24,200 research outputs found
Measuring and engineering entropy and spin squeezing in weakly linked Bose-Einstein condensates
We propose a method to infer the single-particle entropy of bosonic atoms in
an optical lattice and to study the local evolution of entropy, spin squeezing,
and entropic inequalities for entanglement detection in such systems. This
method is based on experimentally feasible measurements of
non-nearest-neighbour coherences. We study a specific example of dynamically
controlling atom tunneling between selected sites and show that this could
potentially also improve the metrologically relevant spin squeezing
Classical bifurcation at the transition from Rabi to Josephson dynamics
We report on the experimental realization of an internal bosonic Josephson
junction in a Rubidium spinor Bose-Einstein condensate. The measurement of the
full time dynamics in phase space allows the characterization of the
theoretically predicted -phase modes and quantitatively confirms
analytical predictions, revealing a classical bifurcation. Our results suggest
that this system is a model system which can be tuned from classical to the
quantum regime and thus is an important step towards the experimental
investigation of entanglement generation close to critical points
Exact renormalization group equations and the field theoretical approach to critical phenomena
After a brief presentation of the exact renormalization group equation, we
illustrate how the field theoretical (perturbative) approach to critical
phenomena takes place in the more general Wilson (nonperturbative) approach.
Notions such as the continuum limit and the renormalizability and the presence
of singularities in the perturbative series are discussed.Comment: 15 pages, 7 figures, to appear in the Proceedings of the 2nd
Conference on the Exact Renormalization Group, Rome 200
Photoelectron spectra of anionic sodium clusters from time-dependent density-functional theory in real-time
We calculate the excitation energies of small neutral sodium clusters in the
framework of time-dependent density-functional theory. In the presented
calculations, we extract these energies from the power spectra of the dipole
and quadrupole signals that result from a real-time and real-space propagation.
For comparison with measured photoelectron spectra, we use the ionic
configurations of the corresponding single-charged anions. Our calculations
clearly improve on earlier results for photoelectron spectra obtained from
static Kohn-Sham eigenvalues
Formation of nanosized strontium substituted hydroxyapatites
Incorporation of specific elements into calcium phosphates offers the combination of a bioactive material and a therapeutic effect. This is important for improving the integration of implants as well as treating medical conditions. Strontium is a suitable candidate and displays the ability to stimulate bone growth and reducing bone resorption. This study investigated the formation of strontium carbonated hydroxyapatite nanoparticles from an amorphous phase. Crystallization of carbonated hydroxyapatite occurred at 585 oC, but samples with an intended 25% and 75% replacement of calcium with strontium crystallized at 624 oC. Heat treatment at the crystallization temperature revealed that strontium free apatite does not crystallize in 5 minutes, but an increasing strontium concentration leads to a higher rate of crystallization. X-ray diffraction patterns suggest that it may be difficult to include strontium, but higher strontium concentrations are possibly included with ease in the lattice. This work has produced a nanosized apatite accompanied by an amorphous phase after a short heat-treatment time. This offers a range of features that collectively show great promise for significantly enhancing the release of strontium for improved bone therapeutic effects
Large magnetocrystalline anisotropy in tetragonally distorted Heuslers: a systematic study
With a view to the design of hard magnets without rare earths we explore the
possibility of large magnetocrystalline anisotropy energies in Heusler
compounds that are unstable with respect to a tetragonal distortion. We
consider the Heusler compounds FeYZ with Y = (Ni, Co, Pt), and CoYZ
with Y = (Ni, Fe, Pt) where, in both cases, Z = (Al, Ga, Ge, In, Sn). We find
that for the CoNiZ, CoPtZ, and FePtZ families the cubic phase is
always, at , unstable with respect to a tetragonal distortion, while, in
contrast, for the FeNiZ and FeCoZ families this is the case for only 2
compounds -- FeCoGe and FeCoSn. For all compounds in which a tetragonal
distortion occurs we calculate the MAE finding remarkably large values for the
Pt containing Heuslers, but also large values for a number of the other
compounds (e.g. CoNiGa has an MAE of -2.11~MJ/m). The tendency to a
tetragonal distortion we find to be strongly correlated with a high density of
states at the Fermi level in the cubic phase. As a corollary to this fact we
observe that upon doping compounds for which the cubic structure is stable such
that the Fermi level enters a region of high DOS, a tetragonal distortion is
induced and a correspondingly large value of the MAE is then observed.Comment: 8 pages, 5 figure
Non-adiabatic electron dynamics in time-dependent density-functional theory
Time-dependent density-functional theory (TDDFT) treats dynamical exchange
and correlation (xc) via a single-particle potential, Vxc(r,t), defined as a
nonlocal functional of the density n(r',t'). The popular adiabatic
local-density approximation (ALDA) for Vxc(r,t) uses only densities at the same
space-time point (r,t). To go beyond the ALDA, two local approximations have
been proposed based on quantum hydrodynamics and elasticity theory: (a) using
the current as basic variable (C-TDDFT) [G. Vignale, C. A. Ullrich, and S.
Conti, Phys. Rev. Lett. 79, 4878 (1997)], (b) working in a co-moving Lagrangian
reference frame (L-TDDFT) [I. V. Tokatly, Phys. Rev. B 71, 165105 (2005)]. This
paper illustrates, compares, and analyzes both non-adiabatic theories for
simple time-dependent model densities in the linear and nonlinear regime, for a
broad range of time and frequency scales. C- and L-TDDFT are identical in
certain limits, but in general exhibit qualitative and quantitative differences
in their respective treatment of elastic and dissipative electron dynamics. In
situations where the electronic density rapidly undergoes large deformations,
it is found that non-adiabatic effects can become significant, causing the ALDA
to break down.Comment: 15 pages, 15 figure
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