Cadmium (Z=48)
100Cd 102Cd 103Cd 105Cd 106Cd 107Cd 108Cd 109Cd 110Cd 111Cd 112Cd 113Cd 114Cd 115Cd 116Cd 117Cd 119Cd 121Cd 123Cd 125Cd 127Cd 129Cd
Recommended† magnetic dipole moments
Isotope Energy [keV] t1/2 Spin/Parity μ [nm] Method Recommended Tables
111Cd 0 stable 1/2+ -0.5940(3) OP/RD INDC(NDS)-0794
245 84 ns 5/2+ -0.766(3) TDPAC INDC(NDS)-0816
342 24 ps 3/2+ +0.9(6) TF INDC(NDS)-0816
396 48.5 m 11/2- -1.1036(5) INDC(NDS)-0794
620 9.7 ps 5/2+ +0.48(13) TF INDC(NDS)-0816


Recommended† electric quadrupole moments
Isotope Energy [keV] t1/2 Spin/Parity Q [b] Method Recommended Tables
111Cd 245 84 ns 5/2+ +0.64(3) TDPAC INDC(NDS)-0833
396 48.5 m 11/2- -0.75(3) CLS INDC(NDS)-0833


Compiled‡ magnetic dipole and electric quadrupole moments from published articles
Isotope Energy [keV] t1/2 Spin/Parity μ [nm] Q [b] Ref. Std Method NSR keyword doi
111Cd 0. stable 1/2+ -0.5948861(8) [1H] OP/RD , 1972SP09
1950PR51		 10.1016/0375-9601(72)90418-5
10.1103/PhysRev.79.35
0.595543(2) [2H] NMR 1974KA04 10.1016/0375-9601(74)90101-7
245. 84 ns 5/2+ -0.766(3) TDPAC 1974BE51 10.1007/BF01680410
(+)0.74(8) [109Cd 463.] TDPAD 1978SP09 10.1007/BF01021832
+0.77(12) st [117In 660.] TDPAC 1973RA02
1976RA09		 10.1103/PhysRevLett.30.10
10.1103/PhysRevB.13.2835
+0.80(10) [115Cd 173.] TDPAD 1983ER01 10.1016/0375-9601(83)90118-4
+0.83(13) [111Cd 396.] TDPAD 1980HE02 10.1007/BF01473117
342. 27 ps 3/2+ 0.0(12) [110Cd 658.] TF 1988BE45 10.1007/BF02398325
396. 48.6 m 11/2- -1.1052(3) [115Cd] CLS 2013YO02 10.1103/PhysRevLett.110.192501
-1.1051(4) [109Cd] OD 1969LA06 10.1103/PhysRev.177.1615
-0.75(3) [calc efg] CLS 2013YO02
2013STZZ		 10.1103/PhysRevLett.110.192501
-0.85(9) [109Cd] OD 1969LA06 10.1103/PhysRev.177.1615
620. 10 ps 5/2+ +0.28(12) [110Cd 658.] TF 1988BE45 10.1007/BF02398325

† Recommended magnetic moments are for the bare nucleus with published results corrected consistently for diamagnetism (including error estimate).
  Where appropriate published results are also adjusted to the most recent adopted half-life for the state.
  Recommended quadrupole moments are adjusted using the best electric field gradient calculation for the system concerned.
  For details see the Reports referenced.

‡ In this listing published results are given without adjustment or correction.