52-Te-133
Spin
Level energy(keV) Spin & Parity
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ground state (3/2+)
3.34270E+02 11/2-
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)
132.910968766 ± 0.000003873 (amu) [mass excess = -82932.060 ± 3.608 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
2954.511 ± 5.897 (keV)
Strong Gamma-rays from Decay of Te-133 (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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312.08 62.4 B-
407.63 27.08 B-
1333.21 10.67 B-
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334.27 7.17 IT
647.51 19.4 B-
863.96 15.64 B-
912.67 55.27 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- 55.4 M 4
B- 12.5 M 3
IT 55.4 M 4
Evaluated Data Libraries
Links to the libraries.
Parent Nuclides by Reactions in JENDL-4.0
Te-132 (Z= 52, A=132), MT=102 (n,γ)
I -135 (Z= 53, A=135), MT= 32 (n,nd)
I -135 (Z= 53, A=135), MT=105 (n,t)
Xe-135 (Z= 54, A=135), MT=106 (n,3He)
Xe-136 (Z= 54, A=136), MT=107 (n,α)
Cs-137 (Z= 55, A=137), MT=112 (n,pα)
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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Te-133 U-235 Thermal 1.209470e-02 7.256880e-04
Te-133 U-235 Fast 1.225550e-02 3.921750e-03
Te-133 U-235 High 5.344570e-03 3.420530e-03
Te-133 U-238 Fast 7.267300e-03 4.651070e-03
Te-133 U-238 High 5.555550e-03 3.555550e-03
Te-133 Pu-239 Thermal 1.364290e-02 1.500730e-03
Te-133 Pu-239 Fast 1.151670e-02 3.685360e-03
Te-133 Pu-239 High 3.828870e-03 2.450480e-03
Te-133 Pu-241 Thermal 1.180130e-02 3.776430e-03
Te-133 Pu-241 Fast 9.792570e-03 6.267250e-03
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Te-133m U-235 Thermal 2.918420e-02 1.751050e-03
Te-133m U-235 Fast 3.434320e-02 3.777760e-03
Te-133m U-235 High 2.451340e-02 7.844270e-03
Te-133m U-238 Fast 2.036500e-02 6.516800e-03
Te-133m U-238 High 2.548100e-02 8.153930e-03
Te-133m Pu-239 Thermal 3.292000e-02 1.975200e-03
Te-133m Pu-239 Fast 3.227310e-02 3.550030e-03
Te-133m Pu-239 High 1.756150e-02 5.619670e-03
Te-133m Pu-241 Thermal 2.847630e-02 9.112400e-03
Te-133m Pu-241 Fast 2.744150e-02 8.781290e-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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Te-133 U-235 Thermal 3.788900e-02 6.737330e-03
Te-133 U-235 Fast 3.269290e-02 9.273810e-03
Te-133 U-235 High 1.593010e-02 5.065890e-03
Te-133 U-238 Fast 4.358710e-02 1.238360e-02
Te-133 U-238 High 3.102940e-02 8.755770e-03
Te-133 Pu-239 Thermal 2.993870e-02 5.092670e-03
Te-133 Pu-239 Fast 2.784890e-02 5.820970e-03
Te-133 Pu-239 High 1.000190e-02 4.104460e-03
Te-133 Pu-241 Thermal 3.983710e-02 1.274170e-02
Te-133 Pu-241 Fast 3.563600e-02 9.488110e-03
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Te-133m U-235 Thermal 3.333100e-02 6.067110e-03
Te-133m U-235 Fast 3.722120e-02 5.336850e-03
Te-133m U-235 High 2.575980e-02 6.556990e-03
Te-133m U-238 Fast 2.696920e-02 1.256780e-02
Te-133m U-238 High 2.970170e-02 1.014320e-02
Te-133m Pu-239 Thermal 3.501380e-02 3.351530e-03
Te-133m Pu-239 Fast 3.439700e-02 3.772680e-03
Te-133m Pu-239 High 1.816970e-02 4.457830e-03
Te-133m Pu-241 Thermal 3.310320e-02 1.903070e-02
Te-133m Pu-241 Fast 3.166310e-02 1.056650e-02
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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