48-Cd-111
Spin
Level energy(keV) Spin & Parity
----------------------------------------
ground state 1/2+
3.96220E+02 11/2-
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)
110.904182872 ± 0.000000605 (amu) [mass excess = -89253.079 ± 0.564 (keV) ]
Beta-decay energy (calculated as M(A,Z)-M(A,Z+1), taken from Ame2012)
-862.178 ± 3.509 (keV)
Strong Gamma-rays from Decay of Cd-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
----------------------------------------------------------
150.82 29.14 IT
245.40 94. IT
----------------------------------------------------------
*: 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
IT 48.54 M 5
Cross Sections (taken from JENDL-4.0)
Table of cross sections, Cd-111.
Figures of cross sections, Cd-111: 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
Cd-110 (Z= 48, A=110), MT=102 (n,γ)
Cd-111 (Z= 48, A=111), MT= 2 (Elastic scattering)
Cd-111 (Z= 48, A=111), MT= 4 (Inelastic scattering)
Cd-112 (Z= 48, A=112), MT= 16 (n,2n)
Cd-113 (Z= 48, A=113), MT= 17 (n,3n)
In-113 (Z= 49, A=113), MT= 32 (n,nd)
In-113 (Z= 49, A=113), MT=105 (n,t)
Sn-112 (Z= 50, A=112), MT=111 (n,2p)
Sn-114 (Z= 50, A=114), MT=107 (n,α)
Sn-115 (Z= 50, A=115), 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)
-----------------------------------------------------------
Cd-111 U-235 High 4.305170e-11 2.755310e-11
Cd-111 U-238 High 1.796440e-13 1.149720e-13
Cd-111 Pu-239 High 1.923620e-08 1.231120e-08
-----------------------------------------------------------
Cd-111m U-235 High 2.666730e-10 1.706710e-10
Cd-111m U-238 High 1.112760e-12 7.121690e-13
Cd-111m Pu-239 High 1.191540e-07 7.625830e-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)
-----------------------------------------------------------
Cd-111 U-235 Thermal 1.724440e-04 1.864130e-06
Cd-111 U-235 Fast 4.205870e-04 5.178790e-06
Cd-111 U-235 High 1.073940e-02 3.068340e-04
Cd-111 U-238 Fast 6.919560e-04 2.018860e-05
Cd-111 U-238 High 9.802020e-03 3.028240e-04
Cd-111 Pu-239 Thermal 2.957190e-03 2.698270e-06
Cd-111 Pu-239 Fast 3.566930e-03 3.188850e-06
Cd-111 Pu-239 High 1.546120e-02 9.284530e-04
Cd-111 Pu-241 Thermal 5.842510e-03 1.259940e-05
Cd-111 Pu-241 Fast 6.432370e-03 1.346550e-05
-----------------------------------------------------------
Cd-111m U-235 High 2.666730e-10 1.704180e-10
Cd-111m U-238 High 1.112760e-12 7.113970e-13
Cd-111m Pu-239 High 1.191540e-07 7.620890e-08
-----------------------------------------------------------
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