38-Sr-92



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      0+                    
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)
     91.911038190 ± 0.000003676 (amu)  [mass excess = -82867.392 ± 3.424 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     1949.662 ± 9.451 (keV) 
Strong Gamma-rays from Decay of Sr- 92 (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 
  ----------------------------------------------------------
        430.49            3.28         B- 
        953.31            3.52         B- 
       1383.93           90.           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-           2.71 H 1         
Evaluated Data Libraries
     Links to the libraries. 

Parent Nuclides by Reactions in JENDL-4.0
     Zr- 95 (Z= 40, A= 95), MT=107 (n,α)
     Zr- 96 (Z= 40, A= 96), 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)
    -----------------------------------------------------------
     Sr- 92    U-235   Thermal   1.073550e-02   6.441270e-04 
     Sr- 92    U-235   Fast      1.610920e-02   5.154950e-03 
     Sr- 92    U-235   High      1.253520e-02   4.011270e-03 
     Sr- 92    U-238   Fast      1.030570e-03   6.595610e-04 
     Sr- 92    U-238   High      2.637130e-03   1.687760e-03 
     Sr- 92   Pu-239   Thermal   1.024220e-02   6.145320e-04 
     Sr- 92   Pu-239   Fast      9.615190e-03   4.326840e-03 
     Sr- 92   Pu-239   High      9.793660e-03   6.267940e-03 
     Sr- 92   Pu-241   Thermal   3.236140e-03   2.071140e-03 
     Sr- 92   Pu-241   Fast      2.772100e-03   1.774150e-03 
    -----------------------------------------------------------
    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)
    -----------------------------------------------------------
     Sr- 92    U-235   Thermal   5.931970e-02   8.333950e-04 
     Sr- 92    U-235   Fast      5.838940e-02   1.169330e-03 
     Sr- 92    U-235   High      5.073840e-02   5.570240e-03 
     Sr- 92    U-238   Fast      4.342720e-02   1.245290e-03 
     Sr- 92    U-238   High      3.895760e-02   1.102860e-03 
     Sr- 92   Pu-239   Thermal   2.964470e-02   8.299260e-04 
     Sr- 92   Pu-239   Fast      3.017730e-02   8.449180e-04 
     Sr- 92   Pu-239   High      2.821090e-02   6.481400e-03 
     Sr- 92   Pu-241   Thermal   2.307890e-02   9.225410e-04 
     Sr- 92   Pu-241   Fast      2.393150e-02   1.914110e-03 
    -----------------------------------------------------------
    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