45-Rh-106
Spin
Level energy(keV) Spin & Parity
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ground state 1+
1.37000E+02 (6)+
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)
105.907286801 ± 0.000005792 (amu) [mass excess = -86361.788 ± 5.395 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
3545.616 ± 5.339 (keV)
Strong Gamma-rays from Decay of Rh-106 (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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511.7 85.5 B-
717.2 28.9 B-
1046.7 30.35 B-
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511.86 20.4 B-
621.93 9.93 B-
1050.41 1.56 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- 30.07 S 35
B- 131 M 2
Evaluated Data Libraries
Links to the libraries.
Parent Nuclides by Reactions in JENDL-4.0
Rh-105 (Z= 45, A=105), MT=102 (n,γ)
Pd-106 (Z= 46, A=106), MT=103 (n,p)
Pd-107 (Z= 46, A=107), MT= 28 (n,np)
Pd-107 (Z= 46, A=107), MT=104 (n,d)
Pd-108 (Z= 46, A=108), MT=105 (n,t)
Ag-107 (Z= 47, A=107), MT=111 (n,2p)
Ag-109 (Z= 47, A=109), MT=107 (n,α)
Ag-110 (Z= 47, A=110), 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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Rh-106 U-235 High 5.256220e-07 3.363970e-07
Rh-106 U-238 High 3.138340e-08 2.008530e-08
Rh-106 Pu-239 Thermal 1.327350e-06 8.495030e-07
Rh-106 Pu-239 Fast 5.905760e-06 3.779690e-06
Rh-106 Pu-239 High 7.339240e-05 4.697100e-05
Rh-106 Pu-241 Thermal 2.966560e-07 1.898600e-07
Rh-106 Pu-241 Fast 4.906070e-07 3.139890e-07
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Rh-106m U-235 High 2.378370e-06 1.522150e-06
Rh-106m U-238 High 1.420050e-07 9.088340e-08
Rh-106m Pu-239 Thermal 3.111950e-06 1.991640e-06
Rh-106m Pu-239 Fast 1.613070e-05 1.032360e-05
Rh-106m Pu-239 High 3.320910e-04 2.125370e-04
Rh-106m Pu-241 Thermal 6.955050e-07 4.451230e-07
Rh-106m Pu-241 Fast 1.340020e-06 8.576100e-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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Rh-106 U-235 Thermal 4.008720e-03 6.758140e-06
Rh-106 U-235 Fast 5.314650e-03 9.294600e-06
Rh-106 U-235 High 1.613030e-02 9.663060e-04
Rh-106 U-238 Fast 2.493380e-02 3.635140e-05
Rh-106 U-238 High 2.463610e-02 6.931690e-04
Rh-106 Pu-239 Thermal 4.349490e-02 8.699760e-04
Rh-106 Pu-239 Fast 4.362700e-02 6.110340e-04
Rh-106 Pu-239 High 3.545980e-02 2.835200e-03
Rh-106 Pu-241 Thermal 6.104480e-02 1.220800e-03
Rh-106 Pu-241 Fast 6.238480e-02 8.760300e-04
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Rh-106m U-235 High 2.378370e-06 1.519900e-06
Rh-106m U-238 High 1.420050e-07 9.078500e-08
Rh-106m Pu-239 Thermal 3.111950e-06 1.991640e-06
Rh-106m Pu-239 Fast 1.613070e-05 1.032360e-05
Rh-106m Pu-239 High 3.320910e-04 2.124000e-04
Rh-106m Pu-241 Thermal 6.955050e-07 4.450510e-07
Rh-106m Pu-241 Fast 1.340020e-06 8.576100e-07
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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