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词条 Isotopes of bismuth
释义

  1. List of isotopes

      Notes  

  2. See also

  3. References

{{infobox bismuth isotopes}}

Bismuth (83Bi) has no stable isotopes, but does have one very long-lived isotope; thus, the standard atomic weight can be given as {{val|208.98040|(1)}}. Although bismuth-209 is now known to be unstable, it has classically been considered to be a "stable" isotope because it has a half-life of over 1.9×1019 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 occur 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.

Commercially the radioactive isotope bismuth-213 can be produced by bombarding radium with bremsstrahlung photons from a linear particle accelerator. In 1997 an antibody conjugate with Bi-213, which has a 45-minute half-life, and decays with the emission of an alpha-particle, 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.[1] Bismuth-213 is also found on the decay chain of uranium-233 which is the fuel "bred" by Thorium reactors.

List of isotopes

nuclide
symbol
historic
name
Z(p) N(n)  
isotopic
mass (u)[2]
 
half-life
[3][4]
decay
mode
[5][6]
daughter
isotope
[7]
nuclear
spin and
parity
representative
isotopic
composition
(mole fraction)
range of
natural
variation
(mole fraction)
excitation energy
184Bi83101 184.00112(14)# 6.6(15) ms 3+#
184mBi150(100)# keV 13(2) ms 10−#
185Bi83102184.99763(6)#2# ms p 184Pb9/2−#
α (rare) 181Tl
185mBi70(50)# keV49(7) µs α 181Tl1/2+
p 184Pb
186Bi83103185.99660(8)14.8(7) ms α 182Tl(3+)
β+ (rare) 186Pb
186mBi270(140)# keV9.8(4) ms α 182Tl(10−)
β+ 186Pb
187Bi83104186.993158(16)32(3) ms α (50%) 183Tl9/2−#
β+ (50%) 187Pb
187m1Bi101(20) keV 320(70) µs 1/2+#
187m2Bi252(1) keV 7(5) µs (13/2+)
188Bi83105187.99227(5)44(3) ms α 184Tl3+#
β+ (rare) 188Pb
188mBi210(140)# keV220(40) ms α 184Tl(10−)
β+ (rare) 188Pb
189Bi83106188.98920(6)674(11) ms α (51%) 185Tl(9/2−)
β+ (49%) 189Pb
189m1Bi181(6) keV 5.0(1) ms (1/2+)
189m2Bi357(1) keV 880(50) ns (13/2+)
190Bi83107189.9883(2)6.3(1) s α (77%) 186Tl(3+)
β+ (30%) 190Pb
190m1Bi420(180) keV6.2(1) s α (70%) 186Tl(10−)
β+ (23%) 190Pb
190m2Bi690(180) keV >500(100) ns 7+#
191Bi83108190.985786(8)12.3(3) s α (60%) 187Tl(9/2−)
β+ (40%) 191Pb
191mBi240(4) keV124(5) ms α (75%) 187Tl(1/2+)
β+ (25%) 191Pb
192Bi83109191.98546(4)34.6(9) s β+ (82%) 192Pb(3+)
α (18%) 188Tl
192mBi150(30) keV39.6(4) s β+ (90.8%) 192Pb(10−)
α (9.2%) 188Tl
193Bi83110192.98296(1)67(3) s β+ (95%) 193Pb(9/2−)
α (5%) 189Tl
193mBi308(7) keV3.2(6) s α (90%) 189Tl(1/2+)
β+ (10%) 193Pb
194Bi83111193.98283(5)95(3) s β+ (99.54%) 194Pb(3+)
α (.46%) 190Tl
194m1Bi110(70) keV125(2) s β+ 194Pb(6+,7+)
α (rare) 190Tl
194m2Bi230(90)# keV 115(4) s (10−)
