39-Y-91



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      1/2-                  
       5.55570E+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)
     90.907297442 ± 0.000002761 (amu)  [mass excess = -86351.877 ± 2.572 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     1544.281 ± 1.841 (keV) 
Strong Gamma-rays from Decay of Y- 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 
  ----------------------------------------------------------
       1204.77            0.26         B- 
  ----------------------------------------------------------
        555.57           95.           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-           58.51 D 6        
       IT           49.71 M 4        
Cross Sections (taken from JENDL-4.0)
     Table of cross sections, Y-91.
     Figures of cross sections, Y-91:  type-1:  type-2:  type-3.
       type-1: total, elastic and inelastic scattering, capture and fision cross sections
       type-2: same as type-1 but cross sections are averaged in 70 energy group intervals
       type-3: threshold reaction cross sections
Evaluated Data Libraries
     Links to the libraries. 

Parent Nuclides by Reactions in JENDL-4.0
     Y - 90 (Z= 39, A= 90), MT=102 (n,γ)
     Y - 91 (Z= 39, A= 91), MT=  2 (Elastic scattering)
     Y - 91 (Z= 39, A= 91), MT=  4 (Inelastic scattering)
     Zr- 91 (Z= 40, A= 91), MT=103 (n,p)
     Zr- 92 (Z= 40, A= 92), MT= 28 (n,np)
     Zr- 92 (Z= 40, A= 92), MT=104 (n,d)
     Zr- 93 (Z= 40, A= 93), MT= 32 (n,nd)
     Zr- 93 (Z= 40, A= 93), MT=105 (n,t)
     Nb- 94 (Z= 41, A= 94), MT=107 (n,α)
     Nb- 95 (Z= 41, 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)
    -----------------------------------------------------------
      Y- 91    U-235   Thermal   6.194120e-07   3.964260e-07 
      Y- 91    U-235   Fast      2.883650e-07   1.845530e-07 
      Y- 91    U-235   High      1.017460e-05   6.511730e-06 
      Y- 91    U-238   Fast      1.492400e-08   9.551340e-09 
      Y- 91    U-238   High      3.475790e-07   2.224500e-07 
      Y- 91   Pu-239   Thermal   4.661650e-06   2.983470e-06 
      Y- 91   Pu-239   Fast      3.307390e-06   2.116730e-06 
      Y- 91   Pu-239   High      1.686920e-05   1.079630e-05 
      Y- 91   Pu-241   Thermal   3.422150e-07   2.190180e-07 
      Y- 91   Pu-241   Fast      1.695520e-07   1.085140e-07 
    -----------------------------------------------------------
      Y- 91m   U-235   Thermal   2.675330e-06   1.712230e-06 
      Y- 91m   U-235   Fast      1.428090e-06   9.139780e-07 
      Y- 91m   U-235   High      8.067000e-05   5.162870e-05 
      Y- 91m   U-238   Fast      7.390920e-08   4.730190e-08 
      Y- 91m   U-238   High      2.755810e-06   1.763710e-06 
      Y- 91m  Pu-239   Thermal   2.013440e-05   1.288600e-05 
      Y- 91m  Pu-239   Fast      1.637940e-05   1.048280e-05 
      Y- 91m  Pu-239   High      1.337490e-04   8.559900e-05 
      Y- 91m  Pu-241   Thermal   1.478080e-06   9.459710e-07 
      Y- 91m  Pu-241   Fast      8.396890e-07   5.374010e-07 
    -----------------------------------------------------------
    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- 91    U-235   Thermal   5.815650e-02   4.254350e-04 
      Y- 91    U-235   Fast      5.719140e-02   8.151830e-04 
      Y- 91    U-235   High      4.826340e-02   1.929000e-03 
      Y- 91    U-238   Fast      4.014450e-02   8.458160e-04 
      Y- 91    U-238   High      3.856620e-02   7.810950e-04 
      Y- 91   Pu-239   Thermal   2.485830e-02   3.480000e-04 
      Y- 91   Pu-239   Fast      2.515540e-02   5.031760e-04 
      Y- 91   Pu-239   High      2.237470e-02   2.455280e-03 
      Y- 91   Pu-241   Thermal   1.862980e-02   3.729750e-04 
      Y- 91   Pu-241   Fast      1.925050e-02   7.724260e-04 
    -----------------------------------------------------------
      Y- 91m   U-235   Thermal   5.175910e-02   2.811490e-02 
      Y- 91m   U-235   Fast      5.090020e-02   2.764660e-02 
      Y- 91m   U-235   High      4.295430e-02   2.334010e-02 
      Y- 91m   U-238   Fast      3.572860e-02   1.939370e-02 
      Y- 91m   U-238   High      3.432390e-02   1.864190e-02 
      Y- 91m  Pu-239   Thermal   2.212200e-02   1.201940e-02 
      Y- 91m  Pu-239   Fast      2.238720e-02   1.216340e-02 
      Y- 91m  Pu-239   High      1.991310e-02   1.081410e-02 
      Y- 91m  Pu-241   Thermal   1.658040e-02   9.008630e-03 
      Y- 91m  Pu-241   Fast      1.713290e-02   9.306660e-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