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Isotopes of bismuth

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.

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)

List of isotopes edit

Nuclide
[n 1]
Historic
name
Z N Isotopic mass (Da)[4]
[n 2][n 3]
Half-life
[n 4]
Decay
mode

[n 5]
Daughter
isotope

[n 6]
Spin and
parity
[n 7][n 8]
Natural abundance (mole fraction)
Excitation energy[n 8] Normal proportion Range of variation
184Bi[5] 83 101 184 00135(13)# 13(2) ms α 180Tl 3+#
184mBi 150(100)# keV 6.6(15) 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[7] 83 103 185.996623(18) 14.8(7) ms α 182Tl (3+)
β+? 186Pb
β+, SF (0.011%) (various)
186mBi 170(100)# keV 9.8(4) ms α 182Tl (10−)
β+? 186Pb
β+, SF (0.011%) (various)
187Bi[7] 83 104 186.993147(11) 37(2) ms α 183Tl (9/2−)
β+ (rare) 187Pb
187m1Bi 108(8) keV 370(20) μs α 183Tl (1/2+)
187m2Bi 252(3) keV 7(5) μs IT 187Bi (13/2+)
188Bi[7] 83 105 187.992276(12) 60(3) ms α 184Tl (3+)
β+ (rare) 188Pb
β+, SF (0.0014%) (various)
188m1Bi 66(30) keV >5 μs IT 184Tl 7+#
188m2Bi 153(30) keV 265(15) ms α 184Tl (10−)
β+ (rare) 188Pb
189Bi[7] 83 106 188.989195(22) 688(5) ms α 185Tl (9/2−)
β+? 189Pb
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[7] 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[7] 83 108 190.985787(8) 12.4(3) s α (51%) 187Tl (9/2−)
β+ (49%) 191Pb
191m1Bi 242(4) keV 124(5) ms α (68%) 187Tl (1/2+)
IT (32%) 191Bi
β+ (rare) 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+ (82%) 192Pb (3+)
α (18%) 188Tl
192mBi 150(30) keV 39.6(4) s β+ (90.8%) 192Pb (10−)
α (9.2%) 188Tl
193Bi 83 110 192.982947(8) 67(3) s β+ (95%) 193Pb (9/2−)
α (5%) 189Tl
193mBi 308(7) keV 3.2(6) s α (90%) 189Tl (1/2+)
β+ (10%) 193Pb
194Bi 83 111 193.982799(6) 95(3) s β+ (99.54%) 194Pb (3+)
α (.46%) 190Tl
194m1Bi 110(70) keV 125(2) s β+ 194Pb (6+, 7+)
α (rare) 190Tl
194m2Bi 230(90)# keV 115(4) s (10−)
195Bi 83 112 194.980649(6) 183(4) s β+ (99.97%) 195Pb (9/2−)
α (.03%) 191Tl
195m1Bi 399(6) keV 87(1) s β+ (67%) 195Pb (1/2+)
α (33%) 191Tl
195m2Bi 2311.4+X keV 750(50) ns (29/2−)
196Bi 83 113 195.980667(26) 5.1(2) min β+ (99.99%) 196Pb (3+)
α (.00115%) 192Tl
196m1Bi 166.6(30) keV 0.6(5) s IT 196Bi (7+)
β+ 196Pb
196m2Bi 270(3) keV 4.00(5) min (10−)
197Bi 83 114 196.978865(9) 9.33(50) min β+ (99.99%) 197Pb (9/2−)
α (10−4%) 193Tl
197m1Bi 690(110) keV 5.04(16) min α (55%) 193Tl (1/2+)
β+ (45%) 197Pb
IT (.3%) 197Bi
197m2Bi 2129.3(4) keV 204(18) ns (23/2−)
197m3Bi 2360.4(5)+X keV 263(13) ns (29/2−)
197m4Bi 2383.1(7)+X keV 253(39) ns (29/2−)
197m5Bi 2929.5(5) keV 209(30) ns (31/2−)
198Bi 83 115 197.979201(30) 10.3(3) min β+ 198Pb (2+, 3+)
198m1Bi 280(40) keV 11.6(3) min β+ 198Pb (7+)
198m2Bi 530(40) keV 7.7(5) s 10−
199Bi 83 116 198.977673(11) 27(1) min β+ 199Pb 9/2−
