Francesco Cappuzzello Università di Catania and INFN-Laboratori Nazionali del Sud, Catania. LNS Users Committee 6 December 2013

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MAGNEX@LNS Francesco Cappuzzello Università di Catania and INFN-Laboratori Nazionali del Sud, Catania LNS Users Committee 6 December 2013

Working group in Catania F. C. 1,2, C. Agodi 2, M. Bondì 1,2, D. Carbone 1,2, M. Cavallaro 2, A. Cunsolo 1,2, M. De Napoli 3, A. Foti 1,3, D. Nicolosi 1,2, S. Tropea 1,2 1. Dipartimento di Fisica e Astronomia, Università degli Studi di Catania, Italy 2. Istituto Nazionale di Fisica Nucleare Laboratori Nazionali del Sud, Italy 3. Istituto Nazionale di Fisica Nucleare Sezione Catania, Italy Collaborations on specific subjects 1. IN2P3 IPN, Orsay, France 2. IFUSP, Sao Paolo, Brazil 3. IFUFF- Niteroi, Brazil 4. TRIUMF, Vancouver, Canada 5. INFN- Sez. Padova, Pisa, Napoli 6. University of Joannina, Greece 7. University of Huelva, Spain 8. University of Osaka 9. University of Casablanca, Morocco 10. University of Notre-Dame, USA 2

MAGNEX: a multipurpose device Pairing correlations Italy, France, Brasil Nuclear rainbow Brasil, Italy α-clustering Brasil, Italy, USA Nuclear break-up Greece, Italy, Spain Giant monopole by FRIBS beams Italy Pick-up reactions Italy, France, Japan Single and double charge exchange Italy, Japan Ab initio Canada, Italy, Brasil, Morocco Quick and partial overview today 3

Pairing correlations Italy, France, Brasil Some mature activity F.Cappuzzello, et al., Phys. Lett.B 711 (2012) 347-352 13 C( 18 O, 16 O) 15 C 7 < θ lab < 17 18 O+ 13 C at 84 MeV 7 < θ lab < 13 inelastic 18 O stripping pick-up 16 O 17 O 15 O 19 O M.Cavallaro, et al., Phys.Rev.C 88 (2013) 054601 18 O+ 12 C at 84 MeV 14 15 16 17 18 19 20 A Several experiments performed (100%) Analyses almost completed (80%) Publication step (30%) Major physics output: discovery of the GPV, determination of pair spectroscopic factor 4

Nuclear rainbow Brasil, Italy Some mature activity 2 + 4 + GQR GMR M.Cavallaro et al NIMA (2011) 648 (2011) 46-51 D.Pereira et al. PLB 710 (2012) 426 J.R.B.Oliveira et al. JPG 40 (2013) 105101 Several experiments performed (70%) Analyses almost completed (70%) Publication step (40%) Major physics output: discovery of the nuclear rainbow in heavy nuclei Major technological achievement: high resolution measurement with CS 5

α-clustering Brasil, Italy, USA Started at LAFN Pelletron 12 C( 6 Li,d) 16 O done 13 C( 6 Li,d) 17 O done Some novel activity Qualifying aspect: 15 kev energy resolution thanks to the Split-Pole to be compared to values of at least 100 kev in literature 9 Be( 6 Li,d) 13 C done 11 B( 6 Li,d) 15 N, new run in september 2013 M.R.D. Rodrigues et al., PRC, accepted T. Borello-Lewin, et al., Int Journ. of Mod. Phys. E 20 (2011) 1018 Major discovery: experimental widths are much smaller than reported in lieterature! L (cm) α-clustering needs to be revised 6

α-clustering Brasil, Italy, USA At INFN-LNS Catania Qualifying aspect: Wide incident energy range (up to 80 MeV) Large acceptance (50 msr) Good energy resolution (1/1000) Coincidence detection of reaction products ( 6 Li,d) reactions as probes (α,α ) reactions as probes Approved experiments at LNS: 90 Zr( 6 Li,d) 94 Mo and 12 C( 6 Li,d) 16 O at 40 MeV February 2014 The 94 Mo(α,α ) experiment approved by LNS PAC and foreseen in 2014-2015 7

Ab initio Canada, Italy, Brasil, Morocco A new research program on fundamental nuclear forces C. Agodi, M. Bondì, F. Cappuzzello, D. Carbone, M. Cavallaro, A. Cunsolo, M. De Napoli, A. Foti, D. Nicolosi, S. Tropea INFN - Laboratori Nazionali del Sud, Catania, Italy; INFN - Sezione di Catania, Catania, Italy; Dipartimento di Fisica e Astronomia, Università di Catania, Catania, Italy; INFN G. Orlandini Dipartimento di Fisica, Universita di Trento, I-38123 Trento, Italy; INFN, Gruppo Collegato di Trento, I-38123 Trento, Italy S. Bacca TRIUMF, 4004 Wesbrook Mall, Vancouver, B.C. V6J 2A3, Canada L. Chamon, P.R.S. Gomes, R. Linares, J. Lubian, J.R.B. Oliveira Instituto de Fisica Nuclear, Universidade de Sao Paulo, Brasil Instituto de Fisica, Universidade Federal Fluminense, Niteroi, Rio de Janeiro, Brazil M. L. Bouhssa, A. Khouaja, J. Inchaouh, A. Morsad, H. Chakir, S. Ouaskit LRSA, Department of Physics, Faculty of Science Ben M'Sik, University Hassan II Mohammedia-Casablanca, Morocco

Ab initio Canada, Italy, Brasil, Morocco A new puzzle in nuclear physics 4 He 0 + resonance at 20.29 MeV S. Bacca et al., PRL 110 (2013) 042503 4 He 0 + ground state Very different form factors! Very similar form factors Best Hamiltonians largely deviate from 4 He(e,e ) 4 He* data!!

