1. Why the complete fusion of weakly bound nuclei is enhanced at sub- barrier energies and suppressed above the barrier. Paulo R. S. Gomes Univ. Fed. Fluminense (UFF), Niteroi, Brazil NN2012- San Antonio, May 27th-June 1st (2012)

2. Reactions with weakly bound nuclei

3. However, nature is more complicated than that simple picture: Breakup following transfer RESULTS measured calculated by p conservation known before after n p Courtesy of Luong

4. See talk by Nanda Dasgupta next Friday

5. Frequently used procedures to answer “Enhancement or suppression in relation to what? a)Comparison of data with theoretical predictions. b) Comparison of data for weakly and tightly bound systems.

6. Effects to be considered Static effects: longer tail of the optical potential arising from the weakly bound nucleons. Dynamical effects: strong coupling between the elastic channel and the continuum states representing the break-up channel.

8. Example: 6 He + 209 Bi Single channel - no halo Single channel – with halo CC with bound channels (schematic calculation) Shortcomings of the procedure: Choice of interaction plays fundamental role Does not allow comparisons of different systems Difficult to include continuum – no separate CF and ICF

9. Conclusions about static effects of halo nuclei. Fusion enhancement when compared with what it should be without halo properties. There is no more discussion left about that.

10. Differences due to static effects :

11. Fusion functions F(x) (our reduction method) Inspired in Wong’s approximation F 0 (x) = Universal Fusion Function (UFF) system independent !

12. Direct use of the reduction method Refining the method Eliminate the failure of the Wong model for light systems at sub-barrier energies

13. Applications with weakly bound systems 1. Canto, Gomes, Lubian, Chamon, Crema, J.Phys. G36 (2009) 015109; NPA 821(2009)51 2.Gomes,, Lubian, Canto, PRC 79 (2009) 027606 2.Gomes, Canto, Lubian, Hussein, PLB 695 (2011), 320

14. Use of UFF for investigating the role of BU dynamical effects on the total fusion of heavy weakly bound systems No effect above the barrier- large enhancement below the barrier

15. Use of UFF for investigating the role of BU dynamical effects on the total fusion of very light weakly bound systems No effect above the barrier- almost no data below the barrier

16. Use of UFF for investigating the role of BU dynamical effects on the total fusion of light weakly bound systems No effect above the barrier- no data below the barrier

17. Use of UFF for investigating the role of BU dynamical effects on the complete fusion of stable weakly bound heavy systems We did not include any resonance of the projectiles in CCC. Suppression above the barrier- enhancement below the barrier

18. Fusion of neutron halo 6,8 He, 11 Be weakly bound systems

19. Conclusion from the systematic (several systems) : CF enhancement at sub-barrier energies and suppression above the barrier, when compared with what it should be without any dynamical effect due to breakup and transfer channels. Question: Why?

20. Example for Complete fusion of 6,7 Li + 209 Bi Effects of suppression and enhancement are more important for 6 Li than for 7 Li. ( 6 Li has smaller BU threshold energy and no bound state)

21. Approaches which might be used -Coupled channel calculations (CDCC calculations including transfer channels and sequential breakup) – not available so far -Dynamic polarization potential (substitutes many channels by one single channel – energy dependent optical potential.

22. Suppression of fusion above the barrier

23. Threshold anomaly in the elastic scattering of tightly bound systems Optical Potencial : U(E) = V 0 + ∆V(E) + W(E) where W(E) = W V (E) + W S (E) Tenreiro et al – PRC 53 (1996), 2870

24. The Threshold Anomaly for “normal systems “ As the energy decreases towards the barrier, reaction channels close and the imaginary potential decreases and vanishes. Due to the dispersion relation, the real potential increases when the imaginary potential decreases. The attraction increases (attractive polarization potential) and consequently there is sub-barrier fusion enhancement. Polarization potentials associated with couplings to transfer and inelastic channels were shown to be attractive

25. A new type of threshold anomaly: break-up thereshold anomaly (BTA) The large NCBUat low energies produces a repulsive polarization potential and suppress fusion. Gomes et al – J Phys G 31 (2005), S1669

26. The behavior for weakly bound systems The breakup is important even below the barrier. So, the imaginary potential does not decrease at the barrier energy. Indeed, it can increase. Consequently, the real potential decreases at this energy region. Fusion is suppressed. This behavior is called ‘breakup threshold anomaly’ (BTA). Of course, the imaginary potential must decrease and vanish at lower energies (we will discuss this point later).