199m1Bi 667(4) keV 24.70(15) min β+ (98%) 199Pb (1/2+)
IT (2%) 199Bi
α (.01%) 195Tl
199m2Bi 1947(25) keV 0.10(3) μs (25/2+)
199m3Bi ~2547.0 keV 168(13) ns 29/2−
200Bi 83 117 199.978131(24) 36.4(5) min β+ 200Pb 7+
200m1Bi 100(70)# keV 31(2) min EC (90%) 200Pb (2+)
IT (10%) 200Bi
200m2Bi 428.20(10) keV 400(50) ms (10−)
201Bi 83 118 200.976995(13) 108(3) min β+ (99.99%) 201Pb 9/2−
α (10−4%) 197Tl
201m1Bi 846.34(21) keV 59.1(6) min EC (92.9%) 201Pb 1/2+
IT (6.8%) 201Bi
α (.3%) 197Tl
201m2Bi 1932.2+X keV 118(28) ns (25/2+)
201m3Bi 1971.2+X keV 105(75) ns (27/2+)
201m4Bi 2739.90(20)+X keV 124(4) ns (29/2−)
202Bi 83 119 201.977723(15) 1.72(5) h β+ 202Pb 5(+#)
α (10−5%) 198Tl
202m1Bi 615(7) keV 3.04(6) μs (10#)−
202m2Bi 2607.1(5) keV 310(50) ns (17+)
203Bi 83 120 202.976892(14) 11.76(5) h β+ 203Pb 9/2−
α (10−5%) 199Tl
203m1Bi 1098.14(7) keV 303(5) ms IT 203Bi 1/2+
203m2Bi 2041.5(6) keV 194(30) ns 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 (17+)
205Bi 83 122 204.977385(5) 15.31(4) d β+ 205Pb 9/2−
206Bi 83 123 205.978499(8) 6.243(3) d β+ 206Pb 6(+)
206m1Bi 59.897(17) keV 7.7(2) μs (4+)
206m2Bi 1044.8(5) keV 890(10) μs (10−)
207Bi 83 124 206.9784706(26) 32.9(14) y β+ 207Pb 9/2−
207mBi 2101.49(16) keV 182(6) μs 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 9][n 10]
83 126 208.9803986(15) 2.01(8)×1019 y
[n 11]
α 205Tl 9/2− 1.0000
210Bi Radium E 83 127 209.9841202(15) 5.012(5) d β 210Po 1− Trace[n 12]
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 13]
β (.276%) 211Po
211mBi 1257(10) keV 1.4(3) μs (25/2−)
212Bi Thorium C 83 129 211.991285(2) 60.55(6) min β (64.05%) 212Po 1(−) Trace[n 14]
α (35.94%) 208Tl
β, α (.014%) 208Pb
212m1Bi 250(30) keV 25.0(2) min α (67%) 208Tl (9−)
β (33%) 212mPo
β, α (.3%) 208Pb
212m2Bi 2200(200)# keV 7.0(3) min >16
213Bi
[n 15][n 16]
83 130 212.994384(5) 45.59(6) min β (97.91%) 213Po 9/2− Trace[n 17]
α (2.09%) 209Tl
214Bi Radium C 83 131 213.998711(12) 19.9(4) min β (99.97%) 214Po 1− Trace[n 12]
α (.021%) 210Tl
β, α (.003%) 210Pb
215Bi 83 132 215.001749(6) 7.6(2) min β 215Po (9/2−) Trace[n 13]
215mBi 1347.5(25) keV 36.9(6) s IT (76.9%) 215Bi (25/2−)
β (23.1%) 215Po
216Bi 83 133 216.006306(12) 2.17(5) min β 216Po (6−, 7−)
216mBi 24(19) keV 6.6(21) min β 216Po 3−#
217Bi 83 134 217.009372(19) 98.5(8) s β 217Po 9/2−#
217mBi 1480(40) keV 2.70(6) μs IT 217Bi 25/2−#
218Bi 83 135 218.014188(29) 33(1) s β 218Po (6−, 7−, 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 β? 221Po 9/2−#
β, n? 220Po
222Bi 83 139 222.03108(32)# 3# s β? 222Po 1−#
β, n? 221Po
223Bi 83 140 223.03461(43)# 1# s β? 223Po 9/2−#
β, n? 222Po
224Bi 83 141 224.03980(43)# 1# s β? 224Po 1−#
β, n? 223Po
This table header & footer:
  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. ^ Modes of decay:
  6. ^ Bold symbol as daughter – Daughter product is stable.
