Evidence for Nuclear Superfluidity in U236 Isomeric- and Prompt-Fission Modes
C. A. Fontenla, Doracy P. Fontenla
Abstract
C. A. Fontenla, Doracy P. Fontenla
Abstract
Isomer fission in $^{236m}\mathrm{U}$, ${t}_{\frac{1}{2}}=125$ nsec, from $^{235}\mathrm{U}(d, pf)$ was compared with prompt fission $^{235}\mathrm{U}({n}_{\mathrm{th}}, f)$, in twin experiments. Fine structure in the total kinetic energy, average total kinetic energy as a function of mass, and mass yield were observed in isomer fission of $^{236m}\mathrm{U}$. This observation is compatible with a superfluid descent from saddle to scission points. Two peaks in the total-kinetic-energy distribution from isomer fission are observed near fragment mass 132, and this is interpreted as due to the proton-pairing effect at $Z=50$.
OpenAlex reports 3 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
Isomer fission in $^{236m}\mathrm{U}$, ${t}_{\frac{1}{2}}=125$ nsec, from $^{235}\mathrm{U}(d, pf)$ was compared with prompt fission $^{235}\mathrm{U}({n}_{\mathrm{th}}, f)$, in twin experiments. Fine structure in the total kinetic energy, average total kinetic energy as a function of mass, and mass yield were observed in isomer fission of $^{236m}\mathrm{U}$. This observation is compatible with a superfluid descent from saddle to scission points. Two peaks in the total-kinetic-energy distribution from isomer fission are observed near fragment mass 132, and this is interpreted as due to the proton-pairing effect at $Z=50$.
Key concepts: Physics, Kinetic energy, Fission, Superfluidity, Energy (signal processing), Nuclear physics, Atomic physics, Neutron