65-Tb-160
Spin
Level energy(keV) Spin & Parity
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ground state 3-
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)
159.927175556 ± 0.000001884 (amu) [mass excess = -67835.532 ± 1.756 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
1835.891 ± 1.264 (keV)
Strong Gamma-rays from Decay of Tb-160 (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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298.58 26.13 B-
879.38 30.1 B-
966.17 25.1 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- 72.3 D 2
Cross Sections (taken from JENDL-4.0)
Table of cross sections, Tb-160.
Figures of cross sections, Tb-160: 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
Tb-159 (Z= 65, A=159), MT=102 (n,γ)
Tb-160 (Z= 65, A=160), MT= 2 (Elastic scattering)
Tb-160 (Z= 65, A=160), MT= 4 (Inelastic scattering)
Dy-160 (Z= 66, A=160), MT=103 (n,p)
Dy-161 (Z= 66, A=161), MT= 28 (n,np)
Dy-161 (Z= 66, A=161), MT=104 (n,d)
Dy-162 (Z= 66, A=162), MT= 32 (n,nd)
Dy-162 (Z= 66, A=162), MT=105 (n,t)
Dy-163 (Z= 66, A=163), MT= 33 (n,nt)
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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Tb-160 U-235 Thermal 2.835490e-10 1.814710e-10
Tb-160 U-235 Fast 1.117690e-10 7.153230e-11
Tb-160 U-235 High 2.112900e-07 1.352260e-07
Tb-160 U-238 Fast 1.890700e-11 1.210050e-11
Tb-160 U-238 High 2.112300e-07 1.351880e-07
Tb-160 Pu-239 Thermal 6.279010e-08 4.018570e-08
Tb-160 Pu-239 Fast 1.809710e-07 1.158210e-07
Tb-160 Pu-239 High 2.172410e-05 1.390340e-05
Tb-160 Pu-241 Thermal 1.250200e-09 8.001290e-10
Tb-160 Pu-241 Fast 1.368970e-08 8.761410e-09
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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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Tb-160 U-235 Thermal 2.835490e-10 1.814710e-10
Tb-160 U-235 Fast 1.117690e-10 7.153230e-11
Tb-160 U-235 High 2.112900e-07 1.350250e-07
Tb-160 U-238 Fast 1.890700e-11 1.209610e-11
Tb-160 U-238 High 2.112300e-07 1.350410e-07
Tb-160 Pu-239 Thermal 6.279010e-08 4.018570e-08
Tb-160 Pu-239 Fast 1.809710e-07 1.158210e-07
Tb-160 Pu-239 High 2.172410e-05 1.389440e-05
Tb-160 Pu-241 Thermal 1.250200e-09 7.999990e-10
Tb-160 Pu-241 Fast 1.368970e-08 8.761410e-09
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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