  7. ^ ( ) spin value – Indicates spin with weak assignment arguments.
  8. ^ a b # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  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. ^ a b Intermediate decay product of 238U
  13. ^ a b 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

Bismuth-213 edit

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.[8] Bismuth-213 is also found in the decay chain of uranium-233, which is the fuel bred by thorium reactors.

References edit

  1. ^ Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3): 030001. doi:10.1088/1674-1137/abddae.
  2. ^ "Standard Atomic Weights: Bismuth". CIAAW. 2005.
  3. ^ Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN 1365-3075.
  4. ^ Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*". Chinese Physics C. 45 (3): 030003. doi:10.1088/1674-1137/abddaf.
  5. ^ Andreyev, A. N.; Ackermann, D.; Heßberger, F. P.; Hofmann, S.; Huyse, M.; Kojouharov, I.; Kindler, B.; Lommel, B.; Münzenberg, G.; Page, R. D.; Vel, K. Van de; Duppen, P. Van; Heyde, K. (1 October 2003). "α-decay spectroscopy of light odd-odd Bi isotopes - II: 186Bi and the new nuclide 184Bi" (PDF). The European Physical Journal A. 18 (1): 55–64. Bibcode:2003EPJA...18...55A. doi:10.1140/epja/i2003-10051-1. ISSN 1434-601X. S2CID 122369569. Retrieved 20 June 2023.
  6. ^ Doherty, D. T.; Andreyev, A. N.; Seweryniak, D.; Woods, P. J.; Carpenter, M. P.; Auranen, K.; Ayangeakaa, A. D.; Back, B. B.; Bottoni, S.; Canete, L.; Cubiss, J. G.; Harker, J.; Haylett, T.; Huang, T.; Janssens, R. V. F.; Jenkins, D. G.; Kondev, F. G.; Lauritsen, T.; Lederer-Woods, C.; Li, J.; Müller-Gatermann, C.; Potterveld, D.; Reviol, W.; Savard, G.; Stolze, S.; Zhu, S. (12 November 2021). "Solving the Puzzles of the Decay of the Heaviest Known Proton-Emitting Nucleus 185Bi". Physical Review Letters. 127 (20): 202501. Bibcode:2021PhRvL.127t2501D. doi:10.1103/PhysRevLett.127.202501. hdl:20.500.11820/ac1e5604-7bba-4a25-a538-795ca4bdc875. ISSN 0031-9007. PMID 34860042. S2CID 244089059. Retrieved 20 June 2023.
  7. ^ a b c d e f Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (1 March 2021). "The NUBASE2020 evaluation of nuclear physics properties *". Chinese Physics C, High Energy Physics and Nuclear Physics. 45 (3): 030001. Bibcode:2021ChPhC..45c0001K. doi:10.1088/1674-1137/abddae. ISSN 1674-1137. OSTI 1774641. S2CID 233794940.
