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Single-Neutron States in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi>Sn</mml:mi><mml:mprescripts/><mml:none/><mml:mn>101</mml:mn></mml:mmultiscripts></mml:math>

D. SeweryniakArgonne National Laboratory, Argonne, Illinois 60439, USAM. P. CarpenterArgonne National Laboratory, Argonne, Illinois, 60439, USAS. GrosArgonne National Laboratory, Argonne, Illinois, 60439, USAA. A. HechtUniversity of Maryland, College Park, Maryland, 20742, USAN. HotelingUniversity of Maryland, College Park, Maryland, 20742, USAR. V. F. JanssensArgonne National Laboratory, Argonne, Illinois, 60439, USAT. L. KhooArgonne National Laboratory, Argonne, Illinois, 60439, USAT. LauritsenArgonne National Laboratory, Argonne, Illinois, 60439, USAC. J. ListerArgonne National Laboratory, Argonne, Illinois, 60439, USAG. LotayUniversity of Edinburgh, Edinburgh, EH9 3JZ United KingdomD. PetersonArgonne National Laboratory, Argonne, Illinois, 60439, USAA. RobinsonArgonne National Laboratory, Argonne, Illinois, 60439, USAW. B. WaltersUniversity of Maryland, College Park, Maryland, 20742, USAX. WangUniversity of Notre Dame, Notre Dame, Indiana 46556, USAP. J. WoodsUniversity of Edinburgh, Edinburgh, EH9 3JZ United KingdomSuiyi ZhuArgonne National Laboratory, Argonne, Illinois, 60439, USA
2007lv
ABI

Annotatsiya

The first data on the relative single-particle energies outside the doubly magic $^{100}\mathrm{Sn}$ nucleus were obtained. A prompt $171.7(6)\text{ }\text{ }\mathrm{keV}$ $\ensuremath{\gamma}$-ray transition was correlated with protons emitted following the $\ensuremath{\beta}$ decay of $^{101}\mathrm{Sn}$ and is interpreted as the transition between the single-neutron ${g}_{7/2}$ and ${d}_{5/2}$ orbitals in $^{101}\mathrm{Sn}$. This observation provides a stringent test of current nuclear structure models. The measured $\ensuremath{\nu}{g}_{7/2}\mathrm{\text{\ensuremath{-}}}\ensuremath{\nu}{d}_{5/2}$ energy splitting is compared with values calculated using mean-field nuclear potentials and is used to calculate low-energy excited states in light Sn isotopes in the framework of the shell model. The correlation technique used in this work offers possibilities for future, more extensive spectroscopy near $^{100}\mathrm{Sn}$.

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