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dc.contributor.authorErdemchimeg, B.
dc.contributor.authorArtukh, A.G.
dc.contributor.authorDavaa, S.
dc.contributor.authorHue, B.M.
dc.contributor.authorIsataev, T.
dc.contributor.authorKlygin, S.A.
dc.contributor.authorKononenko, G.A.
dc.contributor.authorKhuukhenkhuu, G.
dc.contributor.authorLukyanov, S.M.
dc.contributor.authorMikhailova, T.I.
dc.contributor.authorMaslov, V.A.
dc.contributor.authorMendibaev, K.
dc.contributor.authorSereda, Yu.M.
dc.contributor.authorPenionzhkevich, Yu.E.
dc.contributor.authorVorontzov, A.N.
dc.date.accessioned2023-12-04T09:14:18Z
dc.date.available2023-12-04T09:14:18Z
dc.date.issued2019
dc.identifier.otherDOI: 10.29317/ejpfm.2019030203
dc.identifier.urihttp://rep.enu.kz/handle/enu/10662
dc.description.abstractPreliminary results of measurements of the total reaction cross sections σR for nuclei 4 He, 6 He, 8 He, 7 Li, 8 Li, 9 Li, 11 Li, 7 Be, 9 Be, 10 Be, 11 Be, 12 Be, 8 B, 10 B, 11 B and 12 B nuclei at energy range (10-50) AMeV with 28 Si target is presented. The secondary beams of light nuclei were produced by bombardment of the 15N (50 AMeV) primary beam on Be target and separated by COMBAS fragmentseparator. In dispersive focal plane a horizontal slit defined the momentum acceptance as 1% and a wedge degrader of 600 µm Al was installed. The Bρ of the second section of the fragment-separator was adjusted for measurements in energy range (10-45) AMeV. The strong absorption model reproduces the A-dependence of σR , but not the detailed structure. We are comparing our experimental data with predictions of microscopic (dashed line) and strong absorption model, Glauber multiple scattering theory and preliminary results are obtained.ru
dc.language.isoenru
dc.relation.ispartofseriesVol. 3(2);134-138
dc.subjecttotal reaction cross sectionsru
dc.subjecttransmission methodru
dc.titleTotal reaction cross sections of neutron-rich light nuclei measured by the COMBAS fragment-separatorru
dc.typeArticleru


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