Spectroscopy of nuclei around $^{100}$Sn populated via two-neutron knockout reactions

We report on the in-beam gamma spectroscopy of Sn102 and Cd100 produced via two-neutron removal from carbon and CH2 targets at about 150 MeV/nucleon beam energy. New transitions assigned to the decay of a second 2+ excited state at 2470(60) keV in Sn102 were observed. Two-neutron removal cross sections from Sn104 and Cd102 have been extracted. The enhanced cross section to the 22+ in Sn102 populated via the (p,p2n) reaction is traced back to an increase of shell-model structure overlaps, consistent with the hypothesis that the proton-induced two-deeply bound-nucleon removal mechanism is of direct nature.

[1]  C. Vidal,et al.  STAT , 2019, Springer Reference Medizin.

[2]  R. Roth,et al.  Structure of the Lightest Tin Isotopes. , 2017, Physical review letters.

[3]  Kazuki Yoshida,et al.  Asymmetry of the parallel momentum distribution of ( p,pN ) reaction residues , 2015, 1505.06624.

[4]  M. Martini,et al.  Neutron-driven collectivity in light tin isotopes: Proton inelastic scattering from 104Sn , 2015 .

[5]  R. Crespo,et al.  Rescattering effects for the C12(p ,2p)B11 reaction at 400 MeV/u , 2014 .

[6]  S. Takeuchi,et al.  DALI2: A NaI(Tl) detector array for measurements of $\gamma$ rays from fast nuclei , 2014 .

[7]  J. Ryckebusch,et al.  Quasifree ( p,2p) and ( p,pn) reactions with unstable nuclei , 2013, 1311.6734.

[8]  S. Takeuchi,et al.  In-beam γ-ray spectroscopy of ^ Mg : Merging the N=20 and N=28 shell quenching , 2013 .

[9]  A. Boudard,et al.  Evaporation-cost dependence in heavy-ion fragmentation , 2013 .

[10]  B. A. Brown,et al.  Quadrupole collectivity in neutron-deficient Sn nuclei: 104 Sn and the role of proton excitations , 2013, 1310.5987.

[11]  R. Hertenberger,et al.  High resolution spectroscopy of 112 Sn through the 114 Sn(p,t) 112 Sn reaction , 2012 .

[12]  R. Broglia,et al.  Calculation of the transition from pairing vibrational to pairing rotational regimes between magic nuclei ¹⁰⁰Sn and ¹³²Sn via two-nucleon transfer reactions. , 2011, Physical review letters.

[13]  R. Hertenberger,et al.  High-resolution measurement of the {sup 118,124}Sn(p,t){sup 116,122}Sn reactions: Shell-model and microscopic distorted-wave Born approximation calculations , 2011 .

[14]  Hiroshi Suzuki,et al.  BigRIPS separator and ZeroDegree spectrometer at RIKEN RI Beam Factory , 2009 .

[15]  R. Hertenberger,et al.  Sn 118 levels studied by the Sn 120 ( p , t ) reaction: High-resolution measurements, shell model, and distorted-wave Born approximation calculations , 2008 .

[16]  B. A. Brown,et al.  Diffraction dissociation contributions to two-nucleon knockout reactions and the suppression of shell-model strength , 2006 .

[17]  G. Angelis,et al.  108Sn studied with intermediate-energy Coulomb excitation , 2005 .

[18]  B. A. Brown,et al.  Correlated two-nucleon stripping reactions , 2004 .

[19]  R. Hertenberger,et al.  High-resolution study of theSn116(p,t)reaction and shell model structure ofSn114 , 2004 .

[20]  B. A. Brown,et al.  New direct reaction: two-proton knockout from neutron-rich nuclei. , 2003, Physical Review Letters.

[21]  A. Dell'Acqua,et al.  Geant4 - A simulation toolkit , 2003 .

[22]  T. Kubo,et al.  Gamma-ray spectroscopy of 34Mg via RI beam fragmentation , 2002 .

[23]  J. C. Waddington,et al.  Yrast and near-yrast excitations up to high spin in {sub 48}{sup 100}Cd{sub 52} , 2000 .

[24]  R. Hertenberger,et al.  Level structure of Sn-120: High resolution (p,t) reaction and shell model description , 1999 .

[25]  M. Carpenter,et al.  E2 polarization charge in 102Sn , 1998 .

[26]  K. Spohr,et al.  The decay of theIπ=8+ isomer in100Cd-neutron particle and proton hole states , 1994 .

[27]  R. Broglia,et al.  Two-Neutron Transfer Reactions and the Pairing Model , 1973 .

[28]  R. Chapman,et al.  (t, p) reactions on 112, 124Sn and the pairing model , 1969 .

[29]  S. Yoshida Note on the two-nucleon stripping reaction , 1962 .