Neven Soić, Ruđer Bošković Institute, Zagreb, Croatia

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Presentation transcript:

Neven Soić, Ruđer Bošković Institute, Zagreb, Croatia Insight into the 24Mg excited states located in Gamow window for carbon - carbon burning 12C 24Mg γ Neven Soić, Ruđer Bošković Institute, Zagreb, Croatia

Collaborators 1) V. Tokić, S. Blagus, D. Jelavić Malenica, Đ. Miljanić, L. Prepolec, M. Uroić Ruđer Bošković Institute, Zagreb, Croatia 2) M. Milin Faculty of Science, University of Zagreb, Zagreb, Croatia 3) A. Di Pietro, P. Figuera, M. Fisichella, M. Lattuada, V. Scuderi, D. Torresi LNS-INFN/University of Catania, Catania, Italy 4) S. Bailey, N. Curtis, M. Freer, T. Wheldon, J. Walshe, C. Wheldon, V. Ziman University of Birmingham, Birmingham, United Kingdom 5) L. Acosta, I. Martel, A. Sanchez-Benitez University of Huelva, Huelva, Spain

Motivation Objective: search for 12C+12C resonances at the 24Mg excitations 15-20 MeV and their full characterization: excitation energy, width, spin, parity, partial decay widths Two-fold reason: nuclear structure & astrophysical motivation Work in progress, data analysis is not finished yet Gamow window Important new result is even observation of the 0+ state at these excitations with prominent cluster structure – large probability for decay into α+20Ne 20 MeV Ethr(n+23Ne) = 16.532 MeV Ethr(α+α+16O) = 14.044 MeV Ethr(12C+12C) = 13.931 MeV Ethr(1H+23Na) = 11.692 MeV Ethr(α+20Ne) = 9.313 MeV 24Mg

Elastic scattering data Resonant phenomena in heavy ion reaction D. A. Bromley, J. A. Kuehner, E. Almquist, Phys. Rev Lett 4 (1960) 385 Elastic scattering data Resonant phenomena in heavy ion reaction

Formation of quasi-molecular states in 24Mg E. Almquist, D. A. Bromley, J. A. Kuehner, Phys Rev Lett 4 (1960) 515 Reaction data Formation of quasi-molecular states in 24Mg 55 years later: - number of resonances decaying into various channels - kind of unique nuclear system, very complex structure - governed by cluster structure of 12C – oblate deformation in gs - not fully understood yet

Ikeda Diagram

B. R. Fulton et al, Phys Lett B 267 (1991) 325 M. Freer et al, Phys Rev C 57 (1998) 1277 C. Metelko et al, Phys Rev C 68 (2003) 054321

T. Kawabata et al, J. Phys. Conf. Ser. 436, 012009 (2013) The 13.1, 13.4 and 15.8 MeV states have prominent α-cluster structure

Y. Chiba and M. Kimura, PRC 91, 061302(R) (2015) antisymmetrized molecular dynamics combined with the generator coordinate method The 24Mg ground state has significant cluster components 4He+20Ne and 12C+12C The 12C+12C configuration contributes to the O2+, O3+, O5+, and is the main component of the O8+ state at 15.3 MeV

Explosive phenomena in binary systems SNIa: initiates thermonuclear runaway on white dwarf temperature 0.5 - 1.2x109 K → Ecm=1.5-3.3 MeV Super-bursts: trigger of 12C ignition up to 2.5x109 K - 5.7 MeV Massive stars:12C+12C fusion is differentiating between the evolutionary paths leading to either white dwarf or heavy elements burning stages Super-AGB stars

Existing data show large discrepancies Low energy resonance ? Relevant reactions: 12C + 12C → 24Mg +  12C + 12C → 20Ne + α 12C + 12C → 23Na + p 12C + 12C → 23Mg + n E. F. Aguilera et al, Phys. Rev. C 73 (2006) 064601 T. Spillane et al, Phys. Rev. Lett. 98 (2007) 122501 Existing data show large discrepancies Low energy resonance ?

