Level energy(keV)   Spin & Parity       
       ground state      1/2+                  
       1.44780E+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)
     124.904429920 ± 0.000001614 (amu)  [mass excess = -89022.955 ± 1.504 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     -185.770 ± 0.060 (keV) 
Strong Gamma-rays from Decay of Te-125 (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 
         35.50            7.3          IT 
        109.28            0.28         IT 
        144.78          4.E-07         IT 
     *: 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 
       IT           57.40 D 15       
Cross Sections (taken from JENDL-4.0)
     Table of cross sections, Te-125.
     Figures of cross sections, Te-125:  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-124 (Z= 52, A=124), MT=102 (n,γ)
     Te-125 (Z= 52, A=125), MT=  2 (Elastic scattering)
     Te-125 (Z= 52, A=125), MT=  4 (Inelastic scattering)
     Te-126 (Z= 52, A=126), MT= 16 (n,2n)
     Te-127 (Z= 52, A=127), MT= 17 (n,3n)
     I -127 (Z= 53, A=127), MT= 32 (n,nd)
     I -127 (Z= 53, A=127), MT=105 (n,t)
     Xe-128 (Z= 54, A=128), MT=107 (n,α)
     Xe-129 (Z= 54, A=129), MT= 22 (n,nα)

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)
     Te-125    U-235   Thermal   6.980810e-14   4.467720e-14 
     Te-125    U-235   Fast      1.069960e-13   6.847750e-14 
     Te-125    U-235   High      3.755370e-07   2.403440e-07 
     Te-125    U-238   Fast      5.346120e-10   3.421510e-10 
     Te-125    U-238   High      3.899030e-09   2.495370e-09 
     Te-125   Pu-239   Thermal   1.452910e-11   9.298640e-12 
     Te-125   Pu-239   Fast      1.634110e-11   1.045830e-11 
     Te-125   Pu-239   High      8.769640e-06   5.612570e-06 
     Te-125   Pu-241   Thermal   7.840270e-14   5.017780e-14 
     Te-125   Pu-241   Fast      9.832330e-13   6.292690e-13 
     Te-125m   U-235   Thermal   2.285170e-13   1.462510e-13 
     Te-125m   U-235   Fast      4.049470e-13   2.591660e-13 
     Te-125m   U-235   High      2.326170e-06   1.488740e-06 
     Te-125m   U-238   Fast      2.023340e-09   1.294940e-09 
     Te-125m   U-238   High      2.415150e-08   1.545700e-08 
     Te-125m  Pu-239   Thermal   4.756110e-11   3.043910e-11 
     Te-125m  Pu-239   Fast      6.184620e-11   3.958150e-11 
     Te-125m  Pu-239   High      5.432130e-05   3.476560e-05 
     Te-125m  Pu-241   Thermal   2.566520e-13   1.642570e-13 
     Te-125m  Pu-241   Fast      3.721230e-12   2.381590e-12 
    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)
     Te-125    U-235   Thermal   3.396640e-04   6.824720e-06 
     Te-125    U-235   Fast      6.788980e-04   4.084150e-05 
     Te-125    U-235   High      1.462350e-02   1.168440e-03 
     Te-125    U-238   Fast      4.853520e-04   2.911480e-05 
     Te-125    U-238   High      1.196600e-02   4.785390e-04 
     Te-125   Pu-239   Thermal   1.116410e-03   8.932630e-05 
     Te-125   Pu-239   Fast      1.778170e-03   1.422740e-04 
     Te-125   Pu-239   High      1.956130e-02   1.563960e-03 
     Te-125   Pu-241   Thermal   4.690910e-04   3.752090e-05 
     Te-125   Pu-241   Fast      1.510010e-03   1.662320e-04 
     Te-125m   U-235   Thermal   1.188820e-04   4.239190e-05 
     Te-125m   U-235   Fast      2.376140e-04   8.542740e-05 
     Te-125m   U-235   High      5.119600e-03   1.906150e-03 
     Te-125m   U-238   Fast      1.698740e-04   6.131860e-05 
     Te-125m   U-238   High      4.188100e-03   1.505030e-03 
     Te-125m  Pu-239   Thermal   3.907430e-04   1.409560e-04 
     Te-125m  Pu-239   Fast      6.223600e-04   2.265340e-04 
     Te-125m  Pu-239   High      6.878620e-03   2.488410e-03 
     Te-125m  Pu-241   Thermal   1.641820e-04   5.978960e-05 
     Te-125m  Pu-241   Fast      5.285050e-04   2.427780e-04 
    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