39-Y-96
Spin
Level energy(keV) Spin & Parity
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ground state 0-
1.14000E+03 (8+)
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)
95.915896835 ± 0.000006852 (amu) [mass excess = -78341.593 ± 6.383 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
7103.017 ± 6.087 (keV)
Strong Gamma-rays from Decay of Y- 96 (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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617.2 55. B-
914.8 58.96 B-
1750.6 88. B-
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475.3 0.19 B-
1750.4 2.35 B-
2225.6 0.32 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- 5.34 S 5
B- 9.6 S 2
Evaluated Data Libraries
Links to the libraries.
Parent Nuclides by Reactions in JENDL-4.0
Zr- 96 (Z= 40, A= 96), MT=103 (n,p)
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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Y- 96 U-235 Thermal 2.262880e-03 1.448240e-03
Y- 96 U-235 Fast 1.313730e-03 8.407860e-04
Y- 96 U-235 High 1.580620e-03 1.011600e-03
Y- 96 U-238 Fast 7.198190e-04 4.606840e-04
Y- 96 U-238 High 9.394610e-04 6.012550e-04
Y- 96 Pu-239 Thermal 2.510780e-03 1.606890e-03
Y- 96 Pu-239 Fast 2.041810e-03 1.306760e-03
Y- 96 Pu-239 High 1.382370e-03 8.847160e-04
Y- 96 Pu-241 Thermal 1.679380e-03 1.074800e-03
Y- 96 Pu-241 Fast 1.141020e-03 7.302550e-04
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Y- 96m U-235 Thermal 2.014190e-02 6.445400e-03
Y- 96m U-235 Fast 1.344730e-02 4.303140e-03
Y- 96m U-235 High 2.567140e-02 8.214860e-03
Y- 96m U-238 Fast 7.368040e-03 4.715540e-03
Y- 96m U-238 High 1.525810e-02 4.882600e-03
Y- 96m Pu-239 Thermal 2.234840e-02 1.005670e-02
Y- 96m Pu-239 Fast 2.089990e-02 6.687960e-03
Y- 96m Pu-239 High 2.245160e-02 5.163860e-03
Y- 96m Pu-241 Thermal 1.494810e-02 4.783400e-03
Y- 96m Pu-241 Fast 1.167950e-02 3.737420e-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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Y- 96 U-235 Thermal 3.972290e-02 2.245220e-02
Y- 96 U-235 Fast 4.716920e-02 1.378040e-02
Y- 96 U-235 High 2.110920e-02 3.377480e-03
Y- 96 U-238 Fast 5.258650e-02 8.813740e-03
Y- 96 U-238 High 3.966730e-02 1.554270e-02
Y- 96 Pu-239 Thermal 2.114400e-02 4.863110e-03
Y- 96 Pu-239 Fast 2.251460e-02 3.602330e-03
Y- 96 Pu-239 High 1.324590e-02 2.119340e-03
Y- 96 Pu-241 Thermal 2.775800e-02 1.499210e-02
Y- 96 Pu-241 Fast 3.022170e-02 1.197200e-02
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Y- 96m U-235 Thermal 2.014300e-02 9.078060e-03
Y- 96m U-235 Fast 1.344870e-02 3.099630e-03
Y- 96m U-235 High 2.567190e-02 5.895900e-03
Y- 96m U-238 Fast 7.369800e-03 3.315070e-03
Y- 96m U-238 High 1.525950e-02 3.505860e-03
Y- 96m Pu-239 Thermal 2.234890e-02 1.005840e-02
Y- 96m Pu-239 Fast 2.090040e-02 4.807770e-03
Y- 96m Pu-239 High 2.245190e-02 5.160610e-03
Y- 96m Pu-241 Thermal 1.494900e-02 3.437680e-03
Y- 96m Pu-241 Fast 1.168040e-02 2.688490e-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