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Study of 13Be through isobaric analog resonances

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1 Study of 13Be through isobaric analog resonances
Motivation 13Be Method Feasibility Study of 13Be through isobaric analog resonances in the Maya active target Riccardo Raabe (IKS, K.U.Leuven) IKS, K.U.Leuven IEM-CSIC, Madrid Univ. Santiago de Compostela GANIL, Caen Univ. Birmingham Univ. Aarhus LPC-ENSICAEN, Caen Chalmers University, Göteborg NSCL-MSU, East Lansing CEA Saclay IPN Orsay R. Raabe, T. Roger, S. Sambi M.J.G. Borge, E. Nácher, O. Tengblad M. Caamaño, D. Cortina-Gil, B. Fernandez-Dominguez F. De Oliveira Santos, G.F. Grinyer, H. Savajols M. Freer H.O.U. Fynbo, J.S. Johansen, K. Riisager J. Gibelin, M. Marques, N. Orr A. Heinz, B. Jonson, T. Nilsson, G. Nyman W. Mittig, H. Wang E. Pollacco, P. Roussel-Chomaz M. Vandebrouck

2 Shell ordering around N = 8
Motivation 13Be Method Feasibility Shell ordering around N = 8 O. Sorlin, M.-G. Porquet Prog. Part. Nuc. Phys. 61 (2008) 602 Protons removed from p shells  reduction of N = 8 s shell available  halo nuclei 11Be, 11Li, 14Be 13Be: one neutron above N = 8 essential to model the 2-n halo nucleus 14Be p1/2 p3/2 s1/2 π ν 8 d5/2

3 13Be studies (exp) G. Blanchon at al. (2010) Inversion p1/2 – s1/2 ?
Motivation 13Be Method Feasibility 13Be studies (exp) Korsheninnikov 1995 6 Belozyorov 1998 Simon 2007 Ostrowski 1992 Christian 2008 Kondo 2010 Lecouey 2004 4 Thoennessen 2000 1/2− E(12Be-n) (MeV) 5/2+ (5/2+) 5/2+ 5/2+ 5/2+ 2 (5/2+) 1/2+ 1/2− (1/2) s (s, 1/2+) 1/2+ s G. Blanchon at al. (2010) Inversion p1/2 – s1/2 ? Necessary to reproduce 14Be (?)

4 Method: resonant scattering in a thick target
Motivation 13Be Method Feasibility Method: resonant scattering in a thick target AZ beam, Ecm scan in the target Population of resonant states in the A+1Z+1 compound nucleus isobaric analogues (IAS) of the states of interest in A+1Z All states populated Elastic: large cross section Spin-parity assignment 12Be + p → 13B IAS of states in 13Be p ΔE-E Ec.m.

5 Measurement with the Maya active target
Motivation 13Be Method Feasibility Measurement with the Maya active target Usually: p at small angles limited statistics In Maya: Elastic scattering Detection of proton Range of beam-like particle  identification inelastic channels  larger statistics  resolution <10 keV Detection of n-emission channel via identification of 12B p ΔE-E Ec.m. T. Roger, L. Gaudefroy, W. Mittig, H. Wang, et al. T. Roger, L. Gaudefroy, W. Mittig, H. Wang, et al.

6 Motivation 13Be Method Feasibility Feasibility 12Be at 3 MeV/nucleon, min 20 pps (limit on instantaneous rate) Maya filled with C4H10 at ≈100 mbar 50-keV bin (1019 protons/cm2) 0.5 cts/h Production (target...) 12C contamination 12Be(p,n)12B(T=2) 100 cts/bin ≈12 days + detector tuning → 40 shifts

7 Motivation 13Be Method Feasibility Feasibility Production target : ideally fast release – but less reliable REXTRAP: normal mode EBIS: Slow extraction preferred (compatibly with transmission) 12C contamination double stripper

8 Pictures

9 Cross sections 12Be(p,n)12B(T=2) 12Be(p,p)12Be

10 Example G. V. Rogachev et al., Phys. Rev. C 67 (2003)

11 11Be+p


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