49-In-111
Spin
Level energy(keV) Spin & Parity
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ground state 9/2+
5.37000E+02 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)
110.905108458 ± 0.000003768 (amu) [mass excess = -88390.901 ± 3.510 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
-2451.383 ± 6.389 (keV)
Strong Gamma-rays from Decay of In-111 (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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150.81 ~ 3.E-03 EC
171.28 90.65 EC
245.35 94.09 EC
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537. 87.2 IT
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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
EC 2.8047 D 4
IT 7.7 M 2
Evaluated Data Libraries
Links to the libraries.
Parent Nuclides by Reactions in JENDL-4.0
In-113 (Z= 49, A=113), MT= 17 (n,3n)
Sn-112 (Z= 50, A=112), MT= 28 (n,np)
Sn-112 (Z= 50, A=112), MT=104 (n,d)
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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In-111 U-235 High 1.058100e-14 6.771840e-15
In-111 Pu-239 High 4.126760e-11 2.641130e-11
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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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In-111 U-235 High 1.058100e-14 6.771840e-15
In-111 Pu-239 High 4.126760e-11 2.641130e-11
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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