5,811 research outputs found
Weak homology of elliptical galaxies
We start by studying a small set of objects characterized by photometric
profiles that have been pointed out to deviate significantly from the standard
R^{1/4} law. For these objects we confirm that a generic R^{1/n} law, with n a
free parameter, can provide superior fits (the best-fit value of n can be lower
than 2.5 or higher than 10), better than those that can be obtained by a pure
R^{1/4} law, by an R^{1/4}+exponential model, and by other dynamically
justified self--consistent models. Therefore, strictly speaking, elliptical
galaxies should not be considered homologous dynamical systems. Still, a case
for "weak homology", useful for the interpretation of the Fundamental Plane of
elliptical galaxies, could be made if the best-fit parameter n, as often
reported, correlates with galaxy luminosity L, provided the underlying
dynamical structure also follows a systematic trend with luminosity. We
demonstrate that this statement may be true even in the presence of significant
scatter in the correlation n(L). Preliminary indications provided by a set of
"data points" associated with a sample of 14 galaxies suggest that neither the
strict homology nor the constant stellar mass--to--light solution are a
satisfactory explanation of the observed Fundamental Plane (abridged).Comment: 34 pages, 11 figures, accepted by Astronomy and Astrophysic
The Evolution of Early-Type Galaxies in Distant Clusters III.: M/L_V Ratios in the z=0.33 Cluster CL1358+62
Keck spectroscopy and Hubble Space Telescope WFPC2 imaging over a 1.5x1.5 Mpc
field of CL1358+62 at z=0.33 are used to study the Fundamental Plane of
galaxies based on a new, large sample of 53 galaxies. First, we have
constructed the Fundamental Plane for the 30 E and S0 galaxies and find that it
has the following shape: r_e = sigma**(1.31+-0.13) * _e**(-0.86+-0.10),
similar to that found locally. The 1-sigma intrinsic scatter about this plane
is 14% in M/L(V), comparable to that observed in Coma. We conclude that these E
and S0 galaxies are structurally mature and homogeneous, like those observed in
nearby clusters. The M/L(V) ratios of these early-type galaxies are offset from
the Coma Fundamental Plane by delta log M/L(V) = -0.13+- 0.03 (q0=0.1),
indicative of mild luminosity evolution. This evolution suggests a formation
epoch for the stars of z > 1. We have also analyzed the M/L(V) ratios of
galaxies of type S0/a and later. These early-type spirals follow a different
plane from the E and S0 galaxies, with a scatter that is twice as large as the
scatter for the E/S0s. The difference in the tilt between the plane of the
spirals and the plane of the E/S0s is shown to be due to a systematic
correlation of velocity dispersion with residual from the plane of the
early-type galaxies. These residuals also correlate with the residuals from the
Color-Magnitude relation. Thus for spirals in clusters, we see a systematic
variation in the luminosity-weighted mean properties of the stellar populations
with central velocity dispersion. If this is a relative age trend, then
luminosity-weighted age is positively correlated with dispersion. [abridged
version]Comment: 18 pages, 8 figures; revised version, accepted by ApJ on 13 August
199
Toward Equations of Galactic Structure
We find that all classes of galaxies, ranging from disks to spheroids and
from dwarf spheroidals to brightest cluster galaxies, lie on a two dimensional
surface within the space defined by the logarithms of the half-light radius,
r_e, mean surface brightness within r_e, I_e, and internal velocity, V^2 =
(1/2)v_c^2 + sigma^2, where v_c is the rotational velocity and sigma is the
velocity dispersion. If these quantities are expressed in terms of kpc,
L_solar/pc^2, and km/s, then log r_e - log V^2 + log I_e + log Upsilon_e + 0.8
= 0, where we provide a fitting function for Upsilon_e, the mass-to-light ratio
within r_e in units of M_solar/L_solar, that depends only on V and I_e. The
scatter about this surface for our heterogeneous sample of 1925 galaxies is
small (< 0.1 dex) and could be as low as ~ 0.05 dex, or 10%. This small scatter
has three possible implications for how gross galactic structure is affected by
internal factors, such as stellar orbital structure, and by external factors,
such as environment. These factors either 1) play no role beyond generating
some of the observed scatter, 2) move galaxies along the surface, or 3) balance
each other to maintain this surface as the locus of galactic structure
equilibria. We cast the behavior of Upsilon_e in terms of the fraction of
baryons converted to stars, eta, and the concentration of those stars within
the dark matter halo, xi = R_{200}/r_e. We derive eta = 1.9 x 10^{-5} (L/L^*)
Upsilon_* V^{-3} and xi = 1.4 V/r_e. Finally, we present and discuss the
distributions of eta and xi for the full range of galaxies. For systems with
internal velocities comparable to that of the Milky Way (149 < V < 163 km/s),
eta = 0.14 +- 0.05, and xi is, on average, ~ 5 times greater for spheroids than
for disks. (Abridged)Comment: submitted to Ap
Universal IMF vs dark halo response in early-type galaxies: breaking the degeneracy with the fundamental plane
We use the relations between aperture stellar velocity dispersion
(\sigma_ap), stellar mass (M_sps), and galaxy size (R_e) for a sample of \sim
150,000 early-type galaxies from SDSS/DR7 to place constraints on the stellar
initial mass function (IMF) and dark halo response to galaxy formation. We
build LCDM based mass models that reproduce, by construction, the relations
between galaxy size, light concentration and stellar mass, and use the
spherical Jeans equations to predict \sigma_ap. Given our model assumptions
(including those in the stellar population synthesis models), we find that
reproducing the median \sigma_ap vs M_sps relation is not possible with {\it
both} a universal IMF and a universal dark halo response. Significant
departures from a universal IMF and/or dark halo response are required, but
there is a degeneracy between these two solutions. We show that this degeneracy
can be broken using the strength of the correlation between residuals of the
velocity-mass (\Delta log \sigma_ap) and size-mass (\Delta log R_e) relations.