Ab initio Canada, Italy, Brasil, Morocco What we propose to do Studying the 4 He( 4 He, 4 He) 4 He* reaction at 55 MeV Main tools Superconducting Cyclotron beam Gaseous target and implanted 4 He + Ta target MAGNEX spectrometer at forward angles (θ CM = 0 30 )

Ab initio Canada, Italy, Brasil, Morocco Extracting the form factors Measuring the elastic and inelastic cross sections 4 He + 4 He elastic scattering Determining the distorted waves by Coupled Channel analysis Using the Sao Paulo double folding optical potential Extracting the form factors Expected accuracy 10-20% L.C.Chamon et al PRC 83, 034617 (2011)

Single and double charge exchange Italy, Japan Double β-decay T 0ν 1 2 (0 + 0 + ) = G 01 M ββ 0ν 2 m ν m e 2 A lot of new physics inside m ν = i U ei 2 m i e iα i but one should know Nuclear Matrix Element (NME) M ˆ 0 ββ 0ν 2 ββ 0ν ε = 0 f Oε i

β β-decay 1) 2ν double β-decay 1) Does not distinguish between Dirac and Majorana 2) Experimentally observed in several nuclei since 1987 2) 0ν double β-decay Neutrino has mass Neutrino is Majorana particle Violates the leptonic number conservation Experimentally not observed Beyond the standard model ν and anti-ν can be distinguished ν and anti-ν are the same

New physics for the next decades but requires Nuclear Matrix Element (NME)! M ˆ 0 ββ 0ν 2 ββ 0ν ε = 0 f Oε i Calculations: QRPA, Large scale shell model, IBM.. Measurements: Network cross sections including Double Charge Exchange, Single charge exchange, transfer reactions and so on.

State of the art NME calculations From A. Giuliani and A. Poves Adv. in High En. Phys. 2012 (2012) 857016 Figure 2: The neutrinoless double-beta decay; "state-of-the-art" NMEs: QRPA [30] (red bars) and [21, 22] (diamonds), ISM [31] (squares), IBM [25] (circles), and GCM [26] (triangles).

( 18 O, 18 Ne) DCE reactions in Catania 40 Ca( 18 O, 18 Ne) 40 Ar @ 270 MeV 0 < θ lab < 10 Q = -5.9 MeV 18 O and 18 Ne belong to the same multiplet in S and T Very low polarizability of core 16 O Sequential transfer processes very mismatched Target T = 0 only T = 2 states of the residual 1.E+04 1.E+02 dσ/dω (µb/sr) 1.E+00 1.E-02 1.E-04 1.E-06 1.E-08 1.E-10 direct DCE 0 2 4 6 8 10 Scattering angle (deg) sequential transfer 1 2 2 1 2 σ ( q, ω) exp q1 r exp q2 r 3 3 2

Experimental Set-up 18 O 7+ beam from Cyclotron at 270 MeV (10 pna) 40 Ca solid target of 300 μg/cm 2 Ejectiles detected by the MAGNEX spectrometer Angular setting 16 O + 42 Ca Measured Not measured 18 O + 40 Ca 18 F + 40 K 18 Ne + 40 Ar 20 Ne + 38 Ar

Particle Identification Z identification A identification Na 22 Ne 21 Ne 20 Ne 19 Ne 18 Ne F Ne X foc (m) E resid (ch) A. Cunsolo, et al., NIMA484 (2002) 56 A. Cunsolo, et al., NIMA481 (2002) 48 F. Cappuzzello et al., NIMA621 (2010) 419 F. Cappuzzello, et al. NIMA638 (2011) 74 E resid (ch)

Preliminary spectrum of 40 Ar 40 Ca( 18 O, 18 Ne) 40 Ar @ 270 MeV 0 < θ lab <4 FWHM ~ 0.5 MeV counts g.s. 1.46 + g.s. * The 40 Ar 0 + ground state is well separated from the first excited state 2 + at 1.46 MeV E* (MeV)

Preliminary 40 Ar g.s. angular distribution 40 Ca g.s. (0 + )( 18 O, 18 Ne) 40 Ar g.s. (0 + ) @ 270 MeV counts θ lab (deg)

Preliminary spectrum of 38Ar 40 Ca( 18 O, 20 Ne) 38 Ar @ 270 MeV 0 < θ lab <10 16 O( 18 O, 20 Ne) 14 C counts 12 C( 18 O, 20 Ne) 10 Be g.s. g.s. * + 2.167 E* (MeV)

Conclusions MAGNEX is attracting a growing worldwide interest for challenging physics cases Large international collaborations are progressively setting up Considerable amount of beam time are routinely requested from external users Exciting new physics is at our reach in the present and future counts θ lab (deg) 22

Preliminary neutron energy spectra Ecc = Q - Q 0 (MeV) Neutron energy (MeV) Neutron energy (MeV) 23