389 research outputs found
Pairwise wave interactions in ideal polytropic gases
We consider the problem of resolving all pairwise interactions of shock
waves, contact waves, and rarefaction waves in 1-dimensional flow of an ideal
polytropic gas. Resolving an interaction means here to determine the types of
the three outgoing (backward, contact, and forward) waves in the Riemann
problem defined by the extreme left and right states of the two incoming waves,
together with possible vacuum formation. This problem has been considered by
several authors and turns out to be surprisingly involved. For each type of
interaction (head-on, involving a contact, or overtaking) the outcome depends
on the strengths of the incoming waves. In the case of overtaking waves the
type of the reflected wave also depends on the value of the adiabatic constant.
Our analysis provides a complete breakdown and gives the exact outcome of each
interaction.Comment: 39 page
Localization of interacting electrons in quantum dot arrays driven by an ac-field
We investigate the dynamics of two interacting electrons moving in a
one-dimensional array of quantum dots under the influence of an ac-field. We
show that the system exhibits two distinct regimes of behavior, depending on
the ratio of the strength of the driving field to the inter-electron Coulomb
repulsion. When the ac-field dominates, an effect termed coherent destruction
of tunneling occurs at certain frequencies, in which transport along the array
is suppressed. In the other, weak-driving, regime we find the surprising result
that the two electrons can bind into a single composite particle -- despite the
strong Coulomb repulsion between them -- which can then be controlled by the
ac-field in an analogous way. We show how calculation of the Floquet
quasienergies of the system explains these results, and thus how ac-fields can
be used to control the localization of interacting electron systems.Comment: 7 pages, 6 eps figures V2. Minor changes, this version to be
published in Phys. Rev.
Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. IX: Constraint of pairing force to neutron-matter gap
In this latest of our series of Skyrme-HFB mass models, HFB-16, we introduce
the new feature of requiring that the contact pairing force reproduce at each
density the pairing gap of neutron matter as determined in microscopic
calculations with realistic nucleon-nucleon forces. We retain the earlier
constraints on the Skyrme force of reproducing the energy-density curve of
neutron matter, and of having an isoscalar effective mass of in
symmetric infinite nuclear matter at the saturation density; we also keep the
recently adopted device of dropping Coulomb exchange. Furthermore, the
correction term for the spurious energy of collective motion has a form that is
known to favour fission barriers that are in good agreement with experiment.
Despite the extra constraints on the effective force, we have achieved a better
fit to the mass data than any other mean field model, the rms error on the 2149
measured masses of nuclei with and 8 having been reduced to 0.632
MeV; the improvement is particularly striking for the most neutron-rich nuclei.
Moreover, it turns out that even with no flexibility at all remaining for the
pairing force, the spectral pairing gaps that we find suggest that level
densities in good agreement with experiment should be obtained. This new force
is thus particularly well-suited for astrophysical applications, such as
stellar nucleosynthesis and neutron-star crusts.Comment: 38 pages, 9 figures accepted for publication in Nuclear Physics
Relativistic chiral representation of the scattering amplitude I: The Goldberger-Treiman relation
In this work we study the scattering process within the Baryon Chiral
Perturbation Theory framework in the covariant scheme of Extended-On-Mass-Shell
(EOMS).
We compare the description obtained in this scheme with the previously
obtained using the Infrared Regularization scheme and show that EOMS
accomplishes the best convergence, being able to extract from partial wave
analyses reliable values of important quantities as the Goldberger-Treiman
deviation. In regard to the latter, we solve the long-standing problem
concerning to the extraction of the Goldberger-Treiman deviation with covariant
ChPT that jeopardized the applicability of ChPT to the system.
We also show the potential of the unitarization techniques applied to the
perturbative calculation in the EOMS scheme, that allow us to increase the
range of validity of our description up to MeV in .Comment: PROCEEDINGS to the 33rd International School of Nuclear Physics "From
Quarks and Gluons to Hadrons and Nuclei"- 7 Pag,, 1 Table, 4 Figures.
