Parameters of Fermi-motion from Quasielastic Backward Pion-Proton Scattering on Nuclei
| dc.creator | Abramov, B. M. | |
| dc.creator | Bulychjov, S. A. | |
| dc.creator | Dukhovskoy, I. A. | |
| dc.creator | Khanov, A. I. | |
| dc.creator | Krestnikov, Y. S. | |
| dc.creator | Krutenkova, A. P. | |
| dc.creator | Kulikov, V. V. | |
| dc.creator | Matsuk, M. A. | |
| dc.creator | Radkevich, I. A. | |
| dc.creator | Turdakina, E. N. | |
| dc.date | 1999-07-19 | |
| dc.date | 1999-07-20 | |
| dc.date.accessioned | 2026-07-07T05:37:50Z | |
| dc.date.available | 2026-07-07T05:37:50Z | |
| dc.description | In experiment on the study of the quasielastic pion-proton scattering at large momentum transfer on nuclei the proton Fermi-momentum distributions have been analysed in plane-wave approximation for light nuclei $^6$Li, $^7$Li and $^{12}$C. It was found that, contrary to (e,e') experiments, that the oscillator model gives slightly better description of our data than the Fermi - gas model. But the values of parameters of the distributions obtained in our analysis are considerably smaller, than in (e,e') experiments. It gives evidence that the plane-wave approximation is not sufficient and more complicated theoretical models which take into account the effects of distortion of pion-nucleon amplitude in a nuclear medium are necessary for analysis of our data. | |
| dc.description | 6 pages, 4 figures | |
| dc.identifier | https://arxiv.org/abs/nucl-ex/9907011 | |
| dc.identifier | http://arxiv.org/abs/nucl-ex/9907011 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/81416 | |
| dc.subject | Nuclear Experiment | |
| dc.title | Parameters of Fermi-motion from Quasielastic Backward Pion-Proton Scattering on Nuclei | |
| dc.type | text |