40-Zr-93
Spin
Level energy(keV) Spin & Parity
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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)
92.906469947 ± 0.000001952 (amu) [mass excess = -87122.683 ± 1.819 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
90.301 ± 1.549 (keV)
Strong Gamma-rays from Decay of Zr- 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
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30.77 -- B-
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*: 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- 1.61E+6 Y 10
Cross Sections (taken from JENDL-4.0)
Table of cross sections, Zr-93.
Figures of cross sections, Zr-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
Zr- 92 (Z= 40, A= 92), MT=102 (n,γ)
Zr- 93 (Z= 40, A= 93), MT= 2 (Elastic scattering)
Zr- 93 (Z= 40, A= 93), MT= 4 (Inelastic scattering)
Zr- 94 (Z= 40, A= 94), MT= 16 (n,2n)
Zr- 95 (Z= 40, A= 95), MT= 17 (n,3n)
Nb- 93 (Z= 41, A= 93), MT=103 (n,p)
Nb- 94 (Z= 41, A= 94), MT= 28 (n,np)
Nb- 94 (Z= 41, A= 94), MT=104 (n,d)
Nb- 95 (Z= 41, A= 95), MT= 32 (n,nd)
Nb- 95 (Z= 41, A= 95), MT=105 (n,t)
Mo- 95 (Z= 42, A= 95), MT=106 (n,3He)
Mo- 96 (Z= 42, A= 96), MT=107 (n,α)
Mo- 97 (Z= 42, A= 97), 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)
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Zr- 93 U-235 Thermal 1.367820e-06 8.754060e-07
Zr- 93 U-235 Fast 4.919850e-07 3.148700e-07
Zr- 93 U-235 High 3.848270e-05 2.462890e-05
Zr- 93 U-238 Fast 2.170810e-08 1.389320e-08
Zr- 93 U-238 High 8.799580e-07 5.631730e-07
Zr- 93 Pu-239 Thermal 1.685740e-05 1.078870e-05
Zr- 93 Pu-239 Fast 1.146810e-05 7.339610e-06
Zr- 93 Pu-239 High 1.030070e-04 6.592440e-05
Zr- 93 Pu-241 Thermal 6.981120e-07 4.467920e-07
Zr- 93 Pu-241 Fast 4.256800e-07 2.724350e-07
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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)
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Zr- 93 U-235 Thermal 6.339730e-02 4.490650e-04
Zr- 93 U-235 Fast 6.239500e-02 4.611580e-04
Zr- 93 U-235 High 5.203510e-02 3.117620e-03
Zr- 93 U-238 Fast 4.918390e-02 9.839790e-04
Zr- 93 U-238 High 4.538910e-02 1.271920e-03
Zr- 93 Pu-239 Thermal 3.797780e-02 2.658390e-04
Zr- 93 Pu-239 Fast 3.826360e-02 2.678870e-04
Zr- 93 Pu-239 High 3.232100e-02 3.551900e-03
Zr- 93 Pu-241 Thermal 2.980460e-02 4.176260e-04
Zr- 93 Pu-241 Fast 2.981070e-02 3.279100e-03
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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