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Bismuth (83Bi) has 41 known isotopes, ranging from 184Bi to 224Bi. Bismuth has no stable isotopes, but does have one very long-lived isotope; thus, the standard atomic weight can be given as 208.98040(1). Although bismuth-209 is now known to be radioactive, it has classically been considered to be a stable isotope because it has a half-life of approximately 2.01×1019 years, which is more than a billion times the age of the universe. Besides 209Bi, the most stable bismuth radioisotopes are 210mBi with a half-life of 3.04 million years, 208Bi with a half-life of 368,000 years and 207Bi, with a half-life of 32.9 years, none of which occurs in nature. All other isotopes have half-lives under 1 year, most under a day. Of naturally occurring radioisotopes, the most stable is radiogenic 210Bi with a half-life of 5.012 days. 210mBi is unusual for being a nuclear isomer with a half-life multiple orders of magnitude longer than that of the ground state.

Quick Facts Main isotopes, Decay ...
Isotopes of bismuth (83Bi)
Main isotopes[1] Decay
abun­dance half-life (t1/2) mode pro­duct
207Bi synth 31.55 y β+ 207Pb
208Bi synth 3.68×105 y β+ 208Pb
209Bi 100% 2.01×1019 y α 205Tl
210Bi trace 5.012 d β 210Po
α 206Tl
210mBi synth 3.04×106 y α 206Tl
Standard atomic weight Ar°(Bi)
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List of isotopes


More information Nuclide, Historic name ...
Nuclide
[n 1]
Historic
name
Z N Isotopic mass (Da)[4]
[n 2][n 3]
Half-life[1]
[n 4]
Decay
mode
[1]
[n 5]
Daughter
isotope

