42 research outputs found
Električni faktor oblika neutrona pomoću odbojne polarimetrije
Jefferson Lab experiment 93–038 is designed to measure the ratio of the electric to the magnetic form-factor of the neutron from the quasielastic 2H(~e, e ′~n)1H reaction.Za mjerenje omjera električnog i magnetskog faktora oblika neutrona pomoću kvazielastične reakcije 2H(~e, e ′~n)1H postavljen je eksperiment Jefferson Lab 93–038
Električni faktor oblika neutrona pomoću odbojne polarimetrije
Jefferson Lab experiment 93–038 is designed to measure the ratio of the electric to the magnetic form-factor of the neutron from the quasielastic 2H(~e, e ′~n)1H reaction.Za mjerenje omjera električnog i magnetskog faktora oblika neutrona pomoću kvazielastične reakcije 2H(~e, e ′~n)1H postavljen je eksperiment Jefferson Lab 93–038
Inclusive neutron cross-sections at forward angles from Nb Nb and Au Au collisions at 800-MeV/nucleon
Inclusive neutron spectra were measured at 0°, 4°, 8°, 15°, 30°, and 42° from Nb-Nb and Au-Au collisions at 800 MeV/nucleon. A peak that originates from neutron evaporation from the projectile appears in the spectra at angles out to 8°. The shapes and magnitudes of the spectra are compared with those calculated from models of nucleus-nucleus collisions. The differential cross sections for Au-Au collisions are about four times those for Nb-Nb collisions. The predictions of the Vlasov-Uehling-Uhlenbeck (VUU) and QMD theories agree with the angular distributions of the differential cross sections except at small angles; the VUU prediction overestimates the angular distributions from a few degrees to about 20°, whereas the QMD prediction underestimates the angular distributions below 8°. The Firestreak model overestimates the angular distribution for Nb-Nb collisions and underestimates it for Au-Au collisions. Also, the VUU and QMD models agree with the measured double-differential cross sections in more angular and energy regions than the Firestreak and intranuclear cascade models; however, none of the models can account for the peaks at small angles (θ≤15°)
Effect of recent R_p and R_n measurements on extended Gari-Krumpelmann model fits to nucleon electromagnetic form factors
The Gari-Krumpelmann (GK) models of nucleon electromagnetic form factors, in
which the rho, omega, and phi vector meson pole contributions evolve at high
momentum transfer to conform to the predictions of perturbative QCD (pQCD), was
recently extended to include the width of the rho meson by substituting the
result of dispersion relations for the pole and the addition of rho' (1450)
isovector vector meson pole. This extended model was shown to produce a good
overall fit to all the available nucleon electromagnetic form factor (emff)
data. Since then new polarization data shows that the electric to magnetic
ratios R_p and R_n obtained are not consistent with the older G_{Ep} and G_{En}
data in their range of momentum transfer. The model is further extended to
include the omega' (1419) isoscalar vector meson pole. It is found that while
this GKex cannot simultaneously fit the new R_p and the old G_{En} data, it can
fit the new R_p and R_n well simultaneously. An excellent fit to all the
remaining data is obtained when the inconsistent G_{Ep} and G_{En} is omitted.
The model predictions are shown up to momentum transfer squared, Q^2, of 8
GeV^2/c^2.Comment: 14 pages, 8 figures, using RevTeX4; email correspondence to
[email protected] ; minor typos corrected, figures added, conclusions
extende
Nucleon electromagnetic form factors in a quark-gluon core model
We study the nucleon electromagnetic form factors in a quark-gluon core model
framework, which can be viewed as an extension of the Isgur-Karl model of
baryons. Using this picture we derive nucleon electromagnetic dipole form
factors at low Q^2 and the deviation from the dipole form at high Q^2, that are
consistent with the existing experimental data.Comment: 5 pages, 3 figure
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