61-Pm-161
Mass (The Ame2012 atomic mass evaluation (II) by M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, and B.Pfeiffer
Chinese Physics C36 p. 1603-2014, December 2012)
160.946070 ± 0.000320 (amu) [mass excess = -50235 ± 298 (keV) ]
[These values were derived from systematical trend]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
6436 ± 298 (keV) [derived from systematical trend]
Evaluated Data Libraries
Links to the libraries.
Parent Nuclides by Reactions in JENDL-4.0
Fission Yields for Fission Products in JENDL-4.0 Fission Yield Data
- Neutron-induced Fission Yields (from main actinide nuclides) - Independent Fission Yield -
Product Nuclide Energy Fission Yield Uncertainty(1σ)
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Pm-161 U-235 Thermal 4.393010e-09 2.811520e-09
Pm-161 U-235 Fast 4.520670e-08 2.893220e-08
Pm-161 U-235 High 6.438820e-08 4.120840e-08
Pm-161 U-238 Fast 1.280480e-06 8.195050e-07
Pm-161 U-238 High 4.034400e-06 2.582010e-06
Pm-161 Pu-239 Thermal 1.039840e-07 6.654950e-08
Pm-161 Pu-239 Fast 1.109820e-07 7.102850e-08
Pm-161 Pu-239 High 3.262120e-08 2.087750e-08
Pm-161 Pu-241 Thermal 2.440400e-06 1.561850e-06
Pm-161 Pu-241 Fast 2.797900e-06 1.790650e-06
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Thermal=0.0253eV, Fast=500keV(Fast reactor spectrum), High=14MeV
- Neutron-induced Fission Yields (from main actinide nuclides) - Cumulative Fission Yield -
Product Nuclide Energy Fission Yield Uncertainty(1σ)
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Pm-161 U-235 Thermal 4.399160e-09 2.815460e-09
Pm-161 U-235 Fast 4.533640e-08 2.901520e-08
Pm-161 U-235 High 6.449540e-08 4.121140e-08
Pm-161 U-238 Fast 1.297890e-06 8.306450e-07
Pm-161 U-238 High 4.072940e-06 2.604810e-06
Pm-161 Pu-239 Thermal 1.040970e-07 6.655930e-08
Pm-161 Pu-239 Fast 1.110810e-07 7.103880e-08
Pm-161 Pu-239 High 3.265630e-08 2.090000e-08
Pm-161 Pu-241 Thermal 2.450900e-06 1.568000e-06
Pm-161 Pu-241 Fast 2.805310e-06 1.795400e-06
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Thermal=0.0253eV, Fast=500keV(Fast reactor spectrum), High=14MeV
→ Neutron-induced and Spontaneous Fission Yields of all nuclides in JENDL-4.0 Fission Yield Data