Bismuth (Z=83)
189Bi 190Bi 191Bi 192Bi 193Bi 194Bi 195Bi 197Bi 198Bi 199Bi 201Bi 202Bi 203Bi 204Bi 205Bi 206Bi 207Bi 208Bi 209Bi 210Bi 211Bi 212Bi 213Bi
Recommended† magnetic dipole moments
Isotope Energy [keV] t1/2 Spin/Parity μ [nm] Method Recommended Tables
209Bi 0 2.0x1019 y 9/2- +4.092(2) N INDC(NDS)-0915
2564 15 fs (9/2)+ 3.5(7) Mu-X INDC(NDS)-0816
2741 9.1 ps 15/2+ 6.2(12) Mu-X INDC(NDS)-0816
2986 18 ns 19/2+ 3.50(8) TDPAD INDC(NDS)-0816


Recommended† electric quadrupole moments
Isotope Energy [keV] t1/2 Spin/Parity Q [b] Method Recommended Tables
209Bi 0 2.0 1019 y 9/2- -0.516(15) AB INDC(NDS)-0833
2564 15 fs (9/2)+ +0.15(7) Mu-X INDC(NDS)-0833
2741 9.1 ps 15/2+ 0.0(5) 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
+4.1103(5) d R 1996BA94 10.1007/s004600050040
+4.1106(2) [2H] NMR 1953TI01
1951PR02		 10.1103/PhysRev.89.595
10.1103/PhysRev.81.20
-0.516(15) R 2001BI23 10.1103/PhysRevLett.87.133003
-0.37(3) a Mu-X 1972LE07 10.1016/0375-9474(72)90897-4
-0.55(1) AB 1983DE07 10.1007/BF01433607
209Bi 0 2.0×1019 y 9/2- +4.092(2) [1H] N 2018SK03 PhysRevLett.120.093001
-0.77(1) AB 1983DE07 10.1007/BF01433607
-0.40(5) R 1974HO40 10.1088/0031-8949/10/4/3
-0.39(3) O 1967DI04
1970GE10		 10.1139/p67-179
10.1364/JOSA.60.000869
-0.50(8) a Pi-X 1978BE24 10.1007/BF01408978
-0.5(2) a Pi-X 1981BA07 10.1016/0375-9474(81)90534-0
2563 14 fs (9/2)+ 3.5(7) Mu-X 1972LE07 10.1016/0375-9474(72)90897-4
1- +0.11(5) a Mu-X 1972LE07 10.1016/0375-9474(72)90897-4
2741 9.1 ps 15/2+ 6.2(12) Mu-X 1972LE07 10.1016/0375-9474(72)90897-4
0.0(4) a Mu-X 1972LE07 10.1016/0375-9474(72)90897-4
2986 18 ns 19/2+ 3.50(8) TDPAD 1978BE17 10.1103/PhysRevC.17.1359

† 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.