58-Ce-141
Spin
Level energy(keV) Spin & Parity
----------------------------------------
ground state 7/2-
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)
140.908280674 ± 0.000002340 (amu) [mass excess = -85436.002 ± 2.180 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
580.420 ± 1.053 (keV)
Strong Gamma-rays from Decay of Ce-141 (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
----------------------------------------------------------
145.44 48.29 B-
----------------------------------------------------------
*: 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- 32.508 D 1
Cross Sections (taken from JENDL-4.0)
Table of cross sections, Ce-141.
Figures of cross sections, Ce-141: 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
Ce-140 (Z= 58, A=140), MT=102 (n,γ)
Ce-141 (Z= 58, A=141), MT= 2 (Elastic scattering)
Ce-141 (Z= 58, A=141), MT= 4 (Inelastic scattering)
Ce-142 (Z= 58, A=142), MT= 16 (n,2n)
Ce-143 (Z= 58, A=143), MT= 17 (n,3n)
Pr-141 (Z= 59, A=141), MT=103 (n,p)
Pr-143 (Z= 59, A=143), MT= 32 (n,nd)
Pr-143 (Z= 59, A=143), MT=105 (n,t)
Nd-143 (Z= 60, A=143), MT=106 (n,3He)
Nd-144 (Z= 60, A=144), MT=107 (n,α)
Nd-145 (Z= 60, A=145), MT= 22 (n,nα)
Nd-146 (Z= 60, A=146), MT= 24 (n,2nα)
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)
-----------------------------------------------------------
Ce-141 U-235 Thermal 4.982070e-08 3.188520e-08
Ce-141 U-235 Fast 3.213360e-07 1.028280e-07
Ce-141 U-235 High 1.743390e-05 1.115770e-05
Ce-141 U-238 Fast 9.053380e-10 5.794160e-10
Ce-141 U-238 High 1.101190e-07 7.047670e-08
Ce-141 Pu-239 Thermal 2.289640e-06 1.465370e-06
Ce-141 Pu-239 Fast 2.459600e-06 1.574140e-06
Ce-141 Pu-239 High 1.314750e-04 8.414420e-05
Ce-141 Pu-241 Thermal 2.290370e-08 1.465840e-08
Ce-141 Pu-241 Fast 3.687230e-08 2.359830e-08
-----------------------------------------------------------
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)
-----------------------------------------------------------
Ce-141 U-235 Thermal 5.838400e-02 5.909730e-04
Ce-141 U-235 Fast 5.937240e-02 1.669940e-03
Ce-141 U-235 High 4.492480e-02 2.692210e-03
Ce-141 U-238 Fast 5.337390e-02 1.494250e-03
Ce-141 U-238 High 4.386260e-02 8.775730e-04
Ce-141 Pu-239 Thermal 5.246490e-02 1.049390e-03
Ce-141 Pu-239 Fast 5.146670e-02 1.441190e-03
Ce-141 Pu-239 High 3.562640e-02 2.136240e-03
Ce-141 Pu-241 Thermal 4.906770e-02 6.868810e-04
Ce-141 Pu-241 Fast 5.071770e-02 4.060420e-03
-----------------------------------------------------------
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