[n 6]
Spin and
parity[1]
[n 7][n 8]
Isotopic
abundance
Excitation energy[n 8]
184Bi[5] 83 101 184.00135(13)# 6.6(15) ms α 180Tl 3+#
184mBi[n 9] 150(100)# keV 13(2) ms α 180Tl 10−#
185Bi[6] 83 102 184.99760(9)# 2.8+2.3
−1.0
 μs
p (92%) 184Pb (1/2+)
α (8%) 181Tl
185mBi 70(50)# keV 58(2) μs IT 185Bi (7/2−, 9/2−)
186Bi 83 103 185.996623(18) 14.8(7) ms α (99.99%) 182Tl (3+)
β+ (?%) 186Pb
β+, SF (0.011%) (various)
186mBi[n 9] 170(100)# keV 9.8(4) ms α (99.99%) 182Tl (10−)
β+ (?%) 186Pb
β+, SF (0.011%) (various)
187Bi 83 104 186.993147(11) 37(2) ms α 183Tl (9/2−)
187m1Bi 108(8) keV 370(20) μs α 183Tl 1/2+
187m2Bi 252(3) keV 7(5) μs IT 187Bi (13/2+)
188Bi 83 105 187.992276(12) 60(3) ms α 184Tl (3+)
β+, SF (0.0014%) (various)
188m1Bi 66(30) keV >5 μs 7+#
188m2Bi 153(30) keV 265(15) ms α 184Tl (10−)
β+, SF (0.0046%) (various)
189Bi 83 106 188.989195(22) 688(5) ms α 185Tl 9/2−
189m1Bi 184(5) keV 5.0(1) ms α (83%) 185Tl 1/2+
IT (17%) 189Bi
189m2Bi 357.6(5) keV 880(50) ns IT 189Bi 13/2+
190Bi 83 107 189.988625(23) 6.3(1) s α (77%) 186Tl (3+)
β+ (23%) 190Pb
β+, SF (6×10-6%) (various)
190m1Bi 120(40) keV 6.2(1) s α (70%) 186Tl 10−
β+ (30%) 190Pb
β+, SF (4×10-6%) (various)
190m2Bi 121(15) keV 175(8) ns IT 190Bi (5−)
190m3Bi 394(40) keV 1.3(8) μs IT 190Bi (8−)
191Bi 83 108 190.985787(8) 12.4(3) s α (51%) 187Tl 9/2−
β+ (49%) 191Pb
191m1Bi 242(4) keV 125(8) ms α (68%) 187Tl 1/2+
IT (?%) 191Bi
β+ (?%) 191Pb
191m2Bi 429.7(5) keV 562(10) ns IT 191Bi 13/2+
191m3Bi 1875(25)# keV 400(40) ns IT 191Bi 25/2-#
192Bi 83 109 191.98547(3) 34.6(9) s β+ (88%) 192Pb (3+)
α (12%) 188Tl
192mBi 140(30) keV 39.6(4) s β+ (90%) 192Pb 10−
α (10%) 188Tl
193Bi 83 110 192.982947(8) 63.6(30) s β+ (96.5%) 193Pb 9/2−
α (3.5%) 189Tl
193m1Bi 305(6) keV 3.20(14) s α (84%) 189Tl 1/2+
β+ (16%) 193Pb
193m2Bi 605.53(18) keV 153(10) ns IT 193Bi 13/2+
193m3Bi 2349.6(6) keV 85(3) μs IT 193Bi 29/2+
193m4Bi 2405.1(7) keV 3.02(8) μs IT 193Bi (29/2−)
194Bi 83 111 193.982799(6) 95(3) s β+ (99.54%) 194Pb 3+
α (0.46%) 190Tl
194m1Bi 150(50) keV 125(2) s β+ 194Pb (6+, 7+)
194m2Bi 163(4) keV 115(4) s β+ (99.80%) 194Pb (10−)
α (0.20%) 190Tl
195Bi 83 112 194.980649(6) 183(4) s β+ (99.97%) 195Pb 9/2−
α (0.030%) 191Tl
195m1Bi 399(6) keV 87(1) s β+ (67%) 195Pb 1/2+
α (33%) 191Tl
195m2Bi 2381.0(5) keV 614(5) ns IT 195Bi (29/2−)
195m3Bi 2615.9(5) keV 1.49(1) μs IT 195Bi 29/2+
196Bi 83 113 195.980667(26) 5.13(20) min β+ 196Pb (3+)
α (0.00115%) 192Tl
196m1Bi 166.4(29) keV 0.6(5) s IT 196Bi (7+)
196m2Bi 272(3) keV 4.00(5) min β+ (74.2%) 196Pb (10−)
IT (25.8%) 196Bi
α (3.8×10−4%) 196Bi
197Bi 83 114 196.978865(9) 9.33(50) min β+ 197Pb 9/2−
197m1Bi 533(12) keV 5.04(16) min α (55%) 193Tl 1/2+
β+ (45%) 197Pb
197m2Bi 2403(12) keV 263(13) ns IT 197Bi (29/2−)
197m3Bi 2929.5(5) keV 209(30) ns IT 197Bi (31/2−)
198Bi 83 115 197.979201(30) 10.3(3) min β+ 198Pb 3+
198m1Bi 290(40) keV 11.6(3) min β+ 198Pb 7+
198m2Bi 540(40) keV 7.7(5) s IT 198Bi 10−
199Bi 83 116 198.977673(11) 27(1) min β+ 199Pb 9/2−
199m1Bi 667(3) keV 24.70(15) min β+ (>98%) 199Pb (1/2+)
IT (<2%) 199Bi
α (0.01%) 195Tl
199m2Bi 1962(23) keV 0.10(3) μs IT 199Bi 25/2+#
199m3Bi 2548(23) keV 168(13) ns IT 199Bi 29/2−#
200Bi 83 117 199.978131(24) 36.4(5) min β+ 200Pb 7+
200m1Bi[n 9] 100(70)# keV 31(2) min β+ (?%) 200Pb (2+)
IT (?%) 200Bi
200m2Bi 428.20(10) keV 400(50) ms IT 200Bi (10−)
201Bi 83 118 200.976995(13) 103(3) min β+ 201Pb 9/2−
201m1Bi 846.35(18) keV 57.5(21) min β+ 201Pb 1/2+
α (?%) 197Tl
201m2Bi 1973(23) keV 118(28) ns IT 201Bi 25/2+#
201m3Bi 2012(23) keV 105(75) ns IT 201Bi 27/2+#
201m4Bi 2781(23) keV 124(4) ns IT 201Bi 29/2−#
202Bi 83 119 201.977723(15) 1.72(5) h β+ 202Pb 5+
α (<10−5%) 198Tl
202m1Bi 625(12) keV 3.04(6) μs IT 202Bi 10−#
202m2Bi 2617(12) keV 310(50) ns IT 202Bi (17+)
203Bi 83 120 202.976892(14) 11.76(5) h β+ 203Pb 9/2−
203m1Bi 1098.21(9) keV 305(5) ms IT 203Bi 1/2+
203m2Bi 2041.5(6) keV 194(30) ns IT 203Bi 25/2+
204Bi 83 121 203.977836(10) 11.22(10) h β+ 204Pb 6+
204m1Bi 805.5(3) keV 13.0(1) ms IT 204Bi 10−
204m2Bi 2833.4(11) keV 1.07(3) ms IT 204Bi 17+
