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Исследование кластеризации легких ядер в релятивистской фрагментации П.И. Зарубин (ОИЯИ, Дубна) N. P. Andreeva a, D. A. Artemenkov b,V. Bradnova b, M. M. Chernyavsky c, A. Sh. Gaitinov a, S. P. Kharlamov c, A. D. Kovalenko b, М. Haiduc d, S. G. Gerasimov c, L. A. Goncharova c, N. Kachalova b V. G. Larionova c, F. G. Lepekhin e, A. I. Malakhov b, A. A. Moiseenko f, G. I. Orlova c, N. G. Peresadko c, N. G. Polukhina c, P. A. Rukoyatkin b, V. V. Rusakova b, V. R. Sarkisyan f, T. V. Schedrina b, B. B. Simonov e, E. Stan e, R. Stanoeva g, I. Tsakov g, S. Vokal h, P. I. Zarubin b, and I.G Zarubina b a Insitutute of Physics and Technology, Almaty, Kazakhstan b Joint Institute for Nuclear Research, Dubna, Russia c P. N. Lebedev Physical Institute, RAS, Moscow, Russia d Institute of Space Sciences, Bucharest-Magurele, Romania e Petersburg Institute of Nuclear Physics, RAS, Gatchina, Russia f Erevan Physical Institute, Erevan, Armenia g Insttitute for Nuclear Research and Nuclear Energy, BAS, Sofia, Bulgaria h P. J. Šafárik University, Košice, Slovak Republic
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14 N Dissociation with 8 Be like fragmentation 3 after proton
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Mg-Si Dissociation into charge state 2+2+2+2+2+1 5 +proton
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Dubna: Relativistic Nuclei
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Secondary beams of light radioactive nuclei will be produced mostly via charge exchange reactions. 8 B and 9 Be beams has been formed via fragmentation of 10 B.
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Clustering building blocks: more than one nucleon bound, stable & no exited states below particle decay thresholds – deuteron, triton, 4 He, and 3 He nuclei
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A=6 =0.092 MeV
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4.5A GeV/c 6 Li
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7 Li. About 7% of all inelastic interactions of 7 Li nuclei are “white” stars (80 events). Decay of 7 Li nucleus to - particle and triton - 40 events.
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1.9 A GeV 10 B 10 B is disintegrated to 2 doubly charged and 1singly charged particles in 70% of “white” stars. A singly charged particle is the deuteron in 40% like in case of 6 Li. 8 Be contribution is 20%. 10 В 9 Bep – 3%
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ВЫХОДЫ ФРАГМЕНТОВ ЯДРА 11 В А.ВОКАЛОВА и С.Вокал, Я.Врлакова, М.Карабова Семинар посвященый 90-летию со дня рождения К.Д.Толстова “Исследование процессов фрагментации релятивистских ядер на Нуклотроне методом ядерных фотоэмульсий” Дубна, 4-5 октября 2005г.
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Q4Q4 Kanál disociácie (Z F )N 54321 7311 61110 513 51121 5113 5126 52149 51322 551 Spolu116
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Из этих 116 взаимодействий мы выделили те, у которых Nh=0 и ns=0 Nh - ч+с, ns - р Q4Q4 421N 6114 5216 5131
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Splitting to HeHe with two target fragments, HeHe, HeHH, 6 Lip, and 4H. 2 A GeV/c 7 Be.
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2 A GeV/c 10 B 8 B 2 A GeV/c 10 B 8 B
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7 Be% 8 B(+1)% 2+241431541 2+1+142451746 1+1+1+122410 3+191013 Сумма9437
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8 B→ 7 Be+p “white” stars =73 MeV/c =52 MeV/c
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ε ij =arccos((P Ti ∙ P Tj )/ (P Ti ∙ P Tj )) ≈2 8 B→ 7 Be+p “white” stars
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