dc.contributor.author | Goldberg, V. Z. | |
dc.contributor.author | Gazeeva, E. M. | |
dc.contributor.author | Golovkov, M. S. | |
dc.contributor.author | Bezbakh, A. A. | |
dc.contributor.author | Nauruzbayev, D. K. | |
dc.contributor.author | Nurmukhanbetova, A. K. | |
dc.contributor.author | Kurmanaliyev, Zh. | |
dc.contributor.author | Serikov, A. | |
dc.contributor.author | Zalewski, B. | |
dc.contributor.author | Rogachev, G. V. | |
dc.date.accessioned | 2025-01-27T12:06:20Z | |
dc.date.available | 2025-01-27T12:06:20Z | |
dc.date.issued | 2020 | |
dc.identifier.issn | 2643-1564 | |
dc.identifier.other | DOI: 10.1103/PhysRevResearch.2.032036 | |
dc.identifier.uri | http://rep.enu.kz/handle/enu/21212 | |
dc.description.abstract | We applied the thick target inverse kinematics method for a study of resonances decaying through neutron emission. In this approach, the time of flight of the resonant neutrons is defined by the movement of the heavy ions of low-energy beams through an extended target. As a test, we used a well-studied, because of its role in the s process in stars, 13C(α, n) reaction. The measurements demonstrated the high efficiency of the approach. The energy resolution for the 13C(α, n) excitation function was ≈60 keV, the largest contributions coming from the time structure of the beam and the thickness of the neutron detector. The measurements revealed a surprising disagreement with the R-matrix calculations based on the parameters of the recent analysis. | ru |
dc.language.iso | en | ru |
dc.publisher | PHYSICAL REVIEW RESEARCH | ru |
dc.relation.ispartofseries | 2, 032036; | |
dc.title | Thick target inverse kinematics approach for neutron emission | ru |
dc.type | Article | ru |