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Isotopes of bismuth: Difference between revisions

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Line 14: Line 14:
! &nbsp;<br />isotopic mass (u)<br />&nbsp;
! &nbsp;<br />isotopic mass (u)<br />&nbsp;
! rowspan="2" | half-life<ref group="n">Bold for isotopes with half-lives longer than the age of the universe (nearly stable)</ref>
! rowspan="2" | half-life<ref group="n">Bold for isotopes with half-lives longer than the age of the universe (nearly stable)</ref>
! rowspan="2" | decay mode(s)<ref>http://www.nucleonica.net/unc.aspx</ref>
! rowspan="2" | daughter<br>isotope(s)
! rowspan="2" | nuclear<br />spin
! rowspan="2" | nuclear<br />spin
! rowspan="2" | representative<br />isotopic<br />composition<br />(mole fraction)
! rowspan="2" | representative<br />isotopic<br />composition<br />(mole fraction)
Line 25: Line 27:
| 184.00112(14)#
| 184.00112(14)#
| 6.6(15) ms
| 6.6(15) ms
|
|
| 3+#
| 3+#
|
|
Line 32: Line 36:
| colspan="3" style="text-indent:2em" | 150(100)# keV
| colspan="3" style="text-indent:2em" | 150(100)# keV
| 13(2) ms
| 13(2) ms
| 10-#
|
|
|
|
|-
| 10-#
| <sup>185</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 102
| 184.99763(6)#
| 2# ms
| 9/2-#
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>185m</sup>Bi
| rowspan=2|<sup>185</sup>Bi
| colspan="3" style="text-indent:2em" | 70(50)# keV
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 102
| 49(7) µs
| rowspan=2|184.99763(6)#
| 1/2+
| rowspan=2|2# ms
|
| [[proton emission|p]]
|
| <sup>184</sup>Pb
| rowspan=2|9/2-#
| rowspan=2|
| rowspan=2|
|-
|-
| [[alpha decay|α]] (rare)
| <sup>186</sup>Bi
| <sup>181</sup>Tl
| style="text-align:right" | 83
| style="text-align:right" | 103
| 185.99660(8)
| 14.8(7) ms
| (3+)
|
|
|-
|-
| style="text-indent:1em" | <sup>186m</sup>Bi
| rowspan=2 style="text-indent:1em" | <sup>185m</sup>Bi
| colspan="3" style="text-indent:2em" | 270(140)# keV
| rowspan=2 colspan="3" style="text-indent:2em" | 70(50)# keV
| 9.8(4) ms
| rowspan=2|49(7) µs
| (10-)
| α
| <sup>181</sup>Tl
|
| rowspan=2|1/2+
|
| rowspan=2|
| rowspan=2|
|-
|-
| p
| <sup>187</sup>Bi
| <sup>184</sup>Pb
| style="text-align:right" | 83
|-
| style="text-align:right" | 104
| rowspan=2|<sup>186</sup>Bi
| 186.993158(16)
| rowspan=2 style="text-align:right" | 83
| 32(3) ms
| rowspan=2 style="text-align:right" | 103
| 9/2-#
| rowspan=2|185.99660(8)
|
| rowspan=2|14.8(7) ms
|
| α
| <sup>182</sup>Tl
| rowspan=2|(3+)
| rowspan=2|
| rowspan=2|
|-
| [[beta decay|β<sup>+</sup>]] (rare)
| <sup>186</sup>Pb
|-
| rowspan=2 style="text-indent:1em" | <sup>186m</sup>Bi
| rowspan=2 colspan="3" style="text-indent:2em" | 270(140)# keV
| rowspan=2|9.8(4) ms
| α
| <sup>182</sup>Tl
| rowspan=2|(10-)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup>
| <sup>186</sup>Pb
|-
| rowspan=2|<sup>187</sup>Bi
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 104
| rowspan=2|186.993158(16)
| rowspan=2|32(3) ms
| α (50%)
| <sup>183</sup>Tl
| rowspan=2|9/2-#
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (50%)
| <sup>187</sup>Pb
|-
|-
| style="text-indent:1em" | <sup>187m1</sup>Bi
| style="text-indent:1em" | <sup>187m1</sup>Bi
| colspan="3" style="text-indent:2em" | 101(20) keV
| colspan="3" style="text-indent:2em" | 101(20) keV
