38-Sr-91



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      5/2+                  
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)
     90.910195442 ± 0.000006066 (amu)  [mass excess = -83652.406 ± 5.651 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     2699.470 ± 5.256 (keV) 
Strong Gamma-rays from Decay of Sr- 91 (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 
  ----------------------------------------------------------
        652.9             8.04         B- 
        749.8            23.68         B- 
       1024.3            33.5          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-           9.63 H 5         
Evaluated Data Libraries
     Links to the libraries. 

Parent Nuclides by Reactions in JENDL-4.0
     Sr- 90 (Z= 38, A= 90), MT=102 (n,γ)
     Y - 91 (Z= 39, A= 91), MT=103 (n,p)
     Zr- 93 (Z= 40, A= 93), MT=106 (n,3He)
     Zr- 94 (Z= 40, A= 94), MT=107 (n,α)
     Zr- 95 (Z= 40, A= 95), 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- 91    U-235   Thermal   2.501020e-03   1.500620e-04 
     Sr- 91    U-235   Fast      6.837840e-03   4.376220e-03 
     Sr- 91    U-235   High      5.073000e-03   3.246720e-03 
     Sr- 91    U-238   Fast      1.167640e-04   7.472870e-05 
     Sr- 91    U-238   High      6.954270e-04   4.450740e-04 
     Sr- 91   Pu-239   Thermal   3.860300e-03   6.176480e-04 
     Sr- 91   Pu-239   Fast      2.518540e-03   1.611860e-03 
     Sr- 91   Pu-239   High      3.698450e-03   2.367000e-03 
     Sr- 91   Pu-241   Thermal   6.701480e-04   4.288950e-04 
     Sr- 91   Pu-241   Fast      4.509210e-04   2.885890e-04 
    -----------------------------------------------------------
    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- 91    U-235   Thermal   5.815320e-02   5.953350e-04 
     Sr- 91    U-235   Fast      5.718960e-02   1.155520e-03 
     Sr- 91    U-235   High      4.817260e-02   1.925790e-03 
     Sr- 91    U-238   Fast      4.014440e-02   8.458210e-04 
     Sr- 91    U-238   High      3.856310e-02   1.088400e-03 
     Sr- 91   Pu-239   Thermal   2.483350e-02   4.968380e-04 
     Sr- 91   Pu-239   Fast      2.513570e-02   7.041300e-04 
     Sr- 91   Pu-239   High      2.222400e-02   2.444390e-03 
     Sr- 91   Pu-241   Thermal   1.862800e-02   5.220340e-04 
     Sr- 91   Pu-241   Fast      1.924950e-02   1.543440e-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