ISODEC – NEWCHIM Collaboration

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Presentation transcript:

ISODEC – NEWCHIM Collaboration Competizione tra i modi di decadimento ed influenza dell’isospin nei sistemi prodotti nelle collisioni 78,86Kr+40,48Ca a 10AMeV B. Gnoffo INFN – Catania ISODEC – NEWCHIM Collaboration

The Experimental Method Experimental Results • IMF behavior OUTLINE The Physics Case The Experimental Method Experimental Results • IMF behavior • Global features Conclusions and Outlook B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

The Physics Case Neutron richness of a compound nucleus is expected to play a crucial role in the competition between various de-excitation channels -> Information about level density, fission barrier, viscosity The Level density parameter is related to the effective mass of nucleons in the nuclear medium that is sensitive to the n/p of nuclei The fission barriers depend clearly on the symmetry energy that is weakly constrained by existing data The viscosity reflects a coupling between collective modes and intrinsic DoF -> related to the Fermi energy level and to ratio n/p Novel information can be obtained by the study of the fission cross section across long isotopic chains of compound nuclei, extending from the neutron-rich to neutron-poor side B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

The Experimental Method 78,86Kr + 40,48Ca -> 118,134Ba E/A=10 MeV/A E* ≈ 250 MeV CHIMERA at INFN-LNS S. Pirrone et al., EPJ 17 (2011) 16010 G. Politi et al., EPJ 21 (2012) 02003 S. Pirrone et al., AIP Conf. Proc. 1524 (2013) 7 G. Politi et al., JPS Conf. Proc. Vol. 6 (2015) 030082 S. Pirrone et al., Journal of Physics: Conf. Series 515 (2014) 012018 M. La Commara et al., EPJ 11 (2012); 78,82Kr + 40Ca -> 118,122Ba E/A=5.5 MeV/A E* ≈ 100 MeV INDRA at GANIL G. Ademard et al. PRC 83 (2011) 054619 Composite systems with higher E and T -> effects on decay Larger domain of N/Z (max with stable beam) B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Experimental Results Analisys of IMF characteristics Relative abundance of isotopes with 2 < Z < 9 is very different for the two systems B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Charge Yields for IMF in the range θlab = 10°- 16° Experimental Results - IMF characteristics Charge Yields for IMF in the range θlab = 10°- 16° The IMF yields exhibits an odd-even staggering, more pronounced for the n-poor system I. Lombardo et al., PRC 84 (2011) 024613 G. Casini et al., PRC 86 (2012) 011602 B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Preliminary comparison with Di Nuclear System (DNS) code Experimental Results - IMF characteristics Preliminary comparison with Di Nuclear System (DNS) code S.A. Kalandarov et al., PRC 82 (2010) 044603 Simulation performed for the TOTAL cross section normalized at Z=5 DNS seems to reproduce slightly better the n-poor system Yield (a.u.) charge Z B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Preliminary comparison with Gemini ++ code Experimental Results - IMF characteristics Preliminary comparison with Gemini ++ code Simulation performed for the TOTAL cross section normalized at Z=14 Gemini++ seems to reproduce slightly better the n-poor system B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Energy and velocity spectra in CM frame slightly change with Experimental Results - IMF characteristics Average velocity for Z= 3-17 in the center of mass frame for different Z and at different θlab Energy and velocity spectra in CM frame slightly change with detection angle -> high degree of relaxation of kinetic energy B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Signature of a binary process dominated by the Coulomb interaction Experimental Results - IMF characteristics Average velocity for Z= 3-17 in the center of mass frame for different Z compared with Viola – Hinde systematics NPA472 (1987) 318 Signature of a binary process dominated by the Coulomb interaction Experimental average values Viola values B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

