Incomplete-Fusion Reactions in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">N</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>14</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>+<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Tb</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>159</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>System and a "Sum-Rule Model" for Fusion and Incomplete-Fusion Reactions
J. WilczyńskíK. Siwek-WilczyńskaInstitute of Nuclear Physics, 31-342 Cracow, Poland, and Kernfysisch Versneller Instituut, 9747-AA Groningen, The NetherlandsJ. van DrielInstitute of Nuclear Physics, 31-342 Cracow, Poland, and Kernfysisch Versneller Instituut, 9747-AA Groningen, The NetherlandsS. GonggrijpInstitute of Nuclear Physics, 31-342 Cracow, Poland, and Kernfysisch Versneller Instituut, 9747-AA Groningen, The NetherlandsD.C.J.M. HagemanInstitute of Nuclear Physics, 31-342 Cracow, Poland, and Kernfysisch Versneller Instituut, 9747-AA Groningen, The NetherlandsR. V. F. JanssensInstitute of Nuclear Physics, 31-342 Cracow, Poland, and Kernfysisch Versneller Instituut, 9747-AA Groningen, The NetherlandsJ. ŁukasiakInstitute of Nuclear Physics, 31-342 Cracow, Poland, and Kernfysisch Versneller Instituut, 9747-AA Groningen, The NetherlandsR.H. SiemssenInstitute of Nuclear Physics, 31-342 Cracow, Poland, and Kernfysisch Versneller Instituut, 9747-AA Groningen, The Netherlands
1980lv
ABI
Аннотация
Absolute cross sections for a number of binary processes in the $^{14}\mathrm{N}$+$^{159}\mathrm{Tb}$ reaction have been determined by use of $\ensuremath{\gamma}$-particle coincidence techniques. The data are used to test a "sum-rule model" of complete- and incomplete-fusion reactions. The model assumes the reaction probabilities to be scaled by the available phase space and to be constrained additionally by the entrance-channel angular momentum limitations.
Перевод пока недоступен
Идентификаторы
Цитирования и источники
Цитирований: 3Использованных источников: 0