59-Pr-142



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      2-                    
       3.68300E+00       5-                    
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)
     141.910049607 ± 0.000002291 (amu)  [mass excess = -83788.251 ± 2.135 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     2161.635 ± 1.487 (keV) 
Strong Gamma-rays from Decay of Pr-142 (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 
  ----------------------------------------------------------
        642.0           2.E-03         EC 
        508.8             0.02         B- 
       1575.6             3.68         B- 
  ----------------------------------------------------------
         86.7             --           IT 
        268.2             --           IT 
        553.0             --           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 
       B-           19.12 H 4        
       EC           19.12 H 4        
Evaluated Data Libraries
     Links to the libraries. 

Parent Nuclides by Reactions in JENDL-4.0
     Pr-141 (Z= 59, A=141), MT=102 (n,γ)
     Pr-143 (Z= 59, A=143), MT= 16 (n,2n)
     Nd-142 (Z= 60, A=142), MT=103 (n,p)
     Nd-143 (Z= 60, A=143), MT= 28 (n,np)
     Nd-143 (Z= 60, A=143), MT=104 (n,d)
     Nd-144 (Z= 60, A=144), MT= 32 (n,nd)
     Nd-144 (Z= 60, A=144), MT= 41 (n,2np)
     Nd-144 (Z= 60, A=144), MT=105 (n,t)
     Nd-145 (Z= 60, A=145), MT= 33 (n,nt)
     Pm-147 (Z= 61, A=147), MT= 24 (n,2nα)

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)
    -----------------------------------------------------------
     Pr-142    U-235   Thermal   1.382170e-11   8.845910e-12 
     Pr-142    U-235   Fast      4.198930e-12   2.687320e-12 
     Pr-142    U-235   High      5.509960e-08   3.526370e-08 
     Pr-142    U-238   Fast      2.000020e-13   1.280020e-13 
     Pr-142    U-238   High      8.316960e-11   5.322870e-11 
     Pr-142   Pu-239   Thermal   3.258580e-09   2.085500e-09 
     Pr-142   Pu-239   Fast      3.108300e-09   1.989310e-09 
     Pr-142   Pu-239   High      9.309440e-07   5.958040e-07 
     Pr-142   Pu-241   Thermal   8.193930e-12   5.244110e-12 
     Pr-142   Pu-241   Fast      1.518420e-11   9.717880e-12 
    -----------------------------------------------------------
     Pr-142m   U-235   Thermal   3.240470e-11   2.073910e-11 
     Pr-142m   U-235   Fast      1.146870e-11   7.339990e-12 
     Pr-142m   U-235   High      2.493180e-07   1.595630e-07 
     Pr-142m   U-238   Fast      5.462750e-13   3.496170e-13 
     Pr-142m   U-238   High      3.763310e-10   2.408520e-10 
     Pr-142m  Pu-239   Thermal   7.639690e-09   4.889410e-09 
     Pr-142m  Pu-239   Fast      8.489830e-09   5.433480e-09 
     Pr-142m  Pu-239   High      4.212390e-06   2.695930e-06 
     Pr-142m  Pu-241   Thermal   1.921050e-11   1.229470e-11 
     Pr-142m  Pu-241   Fast      4.147320e-11   2.654290e-11 
    -----------------------------------------------------------
    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)
    -----------------------------------------------------------
     Pr-142    U-235   Thermal   4.622650e-11   2.541190e-11 
     Pr-142    U-235   Fast      1.566770e-11   8.519500e-12 
     Pr-142    U-235   High      3.044180e-07   1.644420e-07 
     Pr-142    U-238   Fast      7.462770e-13   4.055860e-13 
     Pr-142    U-238   High      4.595000e-10   2.482060e-10 
     Pr-142   Pu-239   Thermal   1.089830e-08   5.988290e-09 
     Pr-142   Pu-239   Fast      1.159810e-08   6.304030e-09 
     Pr-142   Pu-239   High      5.143340e-06   2.778130e-06 
     Pr-142   Pu-241   Thermal   2.740440e-11   1.505640e-11 
     Pr-142   Pu-241   Fast      5.665740e-11   3.079950e-11 
    -----------------------------------------------------------
     Pr-142m   U-235   Thermal   3.240470e-11   2.073910e-11 
     Pr-142m   U-235   Fast      1.146870e-11   7.339990e-12 
     Pr-142m   U-235   High      2.493180e-07   1.593270e-07 
     Pr-142m   U-238   Fast      5.462750e-13   3.494890e-13 
     Pr-142m   U-238   High      3.763310e-10   2.405910e-10 
     Pr-142m  Pu-239   Thermal   7.639690e-09   4.889410e-09 
     Pr-142m  Pu-239   Fast      8.489830e-09   5.433480e-09 
     Pr-142m  Pu-239   High      4.212390e-06   2.694180e-06 
     Pr-142m  Pu-241   Thermal   1.921050e-11   1.229270e-11 
     Pr-142m  Pu-241   Fast      4.147320e-11   2.654290e-11 
    -----------------------------------------------------------
    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