50-Sn-130
Spin
Level energy(keV) Spin & Parity
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ground state 0+
1.94688E+03 (7-)
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)
129.913973830 ± 0.000002282 (amu) [mass excess = -80132.861 ± 2.126 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
2153.406 ± 14.113 (keV)
Strong Gamma-rays from Decay of Sn-130 (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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84.67 9.54 B-
144.91 22.66 B-
733.4 23. B-
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70.01 34.1 B-
192.42 67. B-
780.44 56.43 B-
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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
B- 1.7 M 1
B- 3.72 M 7
Evaluated Data Libraries
Links to the libraries.
Parent Nuclides by Reactions in JENDL-4.0
Te-132 (Z= 52, A=132), MT=106 (n,3He)
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-130 U-235 Thermal 3.237660e-03 2.072100e-03
Sn-130 U-235 Fast 3.537410e-03 2.263940e-03
Sn-130 U-235 High 1.485650e-03 9.508170e-04
Sn-130 U-238 Fast 4.414600e-03 2.825340e-03
Sn-130 U-238 High 2.772260e-03 1.774250e-03
Sn-130 Pu-239 Thermal 2.808820e-03 1.797640e-03
Sn-130 Pu-239 Fast 2.912430e-03 1.863960e-03
Sn-130 Pu-239 High 1.008860e-03 6.456730e-04
Sn-130 Pu-241 Thermal 3.733450e-03 2.389400e-03
Sn-130 Pu-241 Fast 3.743240e-03 2.395670e-03
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Sn-130m U-235 Thermal 7.590640e-03 4.858010e-03
Sn-130m U-235 Fast 9.661880e-03 6.183610e-03
Sn-130m U-235 High 6.722370e-03 4.302320e-03
Sn-130m U-238 Fast 1.205780e-02 7.716980e-03
Sn-130m U-238 High 1.254410e-02 8.028230e-03
Sn-130m Pu-239 Thermal 6.585220e-03 4.214540e-03
Sn-130m Pu-239 Fast 7.954860e-03 5.091120e-03
Sn-130m Pu-239 High 4.564970e-03 2.921580e-03
Sn-130m Pu-241 Thermal 8.753000e-03 5.601910e-03
Sn-130m Pu-241 Fast 1.022410e-02 6.543410e-03
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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-130 U-235 Thermal 4.226240e-03 2.531220e-03
Sn-130 U-235 Fast 4.676900e-03 2.712320e-03
Sn-130 U-235 High 2.009790e-03 1.155210e-03
Sn-130 U-238 Fast 5.402610e-03 3.196800e-03
Sn-130 U-238 High 5.372350e-03 2.926320e-03
Sn-130 Pu-239 Thermal 3.247280e-03 1.958910e-03
Sn-130 Pu-239 Fast 3.436640e-03 2.058420e-03
Sn-130 Pu-239 High 1.253370e-03 7.377990e-04
Sn-130 Pu-241 Thermal 3.872440e-03 2.440310e-03
Sn-130 Pu-241 Fast 3.893370e-03 2.453430e-03
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Sn-130m U-235 Thermal 7.594200e-03 4.860290e-03
Sn-130m U-235 Fast 9.665560e-03 6.185950e-03
Sn-130m U-235 High 6.722930e-03 4.302670e-03
Sn-130m U-238 Fast 1.206040e-02 7.718670e-03
Sn-130m U-238 High 1.254870e-02 8.031190e-03
Sn-130m Pu-239 Thermal 6.586080e-03 4.215090e-03
Sn-130m Pu-239 Fast 7.955780e-03 5.091700e-03
Sn-130m Pu-239 High 4.565180e-03 2.921710e-03
Sn-130m Pu-241 Thermal 8.756040e-03 5.603870e-03
Sn-130m Pu-241 Fast 1.022790e-02 6.545830e-03
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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