The slope of this correlation, d_vr \equiv \Delta log \sigma_ap/\Delta log R_e,
varies systematically with galaxy mass from d_vr \simeq -0.45 at M_sps \sim
10^{10}M_sun, to d_vr \simeq -0.15 at M_sps \sim 10^{11.6} M_sun. The virial
fundamental plane (FP) has d_vr=-1/2, and thus we find the tilt of the observed
FP is mass dependent. Reproducing this tilt requires {\it both} a non-universal
IMF and a non-universal halo response. Our best model has mass-follows-light at
low masses (Msps < 10^{11.2}M_sun) and unmodified NFW haloes at M_sps \sim
10^{11.5} M_sun. The stellar masses imply a mass dependent IMF which is
"lighter" than Salpeter at low masses and "heavier" than Salpeter at high
masses.Comment: 19 pages, 16 figures, accepted to MNRAS. More extensive discussion, 4
new figures, conclusions unchange
Exploiting Homology Information in Nontemplate Based Prediction of Protein Structures
In this paper we describe a novel strategy for exploring the conformational space of proteins and show that this leads to better models for proteins the structure of which is not amenable to template based methods. Our strategy is based on the assumption that the energy global minimum of homologous proteins must correspond to similar conformations, while the precise profiles of their energy landscape, and consequently the positions of the local minima, are likely to be different. In line with this hypothesis, we apply a replica exchange Monte Carlo simulation protocol that, rather than using different parameters for each parallel simulation, uses the sequences of homologous proteins. We show that our results are competitive with respect to alternative methods, including those producing the best model for each of the analyzed targets in the CASP10 (10th Critical Assessment of techniques for protein Structure Prediction) experiment free modeling category
Sliced Wasserstein Kernel for Persistence Diagrams
Persistence diagrams (PDs) play a key role in topological data analysis
(TDA), in which they are routinely used to describe topological properties of
complicated shapes. PDs enjoy strong stability properties and have proven their
utility in various learning contexts. They do not, however, live in a space
naturally endowed with a Hilbert structure and are usually compared with
specific distances, such as the bottleneck distance. To incorporate PDs in a
learning pipeline, several kernels have been proposed for PDs with a strong
emphasis on the stability of the RKHS distance w.r.t. perturbations of the PDs.
In this article, we use the Sliced Wasserstein approximation SW of the
Wasserstein distance to define a new kernel for PDs, which is not only provably
stable but also provably discriminative (depending on the number of points in
the PDs) w.r.t. the Wasserstein distance between PDs. We also demonstrate
its practicality, by developing an approximation technique to reduce kernel
computation time, and show that our proposal compares favorably to existing
kernels for PDs on several benchmarks.Comment: Minor modification
Semi-empirical catalog of early-type galaxy-halo systems: dark matter density profiles, halo contraction and dark matter annihilation strength
With SDSS galaxy data and halo data from up-to-date N-body simulations we
construct a semi-empirical catalog (SEC) of early-type systems by making a
self-consistent bivariate statistical match of stellar mass (M_star) and
velocity dispersion (sigma) with halo virial mass (M_vir). We then assign
stellar mass profile and velocity dispersion profile parameters to each system
in the SEC using their observed correlations with M_star and sigma.
Simultaneously, we solve for dark matter density profile of each halo using the
spherical Jeans equation. The resulting dark matter density profiles deviate in
general from the dissipationless profile of NFW or Einasto and their mean inner
density slope and concentration vary systematically with M_vir. Statistical
tests of the distribution of profiles at fixed M_vir rule out the null
hypothesis that it follows the distribution predicted by N-body simulations for
M_vir ~< 10^{13.5-14.5} M_solar. These dark matter profiles imply that dark
matter density is, on average, enhanced significantly in the inner region of
halos with M_vir ~< 10^{13.5-14.5} M_solar supporting halo contraction. The
main characteristics of halo contraction are: (1) the mean dark matter density
within the effective radius has increased by a factor varying systematically up
to ~ 3-4 at M_vir = 10^{12} M_solar, and (2) the inner density slope has a mean
of ~ 1.3 with rho(r) ~ r^{-alpha} and a halo-to-halo rms scatter of
rms(alpha) ~ 0.4-0.5 for 10^{12} M_solar ~< M_vir ~< 10^{13-14} M_solar steeper
than the NFW profile (alpha=1). Based on our results we predict that halos of
nearby elliptical and lenticular galaxies can, in principle, be promising
targets for gamma-ray emission from dark matter annihilation.Comment: 43 pages, 20 figures, JCAP, revised and accepted versio
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