42-Mo-116
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)
115.955448 ± 0.000537 (amu) [mass excess = -41500 ± 500 (keV) ]
[These values were derived from systematical trend]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
9956 ± 582 (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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Mo-116 U-235 Fast 5.837950e-14 3.736290e-14
Mo-116 U-235 High 3.935390e-10 2.518650e-10
Mo-116 U-238 Fast 1.220410e-10 7.810620e-11
Mo-116 U-238 High 2.682380e-09 1.716720e-09
Mo-116 Pu-239 Thermal 1.159820e-13 7.422830e-14
Mo-116 Pu-239 Fast 1.189810e-13 7.614770e-14
Mo-116 Pu-239 High 3.162050e-11 2.023710e-11
Mo-116 Pu-241 Thermal 6.080840e-12 3.891740e-12
Mo-116 Pu-241 Fast 6.714950e-12 4.297570e-12
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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)
-----------------------------------------------------------
Mo-116 U-235 Fast 5.837950e-14 3.736290e-14
Mo-116 U-235 High 3.935390e-10 2.514920e-10
Mo-116 U-238 Fast 1.220410e-10 7.808050e-11
Mo-116 U-238 High 2.682380e-09 1.715210e-09
Mo-116 Pu-239 Thermal 1.159820e-13 7.422830e-14
Mo-116 Pu-239 Fast 1.189810e-13 7.614770e-14
Mo-116 Pu-239 High 3.162050e-11 2.022400e-11
Mo-116 Pu-241 Thermal 6.080840e-12 3.891200e-12
Mo-116 Pu-241 Fast 6.714950e-12 4.297570e-12
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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