195Bi83112194.980651(6)183(4) s β+ (99.97%) 195Pb(9/2−)
α (.03%) 191Tl
195m1Bi399(6) keV87(1) s β+ (67%) 195Pb(1/2+)
α (33%) 191Tl
195m2Bi2311.4+X keV 750(50) ns (29/2−)
196Bi83113195.980667(26)5.1(2) min β+ (99.99%) 196Pb(3+)
α (.00115%) 192Tl
196m1Bi166.6(30) keV0.6(5) s IT 196Bi(7+)
β+ 196Pb
196m2Bi270(3) keV 4.00(5) min (10−)
197Bi83114196.978864(9)9.33(50) min β+ (99.99%) 197Pb(9/2−)
α (10−4%) 193Tl
197m1Bi690(110) keV5.04(16) min α (55%) 193Tl(1/2+)
β+ (45%) 197Pb
IT (.3%) 197Bi
197m2Bi2129.3(4) keV 204(18) ns (23/2−)
197m3Bi2360.4(5)+X keV 263(13) ns (29/2−)
197m4Bi2383.1(7)+X keV 253(39) ns (29/2−)
197m5Bi2929.5(5) keV 209(30) ns (31/2−)
198Bi83115 197.97921(3) 10.3(3) min β+ 198Pb (2+,3+)
198m1Bi280(40) keV 11.6(3) min β+ 198Pb (7+)
198m2Bi530(40) keV 7.7(5) s 10−
199Bi83116 198.977672(13) 27(1) min β+ 199Pb 9/2−
199m1Bi667(4) keV24.70(15) min β+ (98%) 199Pb(1/2+)
IT (2%) 199Bi
α (.01%) 195Tl
199m2Bi1947(25) keV 0.10(3) µs (25/2+)
199m3Bi~2547.0 keV 168(13) ns 29/2−
200Bi83117 199.978132(26) 36.4(5) min β+ 200Pb 7+
200m1Bi100(70)# keV31(2) min EC (90%) 200Pb(2+)
IT (10%) 200Bi
200m2Bi428.20(10) keV 400(50) ms (10−)
201Bi83118200.977009(16)108(3) min β+ (99.99%) 201Pb9/2−
α (10−4%) 197Tl
201m1Bi846.34(21) keV59.1(6) min EC (92.9%) 201Pb1/2+
IT (6.8%) 201Bi
α (.3%) 197Tl
201m2Bi1932.2+X keV 118(28) ns (25/2+)
201m3Bi1971.2+X keV 105(75) ns (27/2+)
201m4Bi2739.90(20)+X keV 124(4) ns (29/2−)
202Bi83119201.977742(22)1.72(5) h β+ 202Pb5(+#)
α (10−5%) 198Tl
202m1Bi615(7) keV 3.04(6) µs (10#)−
202m2Bi2607.1(5) keV 310(50) ns (17+)
203Bi83120202.976876(23)11.76(5) h β+ 203Pb9/2−
α (10−5%) 199Tl
203m1Bi1098.14(7) keV 303(5) ms IT 203Bi 1/2+
203m2Bi2041.5(6) keV 194(30) ns 25/2+
204Bi83121 203.977813(28) 11.22(10) h β+ 204Pb 6+
204m1Bi805.5(3) keV 13.0(1) ms IT 204Bi 10−
204m2Bi2833.4(11) keV 1.07(3) ms (17+)
205Bi83122 204.977389(8) 15.31(4) d β+ 205Pb 9/2−
206Bi83123 205.978499(8) 6.243(3) d β+ 206Pb 6(+)
206m1Bi59.897(17) keV 7.7(2) µs (4+)
206m2Bi1044.8(5) keV 890(10) µs (10−)
207Bi83124 206.9784707(26) 32.9(14) y β+ 207Pb 9/2−
207mBi2101.49(16) keV 182(6) µs 21/2+
208Bi83125 207.9797422(25) 3.68(4)×105 y β+ 208Pb (5)+
208mBi1571.1(4) keV 2.58(4) ms IT 208Bi (10)−
209Bi
[8][9]
83126 208.9803987(16) 1.9(2)×1019 y
[10]
α 205Tl 9/2− 1.0000
210BiRadium E83127209.9841204(16)5.012(5) d β 210Po1−Trace[11]
α (1.32×10−4%) 206Tl
210mBi271.31(11) keV 3.04(6)×106 y α 206Tl 9−
211BiActinium C83128210.987269(6)2.14(2) min α (99.72%) 207Tl9/2−Trace[12]
β (.276%) 211Po
211mBi1257(10) keV 1.4(3) µs (25/2−)
212BiThorium C83129211.9912857(21)60.55(6) min β (64.05%) 212Po1(−)Trace[13]
α (35.94%) 208Tl
β, α (.014%) 208Pb
212m1Bi250(30) keV25.0(2) min α (67%) 208Tl(9−)
β (33%) 212mPo
β, α (.3%) 208Pb
