1,150 research outputs found
Lattice results for D/Ds leptonic and semileptonic decays
This review article summarizes recent lattice QCD results for D and D_s meson leptonic and semileptonic decays. Knowing the meson decay constants and semileptonic form factors from theory, one can extract CKM elements V_cd and V_cs from experimental results. At present, the most accurate results for decay constants are from the Fermilab Lattice and MILC Collaborations: f_D=212.5±0.5_{stat}+0.6−1.5|_{syst} MeV and fDs=248.9±0.2_{stat}+0.5−1.6|_{syst} MeV, giving V_cd=0.2184±0.009_{expt}+0.0008−0.0016|_{lattice} and V_cs=1.017±0.02_{expt}+0.002−0.007|_{lattice}. The shapes of the semileptonic form factors from lattice QCD agree very well with experiment, and the accuracy is currently at the 2-5% level for D→πℓν and 1-2% for D→Kℓν. Extracting the CKM elements from the semileptonic decays yields V_cd=0.225(6)_{expt}(10)_{lattice} (HPQCD Collaboration) and V_cs=0.963(5)_{expt}(14)_{lattice} (HPQCD Collaboration). These lattice calculations also revealed that the semileptonic form factors are insensitive to whether the spectator quark is a light or strange quark
Energies of B_s meson excited states - a lattice study
This is a follow-up to our earlier work on the energies and radial
distributions of heavy-light mesons. The heavy quark is taken to be static
(infinitely heavy) and the light quark has a mass about that of the strange
quark. We now concentrate on the energies of the excited states with higher
angular momentum and with a radial node. A new improvement is the use of
hypercubic blocking in the time direction.
The calculation is carried out with dynamical fermions on a 16 cubed times 32
lattice with a lattice spacing approximately 0.1 fm generated using a
non-perturbatively improved clover action.
In nature the closest equivalent of this heavy-light system is the B_s meson,
which allows us to compare our lattice calculations to experimental results
(where available) or to give a prediction where the excited states,
particularly P-wave states, should lie. We pay special attention to the
spin-orbit splitting, to see which one of the states (for a given angular
momentum L) has the lower energy. An attempt is made to understand these
results in terms of the Dirac equation.Comment: 35 pages. v3: Data from two new lattices added. New results in
several chapter
Population imbalanced fermions in harmonically trapped optical lattices
The attractive Fermi-Hubbard Hamiltonian is solved via the Bogoliubov-de
Gennes formalism to analyze the ground state phases of population imbalanced
fermion mixtures in harmonically trapped two-dimensional optical lattices. In
the low density limit the superfluid order parameter modulates in the radial
direction towards the trap edges to accommodate the unpaired fermions that are
pushed away from the trap center with a single peak in their density. However
in the high density limit while the order parameter modulates in the radial
direction towards the trap center for low imbalance, it also modulates towards
the trap edges with increasing imbalance until the superfluid to normal phase
transition occurs beyond a critical imbalance. This leads to a single peak in
the density of unpaired fermions for low and high imbalance but leads to double
peaks for intermediate imbalance.Comment: 4 pages with 4 figures, accepted to appear in PR
P-wave Radial distributions of a Heavy-light meson on a lattice
This is a follow-up to our earlier work for the charge (vector) and matter
(scalar) distributions for S-wave states in a heavy-light meson, where the
heavy quark is static and the light quark has a mass about that of the strange
quark. The calculation is again carried out with dynamical fermions on a
16^3x24 lattice with a lattice spacing of about 0.14 fm. It is shown that
several features of the S- and P-wave distributions are in qualitative
agreement with what one expects from a simple one-body Dirac equation
interpretation.Comment: 5 pages, 2 figures, Quark Confinement and the Hadron Spectrum VI,
Sardinia, Italy, September, 200
Instability and wavelength selection during step flow growth of metal surfaces vicinal to fcc(001)
We study the onset and development of ledge instabilities during growth of
vicinal metal surfaces using kinetic Monte Carlo simulations. We observe the
formation of periodic patterns at [110] close packed step edges on surfaces
vicinal to fcc(001) under realistic molecular beam epitaxy conditions. The
corresponding wavelength and its temperature dependence are studied by
monitoring the autocorrelation function for step edge position. Simulations
suggest that the ledge instability on fcc(1,1,m) vicinal surfaces is controlled
by the strong kink Ehrlich-Schwoebel barrier, with the wavelength determined by
dimer nucleation at the step edge. Our results are in agreement with recent
continuum theoretical predictions, and experiments on Cu(1,1,17) vicinal
surfaces.Comment: 4 pages, 4 figures, RevTe
- …