| 320(70) µs
| 320(70) µs
|
|
| 1/2+#
| 1/2+#
|
|
Line 87: Line 120:
| colspan="3" style="text-indent:2em" | 252(1) keV
| colspan="3" style="text-indent:2em" | 252(1) keV
| 7(5) µs
| 7(5) µs
| (13/2+)
|
|
|
|
| (13/2+)
|-
| <sup>188</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 105
| 187.99227(5)
| 44(3) ms
| 3+#
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>188m</sup>Bi
| rowspan=2|<sup>188</sup>Bi
| colspan="3" style="text-indent:2em" | 210(140)# keV
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 105
| 220(40) ms
| rowspan=2|187.99227(5)
| (10-)
| rowspan=2|44(3) ms
|
|
| α
| <sup>184</sup>Tl
| rowspan=2|3+#
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>189</sup>Bi
| β<sup>+</sup> (rare)
| <sup>188</sup>Pb
| style="text-align:right" | 83
|-
| style="text-align:right" | 106
| rowspan=2 style="text-indent:1em" | <sup>188m</sup>Bi
| 188.98920(6)
| rowspan=2 colspan="3" style="text-indent:2em" | 210(140)# keV
| 674(11) ms
| rowspan=2|220(40) ms
| (9/2-)
|
| α
| <sup>184</sup>Tl
|
| rowspan=2|(10-)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (rare)
| <sup>188</sup>Pb
|-
| rowspan=2|<sup>189</sup>Bi
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 106
| rowspan=2|188.98920(6)
| rowspan=2|674(11) ms
| α (51%)
| <sup>185</sup>Tl
| rowspan=2|(9/2-)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (49%)
| <sup>189</sup>Pb
|-
|-
| style="text-indent:1em" | <sup>189m1</sup>Bi
| style="text-indent:1em" | <sup>189m1</sup>Bi
| colspan="3" style="text-indent:2em" | 181(6) keV
| colspan="3" style="text-indent:2em" | 181(6) keV
| 5.0(1) ms
| 5.0(1) ms
|
|
| (1/2+)
| (1/2+)
|
|
Line 126: Line 178:
| colspan="3" style="text-indent:2em" | 357(1) keV
| colspan="3" style="text-indent:2em" | 357(1) keV
| 880(50) ns
| 880(50) ns
| (13/2+)
|
|
|
|
| (13/2+)
|-
| <sup>190</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 107
| 189.9883(2)
| 6.3(1) s
| (3+)
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>190m1</sup>Bi
| rowspan=2|<sup>190</sup>Bi
| colspan="3" style="text-indent:2em" | 420(180) keV
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 107
| 6.2(1) s
| rowspan=2|189.9883(2)
| (10-)
| rowspan=2|6.3(1) s
|
| α (77%)
|
| <sup>186</sup>Tl
| rowspan=2|(3+)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (30%)
| <sup>190</sup>Pb
|-
| rowspan=2 style="text-indent:1em" | <sup>190m1</sup>Bi
| rowspan=2 colspan="3" style="text-indent:2em" | 420(180) keV
| rowspan=2|6.2(1) s
| α (70%)
| <sup>186</sup>Tl
| rowspan=2|(10-)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (30%)
| <sup>190</sup>Pb
|-
|-
| style="text-indent:1em" | <sup>190m2</sup>Bi
| style="text-indent:1em" | <sup>190m2</sup>Bi
| colspan="3" style="text-indent:2em" | 690(180) keV
| colspan="3" style="text-indent:2em" | 690(180) keV
| >500(100) ns
| >500(100) ns
| 7+#
|
|
|
|
| 7+#
|-
| <sup>191</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 108
| 190.985786(8)
| 12.3(3) s
| (9/2-)
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>191m</sup>Bi
| rowspan=2|<sup>191</sup>Bi
| colspan="3" style="text-indent:2em" | 240(4) keV
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 108
| 124(5) ms
| rowspan=2|190.985786(8)
| (1/2+)
| rowspan=2|12.3(3) s
|
| α (60%)
|
| <sup>187</sup>Tl