Erice-Sicily: 16 - 24 September 201
Large-scale magnetic fields from inflation due to a -even Chern-Simons-like term with Kalb-Ramond and scalar fields
We investigate the generation of large-scale magnetic fields due to the
breaking of the conformal invariance in the electromagnetic field through the
-even dimension-six Chern-Simons-like effective interaction with a fermion
current by taking account of the dynamical Kalb-Ramond and scalar fields in
inflationary cosmology. It is explicitly demonstrated that the magnetic fields
on 1Mpc scale with the field strength of G at the present time
can be induced.Comment: 18 pages, 6 figures, version accepted for publication in Eur. Phys.
J.
Slowing polar molecules using a wire Stark decelerator
We have designed and implemented a new Stark decelerator based on wire
electrodes, which is suitable for ultrahigh vacuum applications. The 100
deceleration stages are fashioned out of 0.6 mm diameter tantalum and the
array's total length is 110 mm, approximately 10 times smaller than a
conventional Stark decelerator with the same number of electrode pairs. Using
the wire decelerator, we have removed more than 90% of the kinetic energy from
metastable CO molecules in a beam.Comment: updated version, added journal referenc
Location of crossings in the Floquet spectrum of a driven two-level system
Calculation of the Floquet quasi-energies of a system driven by a
time-periodic field is an efficient way to understand its dynamics. In
particular, the phenomenon of dynamical localization can be related to the
presence of close approaches between quasi-energies (either crossings or
avoided crossings). We consider here a driven two-level system, and study how
the locations of crossings in the quasi-energy spectrum alter as the field
parameters are changed. A perturbational scheme provides a direct connection
between the form of the driving field and the quasi-energies which is exact in
the limit of high frequencies. We firstly obtain relations for the
quasi-energies for some common types of applied field in the high-frequency
limit. We then show how the locations of the crossings drift as the frequency
is reduced, and find a simple empirical formula which describes this drift
extremely well in general, and appears to be exact for the specific case of
square-wave driving.Comment: 6 pages, 6 figures. Minor changes to text, this version to be
published in Physical Review
Photoproduction of the f2(1270) resonance
We have performed a calculation of the γp→π+π−p reaction, where the two pions have been separated in D-wave producing the f2(1270) resonance. We use elements of the local hidden gauge approach that provides the interaction of vector mesons in which the f2(1270) resonance appears as a ρ-ρ molecular state in L=0 and spin 2. The vector meson dominance, incorporated in the local hidden gauge approach converts a photon into a ρ0 meson and the other meson connects the photon with the proton. The picture is simple and has no free parameters, since the parameters of the theory have been constrained in the previous study of the vector-vector states. In a second step we introduce new elements, not present in the local hidden gauge approach, adapting the ρ propagator to Regge phenomenology and introducing the ρNN tensor coupling. We find that both the differential cross section as well as the t dependence of the cross section are in good agreement with the experimental results and provide support for the molecular picture of the f2(1270) in the first baryonic reaction where it has been tested
Charmless hadronic decays and new physics effects in the general two-Higgs doublet models
Based on the low-energy effective Hamiltonian with the generalized
factorization, we calculate the new physics contributions to the branching
ratios of the two-body charmless hadronic decays of and mesons
induced by the new gluonic and electroweak charged-Higgs penguin diagrams in
the general two-Higgs doublet models (models I, II and III). Within the
considered parameter space, we find that: (a) the new physics effects from new
gluonic penguin diagrams strongly dominate over those from the new -
and - penguin diagrams; (b) in models I and II, new physics contributions
to most studied B meson decay channels are rather small in size: from -15% to
20%; (c) in model III, however, the new physics enhancements to the
penguin-dominated decay modes can be significant, , and
therefore are measurable in forthcoming high precision B experiments; (d) the
new physics enhancements to ratios {\cal B}(B \to K \etap) are significant in
model III, , and hence provide a simple and plausible new
physics interpretation for the observed unexpectedly large B \to K \etap
decay rates; (e) the theoretical predictions for and
in model III are still consistent with the data
within errors; (f) the significant new physics enhancements to the
branching ratios of and decays are helpful to improve the
agreement between the data and the theoretical predictions; (g) the theoretical
predictions of in the 2HDM's are generally
consistent with experimental measurements and upper limits ()Comment: 55 pages, Latex file, 17 PS and EPS figures. With minor corrections,
final version to be published in Phys.Rev. D. Repot-no: PKU-TH-2000-4
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