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August 31 – September 4, 2015, Groningen, Netherlands

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Presentation on theme: "August 31 – September 4, 2015, Groningen, Netherlands"— Presentation transcript:

1 August 31 – September 4, 2015, Groningen, Netherlands
Clustering features of light neutron-deficient nuclei in nuclear fragmentation Denis Artemenkov, (VBLHEP, JINR) EuNPC2015 August 31 – September 4, 2015, Groningen, Netherlands 1

2 BECQUEREL at the JINR Nuclotron is devoted systematic exploration of clustering features of light stable and radioactive nuclei. The fragmentation of a large variety of light nuclei was investigated using the emulsions exposed to few A GeV nuclear beams at JINR Nuclotron. A nuclear track emulsion is used to explore the fragmentation of the relativistic nuclei. 2

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4 Role of the Nuclear and Electromagnetic Interactions in the Coherent Dissociation of the Relativistic 7Li Nucleus into the 3H + 4He Channel N. G. Peresadko, V. N. Fetisov, Yu. A. Aleksandrov, S. G. Gerasimov, V. A. Dronov, V. G. Larionova, E. I. Tamm, S. P. Kharlamov

5 12C3 , A GeV (PAVICOM image) 5

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7 12C(n,n’)3α, En = 14.1 MeV 3α (~3-5 ) μm http://neutrontech.ru
DVIN - explosives detector on the basis of fast tagged neutron method for complex program for population safety in transport 3α (~3-5 ) μm 8Be, 0+ 8Be, 2+ -?

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9 Opening angle distribution of two α-particles
9Be2 Θ 9Be Θ, mrad <Θ>, mrad σΘ, mrad Fraction (Events) Θn ( ) 4.4 ± 0.2 2.1 ± 0.2 0.56 ± 0.04 (164) Θw (15.0 – 45.0) 27.0 ± 0.6 5.9 ± 0.6 0.44 ± 0.04 (130) Fractions of events Θn and Θw demonstrate compliance with weights 0+ and 2+ states of a 8Be core, adopted in the two-body model, ω0+ = and ω2+ = [1,2]. They indicate the presence of these states as components of the ground state of the 9Be nucleus. 1. Y. L. Parfenova and Ch. Leclercq-Willain, «Hyperfine anomaly in Be isotopes and neutron spatial distribution: A three-cluster model for 9Be», Phys. Rev. C 72, (2005). 2. Y. L. Parfenova and Ch. Leclercq-Willain, «Hyperfine anomaly in Be isotopes in the cluster model and the neutron spatial distribution», Phys. Rev. C 72, (2005) ).

10 10C→2α+2p (1.2 A GeV) 10C

11 10С → 9В+р → 8Ве+2р (25-30%)

12 9C

13 The exposure of NTE pellicles by relativistic 11C 1
The exposure of NTE pellicles by relativistic 11C 1.2 A GeV nuclei was held at the JINR Nuclotron Dec The observed channels of fragmentation 11C nuclei Channels “White” stars With emulsion nuclei fragments 6H 3 (2%) 10 (4%) B + H 6 (3%) 7 (3%) He + 4H 15 (9%) 44 (17%) Li + He + H 5 (3%) 17 (7%) Be + He 18 (10%) 26 (10%) 2He + 2H 72 (41%) 140 (53%) 3He 25 (14%) 19 (7%)

14 8Be 9B (a) (b) The distribution of events of the channel 11C 2α + 2p by excitation energy: Q2α pairs α-particles in the inset - enlarged distribution Q2α (a); Q2α + p triples 2α + p, in the inset - enlarged distribution Q2α + p (b).

15 Thank you for your attention!
Summary The presented observations serve as an illustration of prospects of the Nuclotron and NTE for nuclear physics researches. Due to a record space resolution the emulsion technique provides unique entirety in studying of light nuclei, especially, neutron-deficient ones. Providing the 3D observation of narrow dissociation vertices this classical technique gives novel possibilities of moving toward more and more complicated nuclear systems. The results of an exclusive study of the interactions of relativistic 9Be, 10,12C nuclei lead to the conclusion that the known features of their structure are clearly manifested in very peripheral dissociations. Thank you for your attention!


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