205Bi 83 122 204.977385(5) 14.91(7) d β+ 205Pb 9/2−
205m1Bi 1497.17(9) keV 7.9(7) μs IT 205Bi 1/2+
205m2Bi 2064.7(4) keV 100(6) ns IT 205Bi 21/2+
205m3Bi 2139.0(7) keV 220(25) ns IT 205Bi 25/2+
206Bi 83 123 205.978499(8) 6.243(3) d β+ 206Pb 6+
206m1Bi 59.897(17) keV 7.7(2) μs IT 206Bi 4+
206m2Bi 1044.8(7) keV 890(10) μs IT 206Bi 10−
206m3Bi 9233.3(8) keV 155(15) ns IT 206Bi (28−)
206m4Bi 10170.5(8) keV >2 μs IT 206Bi (31+)
207Bi 83 124 206.9784706(26) 31.22(17) y β+ 207Pb 9/2−
207mBi 2101.61(16) keV 182(6) μs IT 207Bi 21/2+
208Bi 83 125 207.9797421(25) 3.68(4)×105 y β+ 208Pb 5+
208mBi 1571.1(4) keV 2.58(4) ms IT 208Bi 10−
209Bi
[n 10][n 11]
83 126 208.9803986(15) 2.01(8)×1019 y
[n 12]
α 205Tl 9/2− 1.0000
210Bi Radium E 83 127 209.9841202(15) 5.012(5) d β 210Po 1− Trace[n 13]
α (1.32×10−4%) 206Tl
210mBi 271.31(11) keV 3.04(6)×106 y α 206Tl 9−
211Bi Actinium C 83 128 210.987269(6) 2.14(2) min α (99.72%) 207Tl 9/2− Trace[n 14]
β (0.276%) 211Po
211mBi 1257(10) keV 1.4(3) μs IT 211Bi (25/2−)
212Bi Thorium C 83 129 211.991285(2) 60.55(6) min β (64.05%) 212Po 1− Trace[n 15]
α (35.94%) 208Tl
β, α (0.014%) 208Pb
212m1Bi 250(30) keV 25.0(2) min α (67%) 208Tl (8−, 9−)
β, α (30%) 208Pb
β (3%) 212Po
212m2Bi 1479(30) keV 7.0(3) min β 212Po (18−)
213Bi
[n 16][n 17]
83 130 212.994384(5) 45.60(4) min β (97.91%) 213Po 9/2− Trace[n 18]
α (2.09%) 209Tl
213mBi 1353(21) keV >168 s 25/2−#
214Bi Radium C 83 131 213.998711(12) 19.9(4) min β (99.98%) 214Po 1− Trace[n 13]
α (0.021%) 210Tl
β, α (0.003%) 210Pb
214mBi 539(30) keV >93 s 8−#
215Bi 83 132 215.001749(6) 7.62(13) min β 215Po (9/2−) Trace[n 14]
215mBi 1367(20)# keV 36.9(6) s IT (76.9%) 215Bi (25/2−)
β (23.1%) 215Po
216Bi 83 133 216.006306(12) 2.21(4) min β 216Po (6−, 7−)
216mBi[n 9] 24(19) keV 6.6(21) min β 216Po 3−#
217Bi 83 134 217.009372(19) 98.5(13) s β 217Po 9/2−#
217mBi 1491(20) keV 3.0(2) μs IT 217Bi 25/2−#
218Bi 83 135 218.014188(29) 33(1) s β 218Po 8−#
219Bi 83 136 219.01752(22)# 8.7(29) s β 219Po 9/2−#
220Bi 83 137 220.02250(32)# 9.5(57) s β 220Po 1−#
221Bi 83 138 221.02598(32)# 2# s
[>300 ns]
9/2−#
222Bi 83 139 222.03108(32)# 3# s
[>300 ns]
1−#
223Bi 83 140 223.03461(43)# 1# s
[>300 ns]
9/2−#
224Bi 83 141 224.03980(43)# 1# s
[>300 ns]
1−#
This table header & footer:
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  1. mBi  Excited nuclear isomer.
  2. ()  Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
  3. #  Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  4. Bold half-life  nearly stable, half-life longer than age of universe.
  5. Bold symbol as daughter  Daughter product is stable.
  6. () spin value  Indicates spin with weak assignment arguments.
  7. #  Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  8. Order of ground state and isomer is uncertain.
  9. Formerly believed to be final decay product of 4n+1 decay chain
  10. Primordial radioisotope, also some is radiogenic from the extinct nuclide 237Np
  11. Formerly believed to be the heaviest stable nuclide
  12. Intermediate decay product of 238U
  13. Intermediate decay product of 235U
  14. Intermediate decay product of 232Th
  15. Used in medicine such as for cancer treatment.
  16. A byproduct of thorium reactors via 233U.
  17. Intermediate decay product of 237Np
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Bismuth-213

Bismuth-213 (213Bi) has a half-life of 45 minutes and decays via alpha emission. Commercially, bismuth-213 can be produced by bombarding radium with bremsstrahlung photons from a linear particle accelerator, which populates its progenitor actinium-225. In 1997, an antibody conjugate with 213Bi was used to treat patients with leukemia. This isotope has also been tried in targeted alpha therapy (TAT) program to treat a variety of cancers.[7] Bismuth-213 is also found in the decay chain of uranium-233, which is the fuel bred by thorium reactors.

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References

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