843 research outputs found
On the I=2 channel pi-pi interaction in the chiral limit
An approximate local potential for the residual pi+ pi+ interaction is
computed. We use an O(a**2) improved action on a coarse 9x9x9x13 lattice with
approximately a=0.4fm. The results present a continuation of previous work:
Increasing the number of gauge configurations and quark propagators we attempt
extrapolation of the pi+ pi+ potential to the chiral limit.Comment: LATTICE98(spectrum) LaTeX2e, 3 pages, 3 eps figure
Extraction of hadron-hadron potentials on the lattice within 2+1 dimensional QED
A potential between mesons is extracted from 4-point functions within lattice
gauge theory taking 2+1 dimensional QED as an example. This theory possesses
confinement and dynamical fermions. The resulting meson-meson potential has a
short-ranged hard repulsive core due to antisymmetrization. The expected
dipole-dipole forces lead to attraction at intermediate distances. Sea quarks
lead to a softer form of the total potential.Comment: 12 pages, uuencoded tar-compressed postscript fil
On the nature of the residual meson-meson interaction from simulations with a QED model
A potential between mesons is extracted from 4-point functions within lattice
gauge theory taking 2+1 dimensional QED as an example. This theory possesses
confinement and dynamical fermions. The resulting meson-meson potential has a
short-ranged hard repulsive core and the expected dipole-dipole forces lead to
attraction at intermediate distances. Sea quarks lead to a softer form of the
total potential.Comment: 4 pages, uuencoded tar-compressed postscript file, contribution to
Lattice'9
Two-body spectra of pseudoscalar mesons with an --improved lattice action using Wilson fermions
We extend our calculations with the second-order tree-level and tadpole
improved next-nearest-neighbor action to meson-meson systems. Correlation
matrices built from interpolating fields representing two pseudoscalar mesons
(pion-pion) with relative momenta p are diagonalized, and the mass spectrum is
extracted. Link variable fuzzing and operator smearing at both sinks and
sources is employed. Calculations are presented for two values of the hopping
parameter. The spectrum is used to discuss the residual interaction in the
meson-meson system.Comment: 3 pages, 4 EPS figures, Poster presented at "Lattice'97", to appear
in the proceeding
Potentials between heavy-light mesons from lattice and inverse scattering theory
We extend our investigation of heavy-light meson-meson interactions to a
system consisting of a heavy-light meson and the corresponding antiparticle. An
effective potential is obtained from meson-antimeson Green-functions computed
in a quenched simulation with staggered fermions. Comparisons with a simulation
using an tree-level and tadpole improved gauge action and a full QCD
simulation show that lattice discretization errors and dynamical quarks have no
drastic influence. Calculations from inverse scattering theory propose a
similar shape for potentials.Comment: 3 pages, 5 EPS figures, Poster presented at "Lattice'97", to appear
in the proceeding
Exploring the pi+ pi+ interaction in lattice QCD
An effective residual interaction for a meson-meson system is computed in
lattice QCD. We describe the theoretical framework and present its application
to the I=2 channel S-wave interaction of the pi pi system. Scattering phase
shifts are also computed and compared to experimental results.Comment: LaTeX2e, 29 pages, 14 eps figure
Meson-meson interactions -- from static to dynamic valence quarks
A method for the extraction of an effective meson-meson potential from Green
functions, which can be obtained from a lattice simulation, is presented.
Simulations are carried out for compact QED and QCD in four dimensions using
the quenched approximation and the hopping parameter expansion. In a further
study, a heavy-light meson is considered employing a conjugate gradient
algorithm for the light propagators. Due to the Pauli exclusion principle, the
results for QED indicate the existence of a hard core, but for QCD there is
strong attraction at small meson distances.Comment: 4 pages, uuencoded gziped postscript file, contribution to
LATTICE'95, Melbourne, Australia (list of authors completed
Influence of strain on magnetization and magnetoelectric effect in La0.7A0.3MnO3 / PMN-PT(001) (A = Sr; Ca)
We investigate the influence of a well-defined reversible biaxial strain
<=0.12 % on the magnetization (M) of epitaxial ferromagnetic manganite films. M
has been recorded depending on temperature, strain and magnetic field in 20 -
50 nm thick films. This is accomplished by reversibly compressing the isotropic
in-plane lattice parameter of the rhombohedral piezoelectric 0.72PMN-0.28PT
(001) substrates by application of an electric field E <= 12 kV cm-1. The
magnitude of the total variable in-plane strain has been derived.
Strain-induced shifts of the ferromagnetic Curie temperature (Tc) of up to 19 K
were found in La0.7Sr0.3MnO3 (LSMO) and La0.7Ca0.3MnO3 films and are
quantitatively analysed for LSMO within a cubic model. The observed large
magnetoelectric coupling coefficient alpha=mu0 dM/dE <= 6 10-8 s m-1 at ambient
temperature results from the strain-induced M change in the
magnetic-film-ferroelectric-substrate system. It corresponds to an enhancement
of mu0 DeltaM <= 19 mT upon biaxial compression of 0.1 %. The extraordinary
large alpha originates from the combination of three crucial properties: (i)
the strong strain dependence of M in the ferromagnetic manganites, (ii) large
piezo-strain of the PMN-PT substrates and (iii) effective elastic coupling at
the film-substrate interface.Comment: 15 pages, 6 figures, 1 tabl
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