  8. ^ Imam, S (2001). "Advancements in cancer therapy with alpha-emitters: a review". International Journal of Radiation Oncology, Biology, Physics. 51 (1): 271–278. doi:10.1016/S0360-3016(01)01585-1. PMID 11516878.

isotopes, bismuth, bismuth, 83bi, known, isotopes, ranging, from, 184bi, 224bi, bismuth, stable, isotopes, does, have, very, long, lived, isotope, thus, standard, atomic, weight, given, 98040, although, bismuth, known, radioactive, classically, been, considere. 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 Isotopes of bismuth 83Bi Main isotopes 1 Decay abun dance half life t1 2 mode pro duct 207Bi synth 31 55 y b 207Pb 208Bi synth 3 68 105 y b 208Pb 209Bi 100 2 01 1019 y a 205Tl 210Bi trace 5 012 d b 210Po a 206Tl 210mBi synth 3 04 106 y a 206TlStandard atomic weight Ar Bi 208 98040 0 00001 2 208 98 0 01 abridged 3 viewtalkeditList of isotopes editNuclide n 1 Historicname Z N Isotopic mass Da 4 n 2 n 3 Half life n 4 Decaymode n 5 Daughterisotope n 6 Spin andparity n 7 n 8 Natural abundance mole fraction Excitation energy n 8 Normal proportion Range of variation 184Bi 5 83 101 184 00135 13 13 2 ms a 180Tl 3 184mBi 150 100 keV 6 6 15 ms a 180Tl 10 185Bi 6 83 102 184 99760 9 2 8 2 3 1 0 ms p 92 184Pb 1 2 a 8 181Tl 185mBi 70 50 keV 58 2 ms IT 185Bi 7 2 9 2 186Bi 7 83 103 185 996623 18 14 8 7 ms a 182Tl 3 b 186Pb b SF 0 011 various 186mBi 170 100 keV 9 8 4 ms a 182Tl 10 b 186Pb b SF 0 011 various 187Bi 7 83 104 186 993147 11 37 2 ms a 183Tl 9 2 b rare 187Pb 187m1Bi 108 8 keV 370 20 ms a 183Tl 1 2 187m2Bi 252 3 keV 7 5 ms IT 187Bi 13 2 188Bi 7 83 105 187 992276 12 60 3 ms a 184Tl 3 b rare 188Pb b SF 0 0014 various 188m1Bi 66 30 keV gt 5 ms IT 184Tl 7 188m2Bi 153 30 keV 265 15 ms a 184Tl 10 b rare 188Pb 189Bi 7 83 106 188 989195 22 688 5 ms a 185Tl 9 2 b 189Pb 189m1Bi 184 5 keV 5 0 1 ms a 83 185Tl 1 2 IT 17 189Bi 189m2Bi 357 6 5 keV 880 50 ns IT 189Bi 13 2 190Bi 7 83 107 189 988625 23 6 3 1 s a 77 186Tl 3 b 23 190Pb b SF 6 10 6 various 190m1Bi 120 40 keV 6 2 1 s a 70 186Tl 10 b 30 190Pb b SF 4 10 6 various 190m2Bi 121 15 keV 175 8 ns IT 190Bi 5 190m3Bi 394 40 keV 1 3 8 ms IT 190Bi 8 191Bi 7 83 108 190 985787 8 12 4 3 s a 51 187Tl 9 2 b 49 191Pb 191m1Bi 242 4 keV 124 5 ms a 68 187Tl 1 2 IT 32 191Bi b rare 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 b 82 192Pb 3 a 18 188Tl 192mBi 150 30 keV 39 6 4 s b 90 8 192Pb 10 a 9 2 188Tl 193Bi 83 110 192 982947 8 67 3 s b 95 193Pb 9 2 a 5 189Tl 193mBi 308 7 keV 3 2 6 s a 90 189Tl 1 2 b 10 193Pb 194Bi 83 111 193 982799 6 95 3 s b 99 54 194Pb 3 a 46 190Tl 194m1Bi 110 70 keV 125 2 s b 194Pb 6 7 a rare 190Tl 194m2Bi 230 90 keV 115 4 s 10 195Bi 83 112 194 980649 6 183 4 s b 99 97 195Pb 9 2 a 03 191Tl 