| rowspan=2|(9/2-)
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>192</sup>Bi
| β<sup>+</sup> (40%)
| <sup>191</sup>Pb
| style="text-align:right" | 83
| style="text-align:right" | 109
| 191.98546(4)
| 34.6(9) s
| (3+)
|
|
|-
|-
| style="text-indent:1em" | <sup>192m</sup>Bi
| rowspan=2 style="text-indent:1em" | <sup>191m</sup>Bi
| colspan="3" style="text-indent:2em" | 150(30) keV
| rowspan=2 colspan="3" style="text-indent:2em" | 240(4) keV
| 39.6(4) s
| rowspan=2|124(5) ms
| (10-)
| α (75%)
| <sup>187</sup>Tl
|
| rowspan=2|(1/2+)
|
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>193</sup>Bi
| β<sup>+</sup> (25%)
| <sup>191</sup>Pb
| style="text-align:right" | 83
| style="text-align:right" | 110
| 192.98296(1)
| 67(3) s
| (9/2-)
|
|
|-
|-
| style="text-indent:1em" | <sup>193m</sup>Bi
| rowspan=2|<sup>192</sup>Bi
| colspan="3" style="text-indent:2em" | 308(7) keV
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 109
| 3.2(6) s
| rowspan=2|191.98546(4)
| (1/2+)
| rowspan=2|34.6(9) s
|
| β<sup>+</sup>
|
| <sup>192</sup>Pb
| rowspan=2|(3+)
| rowspan=2|
| rowspan=2|
|-
|-
| α (18%)
| <sup>194</sup>Bi
| <sup>188</sup>Tl
| style="text-align:right" | 83
| style="text-align:right" | 111
| 193.98283(5)
| 95(3) s
| (3+)
|
|
|-
|-
| style="text-indent:1em" | <sup>194m1</sup>Bi
| rowspan=2 style="text-indent:1em" | <sup>192m</sup>Bi
| colspan="3" style="text-indent:2em" | 110(70) keV
| rowspan=2 colspan="3" style="text-indent:2em" | 150(30) keV
| 125(2) s
| rowspan=2|39.6(4) s
| β<sup>+</sup> (90.8%)
| (6+,7+)
| <sup>192</sup>Pb
|
| rowspan=2|(10-)
|
| rowspan=2|
| rowspan=2|
|-
| α (9.2%)
| <sup>188</sup>Tl
|-
| rowspan=2|<sup>193</sup>Bi
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 110
| rowspan=2|192.98296(1)
| rowspan=2|67(3) s
| β<sup>+</sup> (95%)
| <sup>193</sup>Pb
| rowspan=2|(9/2-)
| rowspan=2|
| rowspan=2|
|-
| α (5%)
| <sup>189</sup>Tl
|-
| rowspan=2 style="text-indent:1em" | <sup>193m</sup>Bi
| rowspan=2 colspan="3" style="text-indent:2em" | 308(7) keV
| rowspan=2|3.2(6) s
| α (90%)
| <sup>189</sup>Tl
| rowspan=2|(1/2+)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (10%)
| <sup>193</sup>Pb
|-
| rowspan=2|<sup>194</sup>Bi
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 111
| rowspan=2|193.98283(5)
| rowspan=2|95(3) s
| β<sup>+</sup> (99.54%)
| <sup>194</sup>Pb
| rowspan=2|(3+)
| rowspan=2|
| rowspan=2|
|-
| α (.46%)
| <sup>190</sup>Tl
|-
| rowspan=2 style="text-indent:1em" | <sup>194m1</sup>Bi
| rowspan=2 colspan="3" style="text-indent:2em" | 110(70) keV
| rowspan=2|125(2) s
| β<sup>+</sup>
| <sup>194</sup>Pb
| rowspan=2|(6+,7+)
| rowspan=2|
| rowspan=2|
|-
| α (rare)
| <sup>190</sup>Tl
|-
|-
| style="text-indent:1em" | <sup>194m2</sup>Bi
| style="text-indent:1em" | <sup>194m2</sup>Bi
| colspan="3" style="text-indent:2em" | 230(90)# keV
| colspan="3" style="text-indent:2em" | 230(90)# keV
| 115(4) s
| 115(4) s
| (10-)
|
|
|
|
|-
| (10-)
| <sup>195</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 112
| 194.980651(6)
| 183(4) s
| (9/2-)
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>195m1</sup>Bi
| rowspan=2|<sup>195</sup>Bi
| colspan="3" style="text-indent:2em" | 399(6) keV
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 112
| 87(1) s
| rowspan=2|194.980651(6)
