Level energy(keV)   Spin & Parity       
       ground state      (4+)                  
       ground state(+X)  (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)
     131.914507691 ± 0.000002900 (amu)  [mass excess = -79635.573 ± 2.701 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     5552.613 ± 4.410 (keV) 
Strong Gamma-rays from Decay of Sb-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 
        103.36         * 61.           B- 
        697.0          * 87.           B- 
        974.34         *100.           B- 
        697.05           86.13         B- 
        973.9            99.           B- 
        989.6            14.85         B- 
        150.67           66.           B- 
        697.05          100.           B- 
        973.9           100.           B- 
     *: 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-           2.79 M 7         
       B-           4.10 M 5         
       B-           4.10 M 5         
Evaluated Data Libraries
     Links to the libraries. 

Parent Nuclides by Reactions in JENDL-4.0
     Te-132 (Z= 52, A=132), MT=103 (n,p)
     I -135 (Z= 53, A=135), MT=107 (n,α)

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)
     Sb-132    U-235   Thermal   1.245860e-02   7.475160e-04 
     Sb-132    U-235   Fast      1.725820e-02   5.522610e-03 
     Sb-132    U-235   High      5.575700e-03   3.568450e-03 
     Sb-132    U-238   Fast      1.436930e-02   4.598170e-03 
     Sb-132    U-238   High      1.024270e-02   3.277660e-03 
     Sb-132   Pu-239   Thermal   1.382370e-02   1.520600e-03 
     Sb-132   Pu-239   Fast      1.020820e-02   3.266640e-03 
     Sb-132   Pu-239   High      3.322820e-03   2.126610e-03 
     Sb-132   Pu-241   Thermal   1.481680e-02   4.741400e-03 
     Sb-132   Pu-241   Fast      1.288780e-02   4.124110e-03 
     Sb-132m   U-235   Thermal   9.170930e-03   5.502560e-04 
     Sb-132m   U-235   Fast      1.530450e-02   4.897430e-03 
     Sb-132m   U-235   High      8.869120e-03   5.676240e-03 
     Sb-132m   U-238   Fast      1.274260e-02   4.077610e-03 
     Sb-132m   U-238   High      1.629280e-02   5.213680e-03 
     Sb-132m  Pu-239   Thermal   1.017570e-02   1.119330e-03 
     Sb-132m  Pu-239   Fast      9.052590e-03   5.793660e-03 
     Sb-132m  Pu-239   High      5.285530e-03   3.382740e-03 
     Sb-132m  Pu-241   Thermal   1.090680e-02   3.490180e-03 
     Sb-132m  Pu-241   Fast      1.142880e-02   3.657230e-03 
    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)
     Sb-132    U-235   Thermal   1.842820e-02   3.103950e-03 
     Sb-132    U-235   Fast      2.048380e-02   6.252450e-03 
     Sb-132    U-235   High      6.595080e-03   2.783090e-03 
     Sb-132    U-238   Fast      3.387950e-02   1.051650e-02 
     Sb-132    U-238   High      1.569300e-02   4.048870e-03 
     Sb-132   Pu-239   Thermal   1.868000e-02   2.752480e-03 
     Sb-132   Pu-239   Fast      1.250890e-02   2.854210e-03 
     Sb-132   Pu-239   High      3.763990e-03   2.277210e-03 
     Sb-132   Pu-241   Thermal   2.009720e-02   4.806710e-03 
     Sb-132   Pu-241   Fast      1.968110e-02   5.050670e-03 
     Sb-132m   U-235   Thermal   9.172720e-03   3.039960e-03 
     Sb-132m   U-235   Fast      1.530620e-02   5.668400e-03 
     Sb-132m   U-235   High      8.869370e-03   4.243150e-03 
     Sb-132m   U-238   Fast      1.275140e-02   2.040220e-03 
     Sb-132m   U-238   High      1.629500e-02   5.135170e-03 
     Sb-132m  Pu-239   Thermal   1.017620e-02   2.544410e-03 
     Sb-132m  Pu-239   Fast      9.053060e-03   4.734030e-03 
     Sb-132m  Pu-239   High      5.285630e-03   3.382800e-03 
     Sb-132m  Pu-241   Thermal   1.090890e-02   4.079970e-03 
     Sb-132m  Pu-241   Fast      1.143090e-02   4.820170e-03 
    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