Entry Distribution, Fission Barrier, and Formation Mechanism of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>N</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow><mml:mn>102</mml:mn></mml:mrow><mml:mrow><mml:mn>254</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow><mml:mi>o</mml:mi></mml:math>
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Annotatsiya
The entry distribution in angular momentum and excitation energy for the formation of ${}^{254}\mathrm{No}$ has been measured after the ${}^{208}\mathrm{Pb}{(}^{48}\mathrm{Ca},2n)$ reaction at 215 and 219 MeV. This nucleus is populated up to spin $22\ensuremath{\Elzxh}$ and excitation energy $\ensuremath{\gtrsim}6\mathrm{MeV}$ above the yrast line, with the half-maximum points of the energy distributions at $\ensuremath{\sim}5\mathrm{MeV}$ for spins between $12\ensuremath{\Elzxh}$ and $22\ensuremath{\Elzxh}$. This suggests that the fission barrier is $\ensuremath{\gtrsim}5\mathrm{MeV}$ and that the shell-correction energy persists to high spin.
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