195m1Bi 399 6 keV 87 1 s b 67 195Pb 1 2 a 33 191Tl 195m2Bi 2311 4 X keV 750 50 ns 29 2 196Bi 83 113 195 980667 26 5 1 2 min b 99 99 196Pb 3 a 00115 192Tl 196m1Bi 166 6 30 keV 0 6 5 s IT 196Bi 7 b 196Pb 196m2Bi 270 3 keV 4 00 5 min 10 197Bi 83 114 196 978865 9 9 33 50 min b 99 99 197Pb 9 2 a 10 4 193Tl 197m1Bi 690 110 keV 5 04 16 min a 55 193Tl 1 2 b 45 197Pb IT 3 197Bi 197m2Bi 2129 3 4 keV 204 18 ns 23 2 197m3Bi 2360 4 5 X keV 263 13 ns 29 2 197m4Bi 2383 1 7 X keV 253 39 ns 29 2 197m5Bi 2929 5 5 keV 209 30 ns 31 2 198Bi 83 115 197 979201 30 10 3 3 min b 198Pb 2 3 198m1Bi 280 40 keV 11 6 3 min b 198Pb 7 198m2Bi 530 40 keV 7 7 5 s 10 199Bi 83 116 198 977673 11 27 1 min b 199Pb 9 2 199m1Bi 667 4 keV 24 70 15 min b 98 199Pb 1 2 IT 2 199Bi a 01 195Tl 199m2Bi 1947 25 keV 0 10 3 ms 25 2 199m3Bi 2547 0 keV 168 13 ns 29 2 200Bi 83 117 199 978131 24 36 4 5 min b 200Pb 7 200m1Bi 100 70 keV 31 2 min EC 90 200Pb 2 IT 10 200Bi 200m2Bi 428 20 10 keV 400 50 ms 10 201Bi 83 118 200 976995 13 108 3 min b 99 99 201Pb 9 2 a 10 4 197Tl 201m1Bi 846 34 21 keV 59 1 6 min EC 92 9 201Pb 1 2 IT 6 8 201Bi a 3 197Tl 201m2Bi 1932 2 X keV 118 28 ns 25 2 201m3Bi 1971 2 X keV 105 75 ns 27 2 201m4Bi 2739 90 20 X keV 124 4 ns 29 2 202Bi 83 119 201 977723 15 1 72 5 h b 202Pb 5 a 10 5 198Tl 202m1Bi 615 7 keV 3 04 6 ms 10 202m2Bi 2607 1 5 keV 310 50 ns 17 203Bi 83 120 202 976892 14 11 76 5 h b 203Pb 9 2 a 10 5 199Tl 203m1Bi 1098 14 7 keV 303 5 ms IT 203Bi 1 2 203m2Bi 2041 5 6 keV 194 30 ns 25 2 204Bi 83 121 203 977836 10 11 22 10 h b 204Pb 6 204m1Bi 805 5 3 keV 13 0 1 ms IT 204Bi 10 204m2Bi 2833 4 11 keV 1 07 3 ms 17 205Bi 83 122 204 977385 5 15 31 4 d b 205Pb 9 2 206Bi 83 123 205 978499 8 6 243 3 d b 206Pb 6 206m1Bi 59 897 17 keV 7 7 2 ms 4 206m2Bi 1044 8 5 keV 890 10 ms 10 207Bi 83 124 206 9784706 26 32 9 14 y b 207Pb 9 2 207mBi 2101 49 16 keV 182 6 ms 21 2 208Bi 83 125 207 9797421 25 3 68 4 105 y b 208Pb 5 208mBi 1571 1 4 keV 2 58 4 ms IT 208Bi 10 209Bi n 9 n 10 83 126 208 9803986 15 2 01 8 1019 y n 11 a 205Tl 9 2 1 0000 210Bi Radium E 83 127 209 9841202 15 5 012 5 d b 210Po 1 Trace n 12 a 1 32 10 4 206Tl 210mBi 271 31 11 keV 3 04 6 106 y a 206Tl 9 211Bi Actinium C 83 128 210 987269 6 2 14 2 min a 99 72 207Tl 9 2 Trace n 13 b 276 211Po 211mBi 1257 10 keV 1 4 3 ms 25 2 212Bi Thorium C 83 129 211 991285 2 60 55 6 min b 64 05 212Po 1 Trace n 14 a 35 94 208Tl b a 014 208Pb 212m1Bi 250 30 keV 25 0 2 min a 67 208Tl 9 b 33 212mPo b a 3 208Pb 212m2Bi 2200 200 keV 7 0 3 min gt 16 213Bi n 15 n 16 83 130 212 994384 5 45 59 6 min b 97 91 213Po 9 2 Trace n 17 a 2 09 209Tl 214Bi Radium C 83 131 213 998711 12 19 9 4 min b 99 97 214Po 1 Trace n 12 a 021 210Tl b a 003 210Pb 215Bi 83 132 215 001749 6 7 6 2 min b 215Po 