759 research outputs found
Zero-temperature generalized phase diagram of the 4d transition metals under pressure
We use an accurate implementation of density functional theory (DFT) to
calculate the zero-temperature generalized phase diagram of the 4 series of
transition metals from Y to Pd as a function of pressure and atomic number
. The implementation used is full-potential linearized augmented plane waves
(FP-LAPW), and we employ the exchange-correlation functional recently developed
by Wu and Cohen. For each element, we obtain the ground-state energy for
several crystal structures over a range of volumes, the energy being converged
with respect to all technical parameters to within meV/atom. The
calculated transition pressures for all the elements and all transitions we
have found are compared with experiment wherever possible, and we discuss the
origin of the significant discrepancies. Agreement with experiment for the
zero-temperature equation of state is generally excellent. The generalized
phase diagram of the 4 series shows that the major boundaries slope towards
lower with increasing for the early elements, as expected from the
pressure induced transfer of electrons from states to states, but are
almost independent of for the later elements. Our results for Mo indicate a
transition from bcc to fcc, rather than the bcc-hcp transition expected from
- transfer.Comment: 28 pages and 10 figures. Submitted to Phys. Rev.
The Peculiar Motions of Early-Type Galaxies in Two Distant Regions -- V. The Mg-- Relation, Age and Metallicity
We have examined the MgâÏ relation for early-type galaxies in the EFAR sample and its dependence on cluster properties. A comprehensive maximum likelihood treatment of the sample selection and measurement errors gives fits to the global MgâÏ relation of Mg bâČ=0.131 log Ï â0.131 and Mg2=0.257 log Ï â0.305. The slope of these relations is 25 per cent steeper than that obtained by most other authors owing to the reduced bias of our fitting method. The intrinsic scatter in the global Mgâ Ï relation is estimated to be 0.016 mag in Mg bâČ and 0.023 mag in Mg2. The Mgâ Ï relation for cD galaxies has a higher zero-point than for E and S0 galaxies, implying that cDs are older and/or more metal-rich than other early-type galaxies with the same velocity dispersion.
We investigate the variation in the zero-point of the Mgâ Ï relation between clusters. We find that it is consistent with the number of galaxies observed per cluster and the intrinsic scatter between galaxies in the global MgâÏ relation. We find no significant correlation between the MgâÏ zero-point and the cluster velocity dispersion, X-ray luminosity or X-ray temperature over a wide range in cluster mass. These results provide constraints for models of the formation of elliptical galaxies. However, the MgâÏ relation on its own does not place strong limits on systematic errors in Fundamental Plane (FP) distance estimates resulting from stellar population differences between clusters.
We compare the intrinsic scatter in the MgâÏ and Fundamental Plane relations with stellar population models in order to constrain the dispersion in ages, metallicities and M/L ratios for early-type galaxies at fixed velocity dispersion. We find that variations in age or metallicity alone cannot explain the measured intrinsic scatter in both Mgâ Ï and the FP. We derive the joint constraints on the dispersion in age and metallicity implied by the scatter in the MgâÏ and FP relations for a simple Gaussian model. We find upper limits on the dispersions in age and metallicity at fixed velocity dispersion of 32 per cent in ÎŽ t/t and 38 per cent in ÎŽ Z/Z if the variations in age and metallicity are uncorrelated; only strongly anticorrelated variations lead to significantly higher upper limits. The joint distribution of residuals from the Mgâ Ï and FP relations is only marginally consistent with a model having no correlation between age and metallicity, and is better matched by a model in which age and metallicity variations are moderately anticorrelated (ÎŽ t/t â 40 per cent, ÎŽ Z/Z â 50 per cent and Ïâ â0.5), with younger galaxies being more metal-rich
The peculiar motions of early-type galaxies in two distant regions - VII. Peculiar velocities and bulk motions
We present peculiar velocities for 84 clusters of galaxies in two large
volumes at distances between 6000 and 15000 km/s in the directions of
Hercules-Corona Borealis and Perseus-Pisces-Cetus. These velocities are based
on Fundamental Plane (FP) distance estimates for early-type galaxies in each
cluster. We fit the FP using a maximum likelihood algorithm which accounts for
both selection effects and measurement errors, and yields FP parameters with
smaller bias and variance than other fitting procedures. We find a best-fit FP
with coefficients consistent with the best existing determinations. We measure
the bulk motions of the sample volumes using the 50 clusters with the
best-determined peculiar velocities. We find the bulk motions in both regions
are small, and consistent with zero at about the 5% level. The EFAR results are
in agreement with the small bulk motions found by Dale et al. (1999) on similar
scales, but are inconsistent with pure dipole motions having the large
amplitudes found by Lauer & Postman (1994) and Hudson et al. (1999). The
alignment of the EFAR sample with the Lauer & Postman dipole produces a strong
rejection of a large-amplitude bulk motion in that direction, but the rejection
of the Hudson et al. result is less certain because their dipole lies at a
large angle to the main axis of the EFAR sample. We find the bulk motion of our
sample is consistent with most cosmological models that approximately reproduce
the shape and normalisation of the observed galaxy power spectrum. We conclude
that existing measurements of large-scale bulk motions provide no significant
evidence against standard models for the formation of structure.Comment: to appear in MNRAS, 27 pages, EFAR paper
Combined local-density and dynamical mean field theory calculations for the compressed lanthanides Ce, Pr, and Nd
This paper reports calculations for compressed Ce (4f^1), Pr (4f^2), and Nd
(4f^3) using a combination of the local-density approximation (LDA) and
dynamical mean field theory (DMFT), or LDA+DMFT. The 4f moment, spectra, and
the total energy among other properties are examined as functions of volume and
atomic number for an assumed face-centered cubic (fcc) structure.Comment: 15 pages, 9 figure
Calibration of Plastic Phoswich Detectors for Charged Particle Detection
The response of an array of plastic phoswich detectors to ions of has been measured from =12 to 72 MeV. The detector response has been
parameterized by a three parameter fit which includes both quenching and high
energy delta-ray effects. The fits have a mean variation of with
respect to the data.Comment: 17 pages, 5 figure
Condensation Energy and Spectral Functions in High Temperature Superconductors
If high temperature cuprate superconductivity is due to electronic
correlations, then the energy difference between the normal and superconducting
states can be expressed in terms of the occupied part of the single particle
spectral function. The latter can, in principle, be determined from angle
resolved photoemission (ARPES) data. As a consequence, the energy gain driving
the development of the superconducting state is intimately related to the
dramatic changes in the photoemission lineshape when going below Tc. These
points are illustrated in the context of the "mode" model used to fit ARPES
data in the normal and superconducting states, where the question of kinetic
energy versus potential energy driven superconductivity is explored in detail.
We use our findings to comment on the relation of ARPES data to the
condensation energy, and to various other experimental data. In particular, our
results suggest that the nature of the superconducting transition is strongly
related to how anomalous (non Fermi liquid like) the normal state spectral
function is, and as such, is dependent upon the doping level.Comment: 10 pages, revtex, 4 encapsulated postscript figure
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