27. BTA M.S. Hussein, P.R.S. Gomes, J. Lubian, L.C. Chamon – PRC 73 (2006) 044610

28. Systems with 6 Li Figueira et al. – PRC 75 (2007), 017602 A. Gomez-Camacho et al., NPA 833 (2010), 156 Figueira et al. – PRC 81 (2010), 024603 Hussein et al., PRC 73 (2006) 044610 Keeley et al., NPA571 (1994) 326 Gomes et al JPG 31 (2005) S1669 6Li + 144Sm Deshmukh et al. PRC 83, 024607 (2011) 6Li + 116Sn

29. More Systems with 6 Li Souza – PRC75, 044601 (2007) Zadro, di Pietro- PRC 80, 064610 (2009) 6Li + 64Zn Kunawat – PRC 78, 044617 (2008) 6Li + 90Zr Biswas- NPA 802, 67 (2008) Santra – PRC83, 034616 (2011) 6Li + 209Bi

30. Systems with 7 Li Souza – PRC75, 044601 (2007) Pakou PRC 69, 054602 (2004) Lubian- PRC 64, 027601 (2001) Gomes JPG 31 (2005) S1669 Figueira – PRC 73, 054603 (2006) 7Li + 27Al Deshmukh et al, accepted EPJA 7Li + 116Sn

31. Systems with 9 Be Signorini –PRC 61, 061603R (2000) Woolliscroft – PRC 69, 044612 (2003) 9be + 208Pb Gomes JPG 31 (2005) S1669 Gomes- PRC70, 054605 (2004) Gomes – NPA 828, 233 (2009) 9Be + 144Sm

32. Systems with radioactive nuclei A. Gomez-Camacho et al., NPA 833 (2010), 156 Garcia, Lubian – PRC 76, 067603 (2007) 6He + 209Bi

33. Calculations of DPP considering direct breakup : repulsive DPP 8 B + 58 Ni – Lubian 6 Li + 209 Bi - Santra 7 LI + 27 Al - Lubian

34. QE barrier distributions BU enhances the Coulomb barrier J. Lubian, T. Correa, P.R.S. Gomes, L. F. Canto – PRC 78 (2008) 064615

35. Conclusions The effect of the coupling to BU was shown to come from the repulsive DPP they provoke. It hinders the CF cross sections. The BU channel increases the barrier as shown in the QE barrier distributions. This leads to the hindrance of the fusion cross section

36. What about the enhancement of CF at sub-barrier energies? We have to look at the low energies for the elastic scattering: The DPP becomes attractive at low energies (below the barrier) Why?

37. At sub-barrier energies, the breakup following transfer predominates over the direct breakup. Each one of them has different DPP: direct BU produces repulsive DPP. BU after transfer produces attractive DPP. The total DPP is attractive Direct BU Sequential BU 7 Li + 144 Sm Otomar 2012

38. Conclusions Direct breakup produces repulsive polarization potential which suppress fusion at energies above the barrier. At sub-barrier energies, the breakup following transfer predominates and produces attractive polarization potential which enhances fusion. More quantitative calculations are required (CDCC calculations including transfer and BU following transfer)

39. Collaborators J. Lubian. R. Linares (UFF), L. F. Canto (UFRJ), M.S. Hussein (USP), M. Dasgupta, D. J. Hinde, D.H. Luong (ANU)