50-Sn-113
Spin
Level energy(keV) Spin & Parity
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ground state 1/2+
7.73800E+01 7/2+
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)
112.905175728 ± 0.000001762 (amu) [mass excess = -88328.240 ± 1.642 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
-3911.164 ± 17.121 (keV)
Strong Gamma-rays from Decay of Sn-113 (Compiled from ENSDF as of March 2011)
[ Intensities before May 23th of 2013 were values when total intensity of the decay mode was 100(%) and a branching ratio of each decay mode was not multiplied. ]
γ-ray energy(keV) Intensity(%) Decay mode
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255.13 2.11 EC
391.70 64.97 EC
638.03 1.E-03 EC
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77. 0.5 IT
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*: relative, ~ approximate, ? calculated or estimatted
>: greater than or equal to, <: less than or equal to
[ Intensities; total intensity of the nuclide is 100(%). ]
Decay data(Chart of the Nuclides 2014)
Decay mode Half-life
EC 21.4 M 4
EC 115.09 D 3
IT 21.4 M 4
Evaluated Data Libraries
Links to the libraries.
Parent Nuclides by Reactions in JENDL-4.0
Sn-112 (Z= 50, A=112), MT=102 (n,γ)
Sn-114 (Z= 50, A=114), MT= 16 (n,2n)
Sn-115 (Z= 50, A=115), MT= 17 (n,3n)
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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Sn-113 Pu-239 High 1.872310e-13 1.198280e-13
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Sn-113m Pu-239 High 2.244350e-12 1.436380e-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)
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Sn-113 Pu-239 High 2.231830e-12 1.251150e-12
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Sn-113m Pu-239 High 2.244350e-12 1.435450e-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