41-Nb-93



Spin
     Level energy(keV)   Spin & Parity       
     ----------------------------------------
       ground state      9/2+                  
       3.07700E+01       1/2-                  
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)
     92.906373004 ± 0.000001958 (amu)  [mass excess = -87212.984 ± 1.824 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
     -406.665 ± 1.934 (keV) 
Strong Gamma-rays from Decay of Nb- 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 
  ----------------------------------------------------------
         30.77          6.E-04         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 
       IT           16.13 Y 14       
Cross Sections (taken from JENDL-4.0)
     Table of cross sections, Nb-93.
     Figures of cross sections, Nb-93:  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
     Nb- 93 (Z= 41, A= 93), MT=  2 (Elastic scattering)
     Nb- 93 (Z= 41, A= 93), MT=  4 (Inelastic scattering)
     Nb- 94 (Z= 41, A= 94), MT= 16 (n,2n)
     Nb- 95 (Z= 41, A= 95), MT= 17 (n,3n)
     Mo- 94 (Z= 42, A= 94), MT= 28 (n,np)
     Mo- 94 (Z= 42, A= 94), MT=104 (n,d)
     Mo- 95 (Z= 42, A= 95), MT= 32 (n,nd)
     Mo- 95 (Z= 42, A= 95), MT=105 (n,t)

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)
    -----------------------------------------------------------
     Nb- 93    U-235   Thermal   3.623050e-11   2.318760e-11 
     Nb- 93    U-235   Fast      1.031210e-11   6.599770e-12 
     Nb- 93    U-235   High      4.505670e-08   2.883630e-08 
     Nb- 93    U-238   Fast      3.399990e-13   2.175990e-13 
     Nb- 93    U-238   High      1.597480e-10   1.022380e-10 
     Nb- 93   Pu-239   Thermal   4.229040e-09   2.706590e-09 
     Nb- 93   Pu-239   Fast      2.345030e-09   1.500810e-09 
     Nb- 93   Pu-239   High      3.324160e-07   2.127460e-07 
     Nb- 93   Pu-241   Thermal   3.178680e-11   2.034360e-11 
     Nb- 93   Pu-241   Fast      1.763350e-11   1.128540e-11 
    -----------------------------------------------------------
     Nb- 93m   U-235   Thermal   8.388360e-12   5.368550e-12 
     Nb- 93m   U-235   Fast      2.082260e-12   1.332650e-12 
     Nb- 93m   U-235   High      5.682830e-09   3.637010e-09 
     Nb- 93m   U-238   Fast      6.865350e-14   4.393830e-14 
     Nb- 93m   U-238   High      2.014840e-11   1.289500e-11 
     Nb- 93m  Pu-239   Thermal   9.791380e-10   6.266480e-10 
     Nb- 93m  Pu-239   Fast      4.735160e-10   3.030500e-10 
     Nb- 93m  Pu-239   High      4.192640e-08   2.683290e-08 
     Nb- 93m  Pu-241   Thermal   7.359510e-12   4.710090e-12 
     Nb- 93m  Pu-241   Fast      3.560600e-12   2.278790e-12 
    -----------------------------------------------------------
    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)
    -----------------------------------------------------------
     Nb- 93    U-235   Thermal   6.339730e-02   4.490650e-04 
     Nb- 93    U-235   Fast      6.239500e-02   4.611580e-04 
     Nb- 93    U-235   High      5.203520e-02   3.117620e-03 
     Nb- 93    U-238   Fast      4.918390e-02   9.839790e-04 
     Nb- 93    U-238   High      4.538910e-02   1.271920e-03 
     Nb- 93   Pu-239   Thermal   3.797780e-02   2.658390e-04 
     Nb- 93   Pu-239   Fast      3.826360e-02   2.678870e-04 
     Nb- 93   Pu-239   High      3.232140e-02   3.551940e-03 
     Nb- 93   Pu-241   Thermal   2.980460e-02   4.176260e-04 
     Nb- 93   Pu-241   Fast      2.981070e-02   5.962000e-04 
    -----------------------------------------------------------
     Nb- 93m   U-235   Thermal   6.022740e-02   4.266190e-04 
     Nb- 93m   U-235   Fast      5.927530e-02   4.380990e-04 
     Nb- 93m   U-235   High      4.943340e-02   2.961740e-03 
     Nb- 93m   U-238   Fast      4.672470e-02   9.347820e-04 
     Nb- 93m   U-238   High      4.311960e-02   1.208320e-03 
     Nb- 93m  Pu-239   Thermal   3.607890e-02   2.525480e-04 
     Nb- 93m  Pu-239   Fast      3.635040e-02   2.544940e-04 
     Nb- 93m  Pu-239   High      3.070500e-02   3.374300e-03 
     Nb- 93m  Pu-241   Thermal   2.831440e-02   3.967430e-04 
     Nb- 93m  Pu-241   Fast      2.832010e-02   1.132780e-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