9 2 Trace n 13 215mBi 1347 5 25 keV 36 9 6 s IT 76 9 215Bi 25 2 b 23 1 215Po 216Bi 83 133 216 006306 12 2 17 5 min b 216Po 6 7 216mBi 24 19 keV 6 6 21 min b 216Po 3 217Bi 83 134 217 009372 19 98 5 8 s b 217Po 9 2 217mBi 1480 40 keV 2 70 6 ms IT 217Bi 25 2 218Bi 83 135 218 014188 29 33 1 s b 218Po 6 7 8 219Bi 83 136 219 01752 22 8 7 29 s b 219Po 9 2 220Bi 83 137 220 02250 32 9 5 57 s b 220Po 1 221Bi 83 138 221 02598 32 2 s b 221Po 9 2 b n 220Po 222Bi 83 139 222 03108 32 3 s b 222Po 1 b n 221Po 223Bi 83 140 223 03461 43 1 s b 223Po 9 2 b n 222Po 224Bi 83 141 224 03980 43 1 s b 224Po 1 b n 223Po This table header amp footer view mBi Excited nuclear isomer Uncertainty 1s is given in concise form in parentheses after the corresponding last digits Atomic mass marked value and uncertainty derived not from purely experimental data but at least partly from trends from the Mass Surface TMS Bold half life nearly stable half life longer than age of universe Modes of decay EC Electron capture IT Isomeric transition p Proton emission Bold symbol as daughter Daughter product is stable spin value Indicates spin with weak assignment arguments a b Values marked are not purely derived from experimental data but at least partly from trends of neighboring nuclides TNN Formerly believed to be final decay product of 4n 1 decay chain Primordial radioisotope also some is radiogenic from the extinct nuclide 237Np Formerly believed to be the heaviest stable nuclide a b Intermediate decay product of 238U a b Intermediate decay product of 235U Intermediate decay product of 232Th Used in medicine such as for cancer treatment A byproduct of thorium reactors via 233U Intermediate decay product of 237NpBismuth 213 editBismuth 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 8 Bismuth 213 is also found in the decay chain of uranium 233 which is the fuel bred by thorium reactors References edit Kondev F G Wang M Huang W J Naimi S Audi G 2021 The NUBASE2020 evaluation of nuclear properties PDF Chinese Physics C 45 3 030001 doi 10 1088 1674 1137 abddae Standard Atomic Weights Bismuth CIAAW 2005 Prohaska Thomas Irrgeher Johanna Benefield Jacqueline Bohlke John K Chesson Lesley A Coplen Tyler B Ding Tiping Dunn Philip J H Groning Manfred Holden Norman E Meijer Harro A J 2022 05 04 Standard atomic weights of the elements 2021 IUPAC Technical Report Pure and Applied Chemistry doi 10 1515 pac 2019 0603 ISSN 1365 3075 Wang Meng Huang W J Kondev F G Audi G Naimi S 2021 The AME 2020 atomic mass evaluation II Tables graphs and references Chinese Physics C 45 3 030003 doi 10 1088 1674 1137 abddaf Andreyev A N Ackermann D Hessberger F P Hofmann S Huyse M Kojouharov I Kindler B Lommel B Munzenberg G