55-Cs-136



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      5+                    
       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)
     135.907311358 ± 0.000002015 (amu)  [mass excess = -86338.914 ± 1.877 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     2548.224 ± 1.857 (keV) 
Strong Gamma-rays from Decay of Cs-136 (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 
  ----------------------------------------------------------
        340.55           42.17         B- 
        818.51           99.7          B- 
       1048.07           79.76         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-           13.16 D 3        
Cross Sections (taken from JENDL-4.0)
     Table of cross sections, Cs-136.
     Figures of cross sections, Cs-136:  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
     Cs-135 (Z= 55, A=135), MT=102 (n,γ)
     Cs-136 (Z= 55, A=136), MT=  2 (Elastic scattering)
     Cs-136 (Z= 55, A=136), MT=  4 (Inelastic scattering)
     Cs-137 (Z= 55, A=137), MT= 16 (n,2n)
     Ba-136 (Z= 56, A=136), MT=103 (n,p)
     Ba-137 (Z= 56, A=137), MT= 28 (n,np)
     Ba-137 (Z= 56, A=137), MT=104 (n,d)
     Ba-138 (Z= 56, A=138), MT=105 (n,t)
     La-138 (Z= 57, A=138), MT=106 (n,3He)
     La-139 (Z= 57, A=139), MT=107 (n,α)
     La-140 (Z= 57, A=140), 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)
    -----------------------------------------------------------
     Cs-136    U-235   Thermal   3.483390e-05   2.229370e-05 
     Cs-136    U-235   Fast      6.823340e-05   4.366940e-05 
     Cs-136    U-235   High      9.708780e-04   6.213600e-04 
     Cs-136    U-238   Fast      5.598890e-06   3.583290e-06 
     Cs-136    U-238   High      9.122710e-05   5.838560e-05 
     Cs-136   Pu-239   Thermal   6.137500e-04   3.928000e-04 
     Cs-136   Pu-239   Fast      7.175220e-04   4.592140e-04 
     Cs-136   Pu-239   High      3.233430e-03   2.069390e-03 
     Cs-136   Pu-241   Thermal   8.892620e-05   5.691280e-05 
     Cs-136   Pu-241   Fast      8.841540e-05   5.658590e-05 
    -----------------------------------------------------------
     Cs-136m   U-235   Thermal   2.045800e-05   1.309310e-05 
     Cs-136m   U-235   Fast      4.880500e-05   3.123520e-05 
     Cs-136m   U-235   High      1.292240e-03   8.270310e-04 
     Cs-136m   U-238   Fast      4.004690e-06   2.563000e-06 
     Cs-136m   U-238   High      1.214240e-04   7.771140e-05 
     Cs-136m  Pu-239   Thermal   3.604560e-04   2.306920e-04 
     Cs-136m  Pu-239   Fast      5.132190e-04   3.284600e-04 
     Cs-136m  Pu-239   High      4.303700e-03   2.754360e-03 
     Cs-136m  Pu-241   Thermal   5.222650e-05   3.342500e-05 
     Cs-136m  Pu-241   Fast      6.324050e-05   4.047390e-05 
    -----------------------------------------------------------
    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)
    -----------------------------------------------------------
     Cs-136    U-235   Thermal   5.529190e-05   3.538680e-05 
     Cs-136    U-235   Fast      1.170380e-04   7.490460e-05 
     Cs-136    U-235   High      2.263120e-03   1.353510e-03 
     Cs-136    U-238   Fast      9.603580e-06   6.146290e-06 
     Cs-136    U-238   High      2.126510e-04   1.272210e-04 
     Cs-136   Pu-239   Thermal   9.742070e-04   6.234930e-04 
     Cs-136   Pu-239   Fast      1.230740e-03   7.876730e-04 
     Cs-136   Pu-239   High      7.537130e-03   4.510770e-03 
     Cs-136   Pu-241   Thermal   1.411530e-04   9.033760e-05 
     Cs-136   Pu-241   Fast      1.516560e-04   9.705980e-05 
    -----------------------------------------------------------
     Cs-136m   U-235   Thermal   2.045800e-05   1.309310e-05 
     Cs-136m   U-235   Fast      4.880500e-05   3.123520e-05 
     Cs-136m   U-235   High      1.292240e-03   8.258060e-04 
     Cs-136m   U-238   Fast      4.004690e-06   2.562070e-06 
     Cs-136m   U-238   High      1.214240e-04   7.762720e-05 
     Cs-136m  Pu-239   Thermal   3.604560e-04   2.306920e-04 
     Cs-136m  Pu-239   Fast      5.132190e-04   3.284600e-04 
     Cs-136m  Pu-239   High      4.303700e-03   2.752580e-03 
     Cs-136m  Pu-241   Thermal   5.222650e-05   3.341960e-05 
     Cs-136m  Pu-241   Fast      6.324050e-05   4.047390e-05 
    -----------------------------------------------------------
    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