39-Y-93



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      1/2-                  
       7.58721E+02       7/2+                  
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)
     92.909577886 ± 0.000011351 (amu)  [mass excess = -84227.656 ± 10.574 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     2895.027 ± 10.491 (keV) 
Strong Gamma-rays from Decay of Y- 93 (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 
  ----------------------------------------------------------
        266.9             7.32         B- 
        947.1             2.09         B- 
       1917.8             1.54         B- 
  ----------------------------------------------------------
        168.50           51.28         IT 
        590.24           99.8          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-           10.18 H 8        
       IT           0.82 S 4         
Evaluated Data Libraries
     Links to the libraries. 

Parent Nuclides by Reactions in JENDL-4.0
     Zr- 93 (Z= 40, A= 93), MT=103 (n,p)
     Zr- 94 (Z= 40, A= 94), MT= 28 (n,np)
     Zr- 94 (Z= 40, A= 94), MT=104 (n,d)
     Zr- 95 (Z= 40, A= 95), MT= 32 (n,nd)
     Zr- 95 (Z= 40, A= 95), MT=105 (n,t)
     Nb- 95 (Z= 41, A= 95), MT=106 (n,3He)

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)
    -----------------------------------------------------------
      Y- 93    U-235   Thermal   9.407240e-04   6.020630e-04 
      Y- 93    U-235   Fast      1.820250e-03   1.164960e-03 
      Y- 93    U-235   High      2.733290e-03   1.749310e-03 
      Y- 93    U-238   Fast      3.495780e-05   2.237310e-05 
      Y- 93    U-238   High      2.830790e-04   1.811700e-04 
      Y- 93   Pu-239   Thermal   1.508830e-03   9.656490e-04 
      Y- 93   Pu-239   Fast      1.328660e-03   8.503420e-04 
      Y- 93   Pu-239   High      3.139530e-03   2.009290e-03 
      Y- 93   Pu-241   Thermal   2.671310e-04   1.709640e-04 
      Y- 93   Pu-241   Fast      1.919460e-04   1.228460e-04 
    -----------------------------------------------------------
      Y- 93m   U-235   Thermal   1.443090e-04   9.235800e-05 
      Y- 93m   U-235   Fast      2.435260e-04   1.558570e-04 
      Y- 93m   U-235   High      2.280210e-04   1.459340e-04 
      Y- 93m   U-238   Fast      4.676900e-06   2.993220e-06 
      Y- 93m   U-238   High      2.361550e-05   1.511390e-05 
      Y- 93m  Pu-239   Thermal   2.314580e-04   1.481330e-04 
      Y- 93m  Pu-239   Fast      1.777570e-04   1.137650e-04 
      Y- 93m  Pu-239   High      2.619110e-04   1.676220e-04 
      Y- 93m  Pu-241   Thermal   4.097860e-05   2.622630e-05 
      Y- 93m  Pu-241   Fast      2.567990e-05   1.643510e-05 
    -----------------------------------------------------------
    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)
    -----------------------------------------------------------
      Y- 93    U-235   Thermal   6.339590e-02   6.446890e-04 
      Y- 93    U-235   Fast      6.239450e-02   1.034810e-03 
      Y- 93    U-235   High      5.199660e-02   3.388820e-03 
      Y- 93    U-238   Fast      4.918390e-02   9.836150e-04 
      Y- 93    U-238   High      4.538820e-02   1.272160e-03 
      Y- 93   Pu-239   Thermal   3.796100e-02   6.912050e-04 
      Y- 93   Pu-239   Fast      3.825210e-02   6.301340e-04 
      Y- 93   Pu-239   High      3.221800e-02   3.956670e-03 
      Y- 93   Pu-241   Thermal   2.980390e-02   4.278420e-04 
      Y- 93   Pu-241   Fast      2.981020e-02   6.875840e-03 
    -----------------------------------------------------------
      Y- 93m   U-235   Thermal   2.164160e-02   1.385050e-02 
      Y- 93m   U-235   Fast      2.105760e-02   1.347690e-02 
      Y- 93m   U-235   High      1.714520e-02   1.097300e-02 
      Y- 93m   U-238   Fast      1.695950e-02   1.085400e-02 
      Y- 93m   U-238   High      1.557670e-02   9.969090e-03 
      Y- 93m  Pu-239   Thermal   1.272760e-02   8.145630e-03 
      Y- 93m  Pu-239   Fast      1.285500e-02   8.227230e-03 
      Y- 93m  Pu-239   High      1.020360e-02   6.530330e-03 
      Y- 93m  Pu-241   Thermal   1.021700e-02   6.538880e-03 
      Y- 93m  Pu-241   Fast      1.023510e-02   6.550450e-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