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Structure of the N = 50 As, Ge, Ga nuclei (CROSBI ID 187266)

Prilog u časopisu | izvorni znanstveni rad | međunarodna recenzija

Sahin, E. ; de Angelis, G. ; Duchene, G. ; Faul, T. ; Gadea, A. ; Lisetskiy, A.F. ; Ackermann, D. ; Algora, A. ; Aydin, S. ; Azaiez, F. et al. Structure of the N = 50 As, Ge, Ga nuclei // Nuclear physics. A, 893 (2012), 1-12. doi: 10.1016/j.nuclphysa.2012.08.007

Podaci o odgovornosti

Sahin, E. ; de Angelis, G. ; Duchene, G. ; Faul, T. ; Gadea, A. ; Lisetskiy, A.F. ; Ackermann, D. ; Algora, A. ; Aydin, S. ; Azaiez, F. ; Bazzacco, D. ; Benzoni, G. ; Bostan, M. ; Byrski, T. ; Čeliković, I. ; Chapman, R. ; Corradi, L. ; Courtin, S. ; Curien, D. ; Datta Pramanik, U. ; Didierjean, F. ; Dorvaux, O. ; Erduran, M.N. ; Erturk, S. ; Farnea, E. ; Fioretto, E. ; de Frances, G. ; Franchoo, S. ; Gall, B. ; Gottardo, A. ; Guiot, B. ; Haas, F. ; Ibrahim, F. ; Ince, E. ; Khouaja A. ; Kusoglu, A. ; La Rana, G. ; Labiche, M. ; Lebhertz, D. ; Lenzi, S. ; Leoni, S. ; Lunardi, S. ; Mason, P. ; Mengoni, D. ; Michelagnoli, C. ; Modamio, V. ; Montagnoli, G. ; Montanari, D. ; Moro, R. ; Mouginot, B. ; Napoli, D.R. ; O’Donnell, D. ; Oliveira, J.R.B. ; Ollier, J. ; Orlandi, R. ; Pollarolo, G. ; Recchia, F. ; Robin, J. ; Salsac, M.-D. ; Scarlassara, F. ; Singh, R.P. ; Silvestri, R. ; Smith, J.F. ; Stefan, I. ; Stefanini, A.M. ; Subotić, K. ; Szilner, Suzana ; Tonev, D. ; Torres, D.A. ; Trotta, M. ; Ujic, P. ; Ur, C. ; Valiente-Dobón, J.J. ; Verney, D. ; Yalcinkaya, M. ; Wadyn, P.T. ; Wiedemann, K.T. ; Zuber, K. ;

engleski

Structure of the N = 50 As, Ge, Ga nuclei

The level structures of the N = 50, 83As, 82Ge, and 81Ga isotones have been investigated by means of multi-nucleon transfer reactions. A first experiment was performed with the CLARA–PRISMA setup to identify these nuclei. A second experiment was carried out with the GASP array in order to deduce the γ -ray coincidence information. The results obtained on the high-spin states of such nuclei are used to test the stability of the N = 50 shell closure in the region of 78Ni (Z = 28). The comparison of the experimental level schemes with the shell-model calculations yields an N = 50 energy gap value of 4.7(3) MeV at Z = 28. This value, in a good agreement with the prediction of the finite-range liquid-drop model as well as with the recent large-scale shell model calculations, does not support a weakening of the N = 50 shell gap down to Z = 28.

nuclear reactions; magnetic spectrometer; Compton-suppressed detectors; shell model

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Podaci o izdanju

893

2012.

1-12

objavljeno

0375-9474

10.1016/j.nuclphysa.2012.08.007

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Fizika

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