56-Ba-135



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      3/2+                  
       2.68218E+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)
     134.905688375 ± 0.000000294 (amu)  [mass excess = -87850.713 ± 0.274 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     -1207.205 ± 9.430 (keV) 
Strong Gamma-rays from Decay of Ba-135 (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 
  ----------------------------------------------------------
        268.22           16.           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           28.7 H 2         
Cross Sections (taken from JENDL-4.0)
     Table of cross sections, Ba-135.
     Figures of cross sections, Ba-135:  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
     Ba-134 (Z= 56, A=134), MT=102 (n,γ)
     Ba-135 (Z= 56, A=135), MT=  2 (Elastic scattering)
     Ba-135 (Z= 56, A=135), MT=  4 (Inelastic scattering)
     Ba-136 (Z= 56, A=136), MT= 16 (n,2n)
     Ba-137 (Z= 56, A=137), MT= 17 (n,3n)
     La-138 (Z= 57, A=138), MT= 33 (n,nt)

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)
    -----------------------------------------------------------
     Ba-135    U-235   Thermal   2.234960e-10   1.430380e-10 
     Ba-135    U-235   Fast      6.430230e-11   4.115340e-11 
     Ba-135    U-235   High      5.341520e-07   3.418570e-07 
     Ba-135    U-238   Fast      5.946030e-12   3.805450e-12 
     Ba-135    U-238   High      3.458470e-09   2.213420e-09 
     Ba-135   Pu-239   Thermal   3.574030e-08   2.287380e-08 
     Ba-135   Pu-239   Fast      3.339560e-08   2.137320e-08 
     Ba-135   Pu-239   High      4.554920e-06   2.915150e-06 
     Ba-135   Pu-241   Thermal   3.809620e-10   2.438160e-10 
     Ba-135   Pu-241   Fast      4.467640e-10   2.859290e-10 
    -----------------------------------------------------------
     Ba-135m   U-235   Thermal   5.392890e-10   3.451460e-10 
     Ba-135m   U-235   Fast      1.801930e-10   1.153230e-10 
     Ba-135m   U-235   High      2.449940e-06   1.567960e-06 
     Ba-135m   U-238   Fast      1.666250e-11   1.066390e-11 
     Ba-135m   U-238   High      1.586260e-08   1.015210e-08 
     Ba-135m  Pu-239   Thermal   8.624030e-08   5.519380e-08 
     Ba-135m  Pu-239   Fast      9.358390e-08   5.989370e-08 
     Ba-135m  Pu-239   High      2.089160e-05   1.337060e-05 
     Ba-135m  Pu-241   Thermal   9.192490e-10   5.883190e-10 
     Ba-135m  Pu-241   Fast      1.251960e-09   8.012530e-10 
    -----------------------------------------------------------
    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)
    -----------------------------------------------------------
     Ba-135    U-235   Thermal   6.523550e-02   2.760680e-04 
     Ba-135    U-235   Fast      6.579160e-02   5.123310e-04 
     Ba-135    U-235   High      5.735910e-02   3.438100e-03 
     Ba-135    U-238   Fast      6.922840e-02   6.621210e-04 
     Ba-135    U-238   High      5.835060e-02   1.170420e-03 
     Ba-135   Pu-239   Thermal   7.617450e-02   5.345800e-04 
     Ba-135   Pu-239   Fast      7.551280e-02   3.790490e-04 
     Ba-135   Pu-239   High      6.379710e-02   7.013300e-03 
     Ba-135   Pu-241   Thermal   7.163080e-02   7.211880e-04 
     Ba-135   Pu-241   Fast      7.054840e-02   1.000770e-03 
    -----------------------------------------------------------
     Ba-135m   U-235   Thermal   5.392890e-10   3.451460e-10 
     Ba-135m   U-235   Fast      1.801930e-10   1.153230e-10 
     Ba-135m   U-235   High      2.449940e-06   1.565640e-06 
     Ba-135m   U-238   Fast      1.666250e-11   1.066000e-11 
     Ba-135m   U-238   High      1.586260e-08   1.014110e-08 
     Ba-135m  Pu-239   Thermal   8.624030e-08   5.519380e-08 
     Ba-135m  Pu-239   Fast      9.358390e-08   5.989370e-08 
     Ba-135m  Pu-239   High      2.089160e-05   1.336190e-05 
     Ba-135m  Pu-241   Thermal   9.192490e-10   5.882240e-10 
     Ba-135m  Pu-241   Fast      1.251960e-09   8.012530e-10 
    -----------------------------------------------------------
    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