1/sinθ behaviour -> high degree of relaxation, long lived system Experimental Results - FF characteristics Angular distributions in the center of mass frame for fission fragments 1/sinθ behaviour -> high degree of relaxation, long lived system Similar results for the n-rich system 78Kr + 40Ca Z=12 Z=15 Z=18 Z=31-32 Z=29-30 Z=27-28 dσ/dΩ (a.u.) B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Angular distributions in the lab frame for groups of Z Experimental Results - ER characteristics Angular distributions in the lab frame for groups of Z Very strongly forward peaked as expected for evaporation residues Z=45-46 Z=43-44 Z=41-42 78Kr + 40Ca dσ/dΩ (a.u.) B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Mtot - Ptot plot for complete events selection: Experimental Results - Global Features Mtot - Ptot plot for complete events selection: Multiplicity ≥ 2 0.8 MCN ≤ Mtot ≤ 1.1 MCN 0.6 ≤ptot/pbeam ≤1 78Kr + 40Ca Ptot/Pbeam Mtot B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Mass - Vpar for reaction products with complete events selection Experimental Results - Global Features Mass - Vpar for reaction products with complete events selection -> Important information on the interplay between mechanism -> Very preliminary analysis seems to show an higher ER/FF ratio for n-poor system compared to the n-rich one ER FF-QF VCN VP B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Experimental Results - Comparison with lower energy Preliminary comparison in the reaction 78Kr +40Ca at two different energies ER FF QF 78Kr +40Ca M1 5.5 AMeV 10 AMeV Present work M2 B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Experimental Results - Comparison with lower energy Very Preliminary comparison of IMF production cross section in the reaction 78Kr +40Ca at two different energies 78Kr + 40Ca 5.5 AMeV 78Kr + 40Ca 10 AMeV Present work G. Ademard et al., PRC 83 (2011) 054619 B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Conclusion and Outlook Results of the reactions 78,86Kr + 40,48Ca at 10 AMeV The kinematical characteristics and the angular distributions seem to indicate for both reactions a high degree of relaxation of the system The results put in evidence the influence of the neutron enrichment of the entrance channel on: Different isotopic composition and relative richness of products Odd - even effect in IMF charge distributions -> stronger for n-poor Sizeable differences for the different reaction channels: FF, QF and ER -> there is a higher ER/FF ratio for n-poor system compared to the n-rich one B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

Data analysis is in progress: Conclusion and Outlook Data analysis is in progress: Cross sections calculations for different mechanisms to confirm this first qualitative observation Study of the Coincidence between LCP-FF, LCP-ER ,LCP-IMF More precise comparisons with theoretical predictions to provide indications on the isospin influence on the reaction mechanism LOI presented in May 2014 at the “Second SPES International Workshop at INFN-LNL“ 92Kr + 40,48Ca 10 AMev 132,140Ba* E* ~ 320 MeV CN with N/Z =1.5 greater then with stable beams. -> study of the evolution, with isospin asymmetry, of the dynamics -> interplay between nuclear structure and reaction mechanism in the emission process B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015

NEWCHIM – ISODEC collaboration S.Pirrone1, G.Politi1,2, M.LaCommara3,4, J.P.Wieleczko5, B.Gnoffo1, E.DeFilippo1, P.Russotto2,6, M.Trimarchi7,8, M.Vigilante3,4, G.Ademard5, F.Amorini6, L.Auditore7,8, C.Beck9, I.Berceanu10, E.Bonnet5, B.Borderie11, G.Cardella1, A.Chbihi5, M.Colonna6, A.D’Onofrio4,12, J.D.Frankland5, E.Geraci2,1, E.Henry13, E.LaGuidara1,14, G.Lanzalone15,6, P.Lautesse16, D.Lebhertz5, N.LeNeindre 17, I.Lombardo4, D.Loria7,8, K.Mazurek5, S.Norella7,8, A.Pagano1, E.V.Pagano2,6, M.Papa1, E.Piasecki18, F.Porto2,6, L.Quattrocchi7,8, M.Quinlann13, F.Rizzo2,6, E.Rosato3,4, W.U.Schroeder13, G.Spadaccini3,4, A.Trifirò7,8, J.Toke13, G.Verde1 1) INFN - Catania, Italy 2) Dipartimento di Fisica e Astronomia, Università di Catania, Italy 3) Dipartimento di Scienze Fisiche, Università Federico II Napoli, Italy 4) INFN - Napoli, Italy 5) GANIL - Caen, France 6) INFN LNS - Catania, Italy 7) Dipartimento di Fisica, Università di Messina, Italy 8) INFN Gruppo Collegato di Messina, Italy 9) IN2P3 - IPHC Strasbourg, France 10) IPNE, Bucharest, Romania 11) IN2P3 - IPN Orsay, France 12) Dipartimento di Scienze Ambientali - Seconda Università di Napoli, Caserta, Italy 13) University of Rochester, USA 14) Centro Siciliano Fisica Nucleare e Struttura della Materia, Catania, Italy 15) Università Kore, Enna, Italy 16) IN2P3 - IPN Lyon, France 17) IN2P3 - LPC Caen, France 18) University of Warsaw, Poland B. Gnoffo 101° Congresso SIF Roma 21-25 Set 2015