Meson exchange currents in electromagnetic one-nucleon emission

The role of meson exchange currents (MEC) in electron- and photon-induced one-nucleon emission processes is studied in a nonrelativistic model including correlations and final state interactions. The nuclear current is the sum of a one-body and of a two-body part. The two-body current includes pion seagull, pion-in-flight and the isobar current contributions. Numerical results are presented for the exclusive 16O(e,e'p)15N and 16O(\gamma,p)15N reactions. MEC effects are in general rather small in (e,e'p), while in (\gamma,p) they are always large and important to obtain a consistent description of (e,e'p) and (\gamma,p) data, with the same spectroscopic factors. The calculated (\gamma,p) cross sections are sensitive to short-range correlations at high values of the recoil momentum, where MEC effects are larger and overwhelm the contribution of correlations.Comment: 9 pages, 6 figure

Overlap functions in correlation methods and quasifree nucleon knockout from 16^{16}O

The cross sections of the ($e,e'N$) and ($\gamma,p$) reactions on $^{16}$O are calculated, for the transitions to the $1/2^{-}$ ground state and the first $3/2^{-}$ excited state of the residual nucleus, using single-particle overlap functions obtained on the basis of one-body density matrices within different correlation methods. The electron-induced one-nucleon knockout reaction is treated within a nonrelativistic DWIA framework. The theoretical treatment of the ($\gamma,p$) reaction includes both contributions of the direct knockout mechanism and of meson-exchange currents. The results are sensitive to details of the different overlap functions. The consistent analysis of the reaction cross sections and the comparison with the experimental data make it possible to study the nucleon--nucleon correlation effects.Comment: 26 pages, LaTeX, 5 Postscript figures, submitted to PR

Relativistic corrections in (gamma,N) knockout reactions

We develop a fully relativistic DWIA model for photonuclear reactions using the relativistic mean field theory for the bound state and the Pauli reduction of the scattering state which is calculated from a relativistic optical potential. Results for the 12C(gamma,p) and 16O(gamma,p) differential cross sections and photon asymmetries are displayed in a photon energy range between 60 and 257 MeV, and compared with nonrelativistic DWIA calculations. The effects of the spinor distortion and of the effective momentum approximation for the scattering state are discussed. The sensitivity of the model to different prescriptions for the one-body current operator is investigated. The off-shell ambiguities are large in (gamma,p) calculations, and even larger in (gamma,n) knockout.Comment: LaTeX2e, 18 pages, and 6 figure

Surto de intoxicação por narasina em suínos An outbreak of narasin poisoning in swine

Descreve-se um surto de intoxicação por narasina em suínos, cujo diagnóstico baseou-se no histórico, quadro clínico-patológico, na reprodução da enfermidade pela experimentação com a ração comercial originalmente oferecida aos suínos, bem como pelo exame químico posterior que detectou narasina em quantidades suficientemente elevadas para causar intoxicação. Apesar de os quadros clínico-patológicos das intoxicações natural e experimental serem da mesma natureza, houve algumas diferenças. Nos casos naturais o índice de letalidade foi elevado, enquanto que na intoxicação experimental nenhum animal morreu. Os exames histopatológicos revelaram, em parte dos casos naturais, além das lesões dos músculos estriados, também lesões nas fibras musculares cardíacas, últimas não verificadas nos casos experimentais. Sugere-se que essas diferenças poderiam ser explicadas pelo estresse ao qual os animais eram submetidos na granja pelo grande número de animais nas baias, ao contrário dos animais experimentais que eram mantidos em compartimentos individuais.<br>An outbreak of narasin poisoning in swine is described. The diagnosis was based on the history, clinical-pathological findings, the reproduction of the disease by the administration of the feed originally given to the animals and by chemical analysis which showed doses sufficiently high to cause poisoning. Inspite that the clinical-pathological picture of the natural and experimental poisoning was of the same nature, there were some differences. In the natural outbreak lethality was high, but in the experiments none of the animals died. In the natural cases besides the lesions in the muscles, also lesions of the heart muscle fibres were seen, not detected in the esperimental animals. It is suggested that these differences could be due to the stress to which the animals were submitted in the piggery by the great number of animals per box, whereas the experimental animals were kept individually