67-Ho-170



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      (6+)                  
       1.20000E+02       (1+)                  
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)
     169.939624846 ± 0.000053738 (amu)  [mass excess = -56239.094 ± 50.057 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     3870.000 ± 50.000 (keV) 
Strong Gamma-rays from Decay of Ho-170 (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 
  ----------------------------------------------------------
         78.7          * 40.           B- 
        812.3          *100.           B- 
       1894.0          * 45.2          B- 
  ----------------------------------------------------------
        181.57           23.33         B- 
        258.17           36.29         B- 
        932.1            35.42         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-           2.76 M 5         
       B-           43 S 2           
Evaluated Data Libraries
     Links to the libraries. 

Parent Nuclides by Reactions in JENDL-4.0
     Er-170 (Z= 68, A=170), MT=103 (n,p)

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)
    -----------------------------------------------------------
     Ho-170    U-235   Thermal   6.900870e-12   4.416560e-12 
     Ho-170    U-235   Fast      1.723960e-11   1.103330e-11 
     Ho-170    U-235   High      1.476220e-07   9.447830e-08 
     Ho-170    U-238   Fast      2.797280e-09   1.790260e-09 
     Ho-170    U-238   High      6.001620e-08   3.841030e-08 
     Ho-170   Pu-239   Thermal   8.172370e-10   5.230310e-10 
     Ho-170   Pu-239   Fast      2.385930e-08   1.527000e-08 
     Ho-170   Pu-239   High      1.999660e-07   1.279780e-07 
     Ho-170   Pu-241   Thermal   1.076910e-09   6.892230e-10 
     Ho-170   Pu-241   Fast      2.150460e-08   1.376300e-08 
    -----------------------------------------------------------
     Ho-170m   U-235   Thermal   2.943450e-12   1.883810e-12 
     Ho-170m   U-235   Fast      6.311770e-12   4.039530e-12 
     Ho-170m   U-235   High      3.262470e-08   2.087980e-08 
     Ho-170m   U-238   Fast      1.024140e-09   6.554520e-10 
     Ho-170m   U-238   High      1.326370e-08   8.488730e-09 
     Ho-170m  Pu-239   Thermal   3.485790e-10   2.230900e-10 
     Ho-170m  Pu-239   Fast      8.735380e-09   5.590640e-09 
     Ho-170m  Pu-239   High      4.419270e-08   2.828330e-08 
     Ho-170m  Pu-241   Thermal   4.593380e-10   2.939770e-10 
     Ho-170m  Pu-241   Fast      7.873280e-09   5.038900e-09 
    -----------------------------------------------------------
    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)
    -----------------------------------------------------------
     Ho-170    U-235   Thermal   6.900870e-12   3.105390e-12 
     Ho-170    U-235   Fast      1.723960e-11   7.757840e-12 
     Ho-170    U-235   High      1.476220e-07   9.447780e-08 
     Ho-170    U-238   Fast      2.797280e-09   1.258770e-09 
     Ho-170    U-238   High      6.001620e-08   1.920520e-08 
     Ho-170   Pu-239   Thermal   8.172370e-10   5.230320e-10 
     Ho-170   Pu-239   Fast      2.385930e-08   1.527000e-08 
     Ho-170   Pu-239   High      1.999660e-07   1.279780e-07 
     Ho-170   Pu-241   Thermal   1.076910e-09   4.846080e-10 
     Ho-170   Pu-241   Fast      2.150460e-08   9.677080e-09 
    -----------------------------------------------------------
     Ho-170m   U-235   Thermal   4.244740e-11   2.716640e-11 
     Ho-170m   U-235   Fast      1.738020e-10   1.112330e-10 
     Ho-170m   U-235   High      1.307880e-07   8.370430e-08 
     Ho-170m   U-238   Fast      9.935240e-08   6.358570e-08 
     Ho-170m   U-238   High      5.340010e-07   3.417600e-07 
     Ho-170m  Pu-239   Thermal   2.222100e-09   1.422140e-09 
     Ho-170m  Pu-239   Fast      4.723760e-08   3.023200e-08 
     Ho-170m  Pu-239   High      1.001950e-07   6.275670e-08 
     Ho-170m  Pu-241   Thermal   1.533090e-08   9.811780e-09 
     Ho-170m  Pu-241   Fast      1.426970e-07   9.132610e-08 
    -----------------------------------------------------------
    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