212m2Bi2200(200)# keV 7.0(3) min >16
213Bi
[14][15]
83130212.994385(5)45.59(6) min β (97.91%) 213Po9/2−
α (2.09%) 209Tl
214BiRadium C83131213.998712(12)19.9(4) min β (99.97%) 214Po1−Trace[11]
α (.021%) 210Tl
β, α (.003%) 210Pb
215Bi83132 215.001770(16) 7.6(2) min β 215Po (9/2−) Trace[12]
215mBi1347.5(25) keV36.9(0.6) s IT (76.9%) 215Bi(25/2−)
β (23.1%) 215Po
216Bi83133 216.006306(12) 2.17(5) min β 216Po (6-, 7-)
216mBi24(19) keV 6.6(2.1) min β 216Po 3-#
217Bi83134 217.009372(19) 98.5(8) s β 217Po 9/2−#
217mBi1480(40) keV 2.70(0.06) µs IT 217Bi 25/2−#
218Bi83135 218.014188(29) 33(1) s β 218Po (6-, 7-, 8-)
219Bi83136 219.017480(210)# 8.7(2.9) s β 219Po 9/2-#
220Bi83137 220.022350(320)# 9.5(5.7) s β 220Po 1-#
1. ^{{cite journal|doi=10.1016/S0360-3016(01)01585-1|title=Advancements in cancer therapy with alpha-emitters: a review|year=2001|last1=Imam|first1=S|journal=International Journal of Radiation Oncology Biology Physics|volume=51|pages=271}}
2. ^{{cite journal|last=Wang|first=M.|last2=Audi|first2=G.|last3=Kondev|first3=F.G. |last4=Huang|first4=W.J.|last5=Naimi|first5=S.|last6=Xu|first6=X.|title=The AME2016 atomic mass evaluation (II). Tables, graphs, and references|journal=Chinese Physics C|volume=41|issue=3|pages=030003|date=2017|doi=10.1088/1674-1137/41/3/030003}}
3. ^{{NUBASE 2016}}
4. ^Bold for isotopes with half-lives longer than the age of the universe (nearly stable)
5. ^{{cite web |url=http://www.nucleonica.net/unc.aspx |title=Universal Nuclide Chart |publisher=nucleonica |registration=yes}}
6. ^Abbreviations:
EC: Electron capture
IT: Isomeric transition
7. ^Bold for stable isotopes
8. ^Formerly believed to be final decay product of 4n+1 decay chain
9. ^Primordial radioisotope, also some is radiogenic from the extinct nuclide 237Np
10. ^Formerly believed to be the heaviest stable nuclide
11. ^Intermediate decay product of 238U
12. ^Intermediate decay product of 235U
13. ^Intermediate decay product of 232Th
14. ^Used in medicine such as for cancer treatment.
15. ^A byproduct of Thorium reactors via 233U.

Notes

  • Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
  • Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use expanded uncertainties.

See also

{{Wikipedia-Books|Bismuth}}{{-}}

References

  • Isotope masses from:
    • {{NUBASE 2003}}
  • Isotopic compositions and standard atomic masses from:
    • {{CAWIA 2003}}
    • {{CIAAW 2005}}
  • Half-life, spin, and isomer data selected from the following sources. See editing notes on this article's talk page.
    • {{NUBASE 2003}}
    • {{NNDC}}
    • {{CRC85|chapter=11}}
{{Navbox element isotopes}}

3 : Bismuth|Isotopes of bismuth|Lists of isotopes by element

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