Gadolinium (Z=64)
144Gd 145Gd 146Gd 147Gd 148Gd 149Gd 151Gd 152Gd 153Gd 154Gd 155Gd 156Gd 157Gd 158Gd 159Gd 160Gd

Recommended magnetic dipole moments
Isotope Energy [keV] t1/2 Spin/Parity μ [nm] Method Recommended Tables
156Gd 89 2.21 ns 2+ +0.774(8) ME INDC(NDS)-0816
288 112 ps 4+ +1.55(14) TF INDC(NDS)-0816
585 15.8 ps 6+ +2.2(4) TF INDC(NDS)-0816
965 4.3 ps 8+ +2.7(4) TF INDC(NDS)-0816
1511 189 ps 4+ +3.24(11) IPAC INDC(NDS)-0816


Recommended electric quadrupole moments
Isotope Energy [keV] t1/2 Spin/Parity Q [b] Method Recommended Tables
156Gd 89 2.21 ns 2+ -1.93(4) Mu-X 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
156Gd 89. 2.21 ns 2+ +0.82(14) [158Gd 261] TF 1991ST01 10.1007/BF01284786
+0.774(8) [155Gd] ME 1974AR23 10.1016/0375-9474(74)90464-3
-1.93(4) a Mu-X 1983LA08
2013STZZ
10.1103/PhysRevC.27.1772
-1.96(4) [155Gd] ME 1974AR23 10.1016/0375-9474(74)90464-3
288. 112 ps 4+ +1.68(12) [156Gd 89.] TF 1992BR07 10.1103/PhysRevC.45.1549
+1.76(16) [156Gd 89.] TF 1990BA39 10.1007/BF02401205
+1.31(8) [Bhf Gd(Fe)] IPAC 1990SC10 10.1007/BF01290185
+1.63(15) [158Gd 261] TF 1991ST01 10.1007/BF01284786
+1.55(14) [156Gd 89.] TF 1991ST01 10.1007/BF01284786
+1.24(8) IPAC 1988AL33 10.1007/BF01355597
585. 16 ps 6+ +2.4(2) [156Gd 89.] TF 1992BR07 10.1103/PhysRevC.45.1549
+2.3(4) [158Gd 261] TF 1991ST01 10.1007/BF01284786
+2.2(4) [156Gd 89.] TF 1991ST01 10.1007/BF01284786
+1.5(13) IPAC 1988AL33 10.1007/BF01355597
965. 4.3 ps 8+ +2.7(3) [156Gd 89.] TF 1992BR07 10.1103/PhysRevC.45.1549
1511. 190 ps 4+ +3.24(11) IPAC 1988AL33 10.1007/BF01355597
gs band <10+ g(10+)/g(2+) =0.89(12) TF 1983HA24 10.1016/0375-9474(83)90466-9
α×10-3=-1.1(12)

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.