Experiment at INFN – LNS Coincident detection of 2 (or more) reaction products 12C + 16O → 4He + 12C + 12C Q=-7.16 MeV Ethr(24Mg)=13.93 MeV → 4He + 16O + 8Be Q=-7.37 MeV Ethr(24Mg)= 14.14 MeV → 4He + 20Ne + 4He Q=-2.54 MeV Ethr(24Mg)= 9.31 MeV → 4He + 23Na + 1H Q=-4.92 MeV Ethr(24Mg)= 11.69 MeV the 16O beam from the tandem accelerator beam energy 94 MeV target 12C, thickness of 45 μg/cm2 11 days of beam-time

Detector telescopes: 50 x 50 mm2 20 μm SSSD + 1000/500 μm PSD & DSSD Particle identification from p to 12C

Single events 24Mg spectra No. Ex(MeV) FWHM(MeV) 8. 13.1 0.4 13.9 0.5 15.2 0.5 16.5 0.6 17.4 0.7 18.3 0.5 19.1 0.6 20.2 0.9 T2,T5 One strip data

One strip data Telescope 6 No. Ex(MeV) FWHM(MeV) 13.1 0.4 14.0 0.5 13.1 0.4 14.0 0.5 15.1 0.5 16.5 0.8 17.5 0.8 T1,T6 One strip data

α+20Ne decay (α-α coincident events) Catania plot: E3-Q=P32/(2A) T2-T4 T3-T6 1.6 2+ 4.2 4+ 4.2 4+ 6.9 gs 0+ 1.6 2+ 5.6 3-,1- gs 0+

Relative energy plots for the 20Ne ground state decay T2-T4

12C+12C decay 12C+12C coincident events 12C detected in T3 & T4 only

Relative energy plots for the 12C ground state decay Ex(24Mg): 19.9, 20.9, 21.3, 21.7, 22.7, 23.8, 24.2, 25.6 (25.0+25.9 ?), 27.0, 27.6 (27.0+28.0 ?), 28.0, 28.8 (28.4+29.2 ?), 29.2, 30.4 MeV

Relative energy plots for the 12C+12C*(4.4 MeV) decay Ex(24Mg): 24.2, 25.0, 25.9, 26.4, 27.6, 28.8 (28.4+29.2), 30.0, 30.8, 31.2, 31.9, 32.5, 33.2, 33.8 MeV

Relative energy plots for the 12C*(4.4 MeV)+12C*(4.4 MeV) decay Ex(24Mg): 30.4, 33.2, 34.1, 35.7 MeV

Ex(24Mg): 19.9, 20.9, 21.3, 21.7, 22.7, 23.8, 24.2, 25.0, 25.6, 25.9, 26.4, 27.0, 27.6, 28.0, 28.8, 29.2, 30.4, 30.8, 31.2, 31.9, 32.5, 33.2, 33.8, 34.1, 35.7 MeV

Relative energy plots for the 12C+12C*(7.6, 9.6 MeV) decay Ex(24Mg): 28.4, 31.9, 33.2, 34.6 MeV – 7.6 MeV Ex(24Mg): 31.9, 32.5, 33.2, 34.6, 37.0 MeV – 9.6 MeV

12C+12C decay 12C+α coincident events

Relative energy plots for the 12C ground state decay

id=34 Ex(24Mg): 19.9, 20.9, 21.3, 21.7, 22.7, 23.1, 23.8, 24.2, 25.0, 25.6, 25.9, 26.4, 27.0, 27.6, 28.0, 28.8, 30.0, 30.8, 31.2, 31.7, 31.9 MeV

Observed only already known resonances at 18.9, 19.6 and 19.9 MeV Right Q-value, higher Q, lower Q Observed only already known resonances at 18.9, 19.6 and 19.9 MeV

16O+8Be decay 16O+8Be coincident events Ex(24Mg): 21.7, 23.1, 24.2, 24.8, 25.7, 26.7 MeV

20Ne+α resonant scattering experiment Beam energy Thick gas target measurements: detector telescope at 0 deg R-matrix calculations: spin and parity of the resonances

Summary a number of states at the 24Mg excitations above 20 MeV have been observed – some are new, some new decay modes observed 12C+12C decay of known states at 18.9, 19.6 and 19.9 MeV observed – they all also observed to decay into the 20Ne+α channel limitations of the experimental setup/DAQ system – large rate of accidental coincidence events due to large elastic scatering rate – limited sensitivity obstructs observation of the 12C+12C decay of the states below 18.9 MeV another approach: the 20Ne+α resonant scattering + R-matrix fit – search for 0+ state(s) below 18.9 MeV Thank you !

H2020 ERA Chair project at RBI Expanding Potential in Particle and Radiation Detectors, Sensors and Electronics in Croatia nuclear physics, high energy physics, applications fundind 2.5 M€, 5 years project We look for the expert on detectors and electronics for the ERA Chair position and four experienced postdocs. Contact & info: soic@irb.hr