normalization of the stellar initial
mass function (IMF) of massive early-type galaxies (ETGs) varies with cosmic
time and/or with mean stellar mass density Sigma (M*/2\pi Re^2). For this
purpose we collected a sample of 18 dense (Sigma>2500 M_sun/pc^2) ETGs at
1.2<z<1.6 with available velocity dispersion sigma_e. We have constrained their
mass-normalization by comparing their true stellar masses (M_true) derived
through virial theorem, hence IMF independent, with those inferred through the
fit of the photometry assuming a reference IMF (M_ref). Adopting the virial
estimator as proxy of the true stellar mass, we have assumed for these ETGs
zero dark matter (DM). However, dynamical models and numerical simulations of
galaxy evolution have shown that the DM fraction within Re in dense high-z ETGs
is negligible. We have considered the possible bias of virial theorem in
recovering the total masses and have shown that for dense ETGs the virial
masses are in agreement with those derived through more sophisticated dynamical
models. The variation of the parameter Gamma = M_true/M_ref with sigma_e shows
that, on average, dense ETGs at = 1.4 follow the same IMF-sigma_e trend of
typical local ETGs, but with a lower mass-normalization. Nonetheless, once the
IMF-sigma_e trend we have found for high-z dense ETGs is compared with that of
local ETGs with similar Sigma and sigma_e, they turn out to be consistent. The
similarity between the IMF-sigma_e trends of dense high-z and low-z ETGs over 9
Gyr of evolution and their lower mass-normalization with respect to the mean
value of local ETGs suggest that, independently on formation redshift, the
physical conditions characterizing the formation of a dense spheroid lead to a
mass spectrum of new formed stars with an higher ratio of high- to low-mass
stars with respect to the IMF of normal local ETGs.Comment: 9 pages, 4 figures, accepted for pubblication in A&A, updated to
match final journal versio
Star Formation, Metallicity and Dust Properties Derived from the SAPM Galaxy Survey Spectra
We have derived star formation rates (SFRs), gas-phase oxygen abundances and
effective dust absorption optical depths for a sample of galaxies drawn from
the Stromlo-APM redshift survey using the new Charlot and Longhetti (2001;
CL01) models, which provide a physically consistent description of the effects
of stars, gas and dust on the integrated spectra of galaxies. Our sample
consists of 705 galaxies with measurements of the fluxes and equivalent widths
of Halpha, [OII], and one or both of [NII] and [SII]. For a subset of the
galaxies, 60 and 100 micron IRAS fluxes are available. We compare the star
formation rates derived using the models with those derived using standard
estimators based on the Halpha, the [OII] and the far-infrared luminosities of
the galaxies. The CL01 SFR estimates agree well with those derived from the
IRAS fluxes, but are typically a factor of ~3 higher than those derived from
the Halpha or the [OII] fluxes, even after the usual mean attenuation
correction of A_Halpha=1 mag is applied to the data. We show that the reason
for this discrepancy is that the standard Halpha estimator neglects the
absorption of ionizing photons by dust in HII regions and the contamination of
Halpha emission by stellar absorption. We also use our sample to study
variations in star formation and metallicity as a function of galaxy absolute
bJ magnitude. For this sample, the star formation rate per unit bJ luminosity
is independent of magnitude. The gas-phase oxygen abundance does increase with
bJ luminosity, although the scatter in metallicity at fixed magnitude is large.Comment: 17 pages, 8 figures, accepted for publication in MNRA
Probing the evolution of the near-IR luminosity function of galaxies to z ~ 3 in the Hubble Deep Field South
[Abridged] We present the rest-frame Js-band and Ks-band luminosity function
of a sample of about 300 galaxies selected in the HDF-S at Ks<23 (Vega). We use
calibrated photometric redshift together with spectroscopic redshift for 25% of
the sample. The sample has allowed to probe the evolution of the LF in the
three redshift bins [0;0.8), [0.8;1.9) and [1.9;4) centered at the median
redshift z_m ~ [0.6,1.2,3]. The values of alpha we estimate are consistent with
the local value and do not show any trend with redshift. We do not see evidence
of evolution from z=0 to z_m ~ 0.6 suggesting that the population of local
bright galaxies was already formed at z<0.8. On the contrary, we clearly detect
an evolution of the LF to z_m ~ 1.2 characterized by a brightening of M* and by
a decline of phi*. To z_m ~ 1.2 M* brightens by about 0.4-0.6 mag and phi*
decreases by a factor 2-3. This trend persists, even if at a less extent, down
to z_m ~ 3 both in the Js-band and in the Ks-band LF. The decline of the number
density of bright galaxies seen at z>0.8 suggests that a significant fraction
of them increases their stellar mass at 1<z<2-3 and that they underwent a
strong evolution in this redshift range. On the other hand, this implies also
that a significant fraction of local bright/massive galaxies was already in
place at z>3. Thus, our results suggest that the assembly of high-mass galaxies
is spread over a large redshift range and that the increase of their stellar
mass has been very efficient also at very high redshift at least for a fraction
of them.Comment: 18 pages, 21 figures, Accepted for publication in MNRA
- …