52-Te-132
Spin
Level energy(keV) Spin & Parity
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ground state 0+
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)
131.908546716 ± 0.000003742 (amu) [mass excess = -85188.185 ± 3.486 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
515.305 ± 3.483 (keV)
Strong Gamma-rays from Decay of Te-132 (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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49.72 14.96 B-
116.30 1.96 B-
228.16 88. B-
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103.4 39.7 IT
696.9 99.7 IT
974.0 99.8 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
B- 3.204 D 13
Cross Sections (taken from JENDL-4.0)
Table of cross sections, Te-132.
Figures of cross sections, Te-132: type-1: type-2: type-3.
type-1: total, elastic and inelastic scattering, capture and fision cross sections
type-2: same as type-1 but cross sections are averaged in 70 energy group intervals
type-3: threshold reaction cross sections
Evaluated Data Libraries
Links to the libraries.
Parent Nuclides by Reactions in JENDL-4.0
Te-132 (Z= 52, A=132), MT= 2 (Elastic scattering)
Te-132 (Z= 52, A=132), MT= 4 (Inelastic scattering)
Xe-134 (Z= 54, A=134), MT=106 (n,3He)
Xe-135 (Z= 54, A=135), MT=107 (n,α)
Xe-136 (Z= 54, A=136), MT= 22 (n,nα)
Cs-136 (Z= 55, A=136), MT=112 (n,pα)
Cs-137 (Z= 55, A=137), MT= 45 (n,npα)
Cs-137 (Z= 55, A=137), MT=117 (n,dα)
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-132 U-235 Thermal 1.528510e-02 9.171080e-04
Te-132 U-235 Fast 1.072530e-02 1.716040e-03
Te-132 U-235 High 2.549370e-02 4.079000e-03
Te-132 U-238 Fast 4.713940e-03 3.016920e-03
Te-132 U-238 High 1.459310e-02 3.356420e-03
Te-132 Pu-239 Thermal 2.253180e-02 1.351910e-03
Te-132 Pu-239 Fast 2.996730e-02 4.794760e-03
Te-132 Pu-239 High 2.392380e-02 3.827810e-03
Te-132 Pu-241 Thermal 1.403800e-02 3.228730e-03
Te-132 Pu-241 Fast 1.564790e-02 3.599020e-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-132 U-235 Thermal 4.288600e-02 6.044570e-04
Te-132 U-235 Fast 4.651530e-02 9.367230e-04
Te-132 U-235 High 4.095820e-02 1.637020e-03
Te-132 U-238 Fast 5.134480e-02 7.211300e-04
Te-132 U-238 High 4.658120e-02 6.539950e-04
Te-132 Pu-239 Thermal 5.138800e-02 1.027910e-03
Te-132 Pu-239 Fast 5.152920e-02 1.030740e-03
Te-132 Pu-239 High 3.297340e-02 1.977230e-03
Te-132 Pu-241 Thermal 4.504400e-02 1.260970e-03
Te-132 Pu-241 Fast 4.676000e-02 2.807620e-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