90-Th-228
Spin
Level energy(keV) Spin & Parity
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ground state 0+
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)
228.028741272 ± 0.000002315 (amu) [mass excess = 26772.323 ± 2.156 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
-2152.124 ± 4.378 (keV)
Strong Gamma-rays from Decay of Th-228 (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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84.37 1.22 Alpha
131.61 0.13 Alpha
215.98 0.25 Alpha
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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
A 1.912 Y 2
Cross Sections (taken from JENDL-4.0)
Table of cross sections, Th-228.
Figures of cross sections, Th-228: 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
Th-227 (Z= 90, A=227), MT=102 (n,γ)
Th-228 (Z= 90, A=228), MT= 2 (Elastic scattering)
Th-228 (Z= 90, A=228), MT= 4 (Inelastic scattering)
Th-229 (Z= 90, A=229), MT= 16 (n,2n)
Th-230 (Z= 90, A=230), MT= 17 (n,3n)
Th-231 (Z= 90, A=231), MT= 37 (n,4n)