45-Rh-101



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      1/2-                  
       1.57410E+02       9/2+                  
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)
     100.906160613 ± 0.000006286 (amu)  [mass excess = -87410.826 ± 5.856 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     -1980.169 ± 3.903 (keV) 
Strong Gamma-rays from Decay of Rh-101 (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 
  ----------------------------------------------------------
        127.23           68.04         EC 
        198.01           73.           EC 
        325.23           11.83         EC 
  ----------------------------------------------------------
        157.41            0.24         IT 
        127.23            0.64         EC 
        306.86           80.59         EC 
        545.12            4.27         EC 
  ----------------------------------------------------------
     *: 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 
       EC           3.3 Y 3          
       EC           4.34 D 1         
       IT           4.34 D 1         
Evaluated Data Libraries
     Links to the libraries. 

Parent Nuclides by Reactions in JENDL-4.0
     Rh-103 (Z= 45, A=103), MT= 17 (n,3n)
     Pd-102 (Z= 46, A=102), MT= 28 (n,np)
     Pd-102 (Z= 46, A=102), MT=104 (n,d)

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)
    -----------------------------------------------------------
     Rh-101    U-235   Thermal   6.119060e-14   3.916190e-14 
     Rh-101    U-235   High      2.419150e-12   1.548260e-12 
     Rh-101   Pu-239   Thermal   8.862800e-14   5.672190e-14 
     Rh-101   Pu-239   Fast      5.826980e-14   3.729260e-14 
     Rh-101   Pu-239   High      1.663160e-10   1.064420e-10 
    -----------------------------------------------------------
     Rh-101m   U-235   High      1.918040e-11   1.227550e-11 
     Rh-101m  Pu-239   Thermal   3.827970e-13   2.449910e-13 
     Rh-101m  Pu-239   Fast      2.885740e-13   1.846880e-13 
     Rh-101m  Pu-239   High      1.318650e-09   8.439340e-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)
    -----------------------------------------------------------
     Rh-101    U-235   Thermal   6.119060e-14   3.916190e-14 
     Rh-101    U-235   High      3.646700e-12   2.333890e-12 
     Rh-101   Pu-239   Thermal   1.131270e-13   7.240150e-14 
     Rh-101   Pu-239   Fast      7.673850e-14   4.911260e-14 
     Rh-101   Pu-239   High      2.507090e-10   1.604540e-10 
    -----------------------------------------------------------
     Rh-101m   U-235   High      1.918040e-11   1.225730e-11 
     Rh-101m  Pu-239   Thermal   3.827970e-13   2.449910e-13 
     Rh-101m  Pu-239   Fast      2.885740e-13   1.846880e-13 
     Rh-101m  Pu-239   High      1.318650e-09   8.433870e-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