Page R D Vel K Van de Duppen P Van Heyde K 1 October 2003 a decay spectroscopy of light odd odd Bi isotopes II 186Bi and the new nuclide 184Bi PDF The European Physical Journal A 18 1 55 64 Bibcode 2003EPJA 18 55A doi 10 1140 epja i2003 10051 1 ISSN 1434 601X S2CID 122369569 Retrieved 20 June 2023 Doherty D T Andreyev A N Seweryniak D Woods P J Carpenter M P Auranen K Ayangeakaa A D Back B B Bottoni S Canete L Cubiss J G Harker J Haylett T Huang T Janssens R V F Jenkins D G Kondev F G Lauritsen T Lederer Woods C Li J Muller Gatermann C Potterveld D Reviol W Savard G Stolze S Zhu S 12 November 2021 Solving the Puzzles of the Decay of the Heaviest Known Proton Emitting Nucleus 185Bi Physical Review Letters 127 20 202501 Bibcode 2021PhRvL 127t2501D doi 10 1103 PhysRevLett 127 202501 hdl 20 500 11820 ac1e5604 7bba 4a25 a538 795ca4bdc875 ISSN 0031 9007 PMID 34860042 S2CID 244089059 Retrieved 20 June 2023 a b c d e f Kondev F G Wang M Huang W J Naimi S Audi G 1 March 2021 The NUBASE2020 evaluation of nuclear physics properties Chinese Physics C High Energy Physics and Nuclear Physics 45 3 030001 Bibcode 2021ChPhC 45c0001K doi 10 1088 1674 1137 abddae ISSN 1674 1137 OSTI 1774641 S2CID 233794940 Imam S 2001 Advancements in cancer therapy with alpha emitters a review International Journal of Radiation Oncology Biology Physics 51 1 271 278 doi 10 1016 S0360 3016 01 01585 1 PMID 11516878 Isotopic compositions and standard atomic masses from de Laeter John Robert Bohlke John Karl De Bievre Paul Hidaka Hiroshi Peiser H Steffen Rosman Kevin J R Taylor Philip D P 2003 Atomic weights of the elements Review 2000 IUPAC Technical Report Pure and Applied Chemistry 75 6 683 800 doi 10 1351 pac200375060683 Wieser Michael E 2006 Atomic weights of the elements 2005 IUPAC Technical Report Pure and Applied Chemistry 78 11 2051 2066 doi 10 1351 pac200678112051 News amp Notices Standard Atomic Weights Revised International Union of Pure and Applied Chemistry 19 October 2005 Half life spin and isomer data selected from the following sources Audi Georges Bersillon Olivier Blachot Jean Wapstra Aaldert Hendrik 2003 The NUBASE evaluation of nuclear and decay properties Nuclear Physics A 729 3 128 Bibcode 2003NuPhA 729 3A doi 10 1016 j nuclphysa 2003 11 001 National Nuclear Data Center NuDat 2 x database Brookhaven National Laboratory Holden Norman E 2004 11 Table of the Isotopes In Lide David R ed CRC Handbook of Chemistry and Physics 85th ed Boca Raton Florida CRC Press ISBN 978 0 8493 0485 9 Retrieved from https en wikipedia org w index php title Isotopes of bismuth amp oldid 1196448611 Bismuth 210m, wikipedia, wiki, book, books, library,

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