| (1/2+)
| rowspan=2|183(4) s
|
| β<sup>+</sup> (99.97%)
|
| <sup>195</sup>Pb
| rowspan=2|(9/2-)
| rowspan=2|
| rowspan=2|
|-
| α (.03%)
| <sup>191</sup>Tl
|-
| rowspan=2 style="text-indent:1em" | <sup>195m1</sup>Bi
| rowspan=2 colspan="3" style="text-indent:2em" | 399(6) keV
| rowspan=2|87(1) s
| β<sup>+</sup> (67%)
| <sup>195</sup>Pb
| rowspan=2|(1/2+)
| rowspan=2|
| rowspan=2|
|-
| α (33%)
| <sup>191</sup>Tl
|-
|-
| style="text-indent:1em" | <sup>195m2</sup>Bi
| style="text-indent:1em" | <sup>195m2</sup>Bi
| colspan="3" style="text-indent:2em" | 2311.4+X keV
| colspan="3" style="text-indent:2em" | 2311.4+X keV
| 750(50) ns
| 750(50) ns
|
|
| (29/2-)
| (29/2-)
|
|
|
|
|-
|-
| rowspan=2|<sup>196</sup>Bi
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 113
| rowspan=2|195.980667(26)
| rowspan=2|5.1(2) min
| β<sup>+</sup> (99.99%)
| <sup>196</sup>Pb
| rowspan=2|(3+)
| rowspan=2|
| rowspan=2|
|-
| α (.00115%)
| <sup>192</sup>Tl
|-
| rowspan=2 style="text-indent:1em" | <sup>196m1</sup>Bi
| rowspan=2 colspan="3" style="text-indent:2em" | 166.6(30) keV
| rowspan=2|0.6(5) s
| [[Isomeric transition|IT]]
| <sup>196</sup>Bi
| <sup>196</sup>Bi
| rowspan=2|(7+)
| style="text-align:right" | 83
| rowspan=2|
| style="text-align:right" | 113
| rowspan=2|
| 195.980667(26)
| 5.1(2) min
| (3+)
|
|
|-
|-
| style="text-indent:1em" | <sup>196m1</sup>Bi
| β<sup>+</sup>
| <sup>196</sup>Pb
| colspan="3" style="text-indent:2em" | 166.6(30) keV
| 0.6(5) s
| (7+)
|
|
|-
|-
| style="text-indent:1em" | <sup>196m2</sup>Bi
| style="text-indent:1em" | <sup>196m2</sup>Bi
| colspan="3" style="text-indent:2em" | 270(3) keV
| colspan="3" style="text-indent:2em" | 270(3) keV
| 4.00(5) min
| 4.00(5) min
|
|
| (10-)
| (10-)
|
|
|
|
|-
|-
| <sup>197</sup>Bi
| rowspan=2|<sup>197</sup>Bi
| style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 83
| style="text-align:right" | 114
| rowspan=2 style="text-align:right" | 114
| 196.978864(9)
| rowspan=2|196.978864(9)
| 9.33(50) min
| rowspan=2|9.33(50) min
| β<sup>+</sup> (99.99%)
| (9/2-)
| <sup>197</sup>Pb
|
| rowspan=2|(9/2-)
|
| rowspan=2|
| rowspan=2|
|-
|-
| α (.0001%)
| style="text-indent:1em" | <sup>197m1</sup>Bi
| <sup>193</sup>Tl
| colspan="3" style="text-indent:2em" | 690(110) keV
|-
| 5.04(16) min
| rowspan=3 style="text-indent:1em" | <sup>197m1</sup>Bi
| (1/2+)
| rowspan=3 colspan="3" style="text-indent:2em" | 690(110) keV
|
| rowspan=3|5.04(16) min
|
| α (55%)
| <sup>193</sup>Tl
| rowspan=3|(1/2+)
| rowspan=3|
| rowspan=3|
|-
| β<sup>+</sup> (45%)
| <sup>197</sup>Pb
|-
| IT (.3%)
| <sup>197</sup>Bi
|-
|-
| style="text-indent:1em" | <sup>197m2</sup>Bi
| style="text-indent:1em" | <sup>197m2</sup>Bi
| colspan="3" style="text-indent:2em" | 2129.3(4) keV
| colspan="3" style="text-indent:2em" | 2129.3(4) keV
| 204(18) ns
| 204(18) ns
|
|
| (23/2-)
| (23/2-)
|
|
Line 296: Line 443:
| colspan="3" style="text-indent:2em" | 2360.4(5)+X keV
| colspan="3" style="text-indent:2em" | 2360.4(5)+X keV
| 263(13) ns
| 263(13) ns
|
|
| (29/2-)
| (29/2-)
|
|
Line 303: Line 452:
| colspan="3" style="text-indent:2em" | 2383.1(7)+X keV
| colspan="3" style="text-indent:2em" | 2383.1(7)+X keV
| 253(39) ns
| 253(39) ns
|
|
| (29/2-)
| (29/2-)
|
|
Line 310: Line 461:
| colspan="3" style="text-indent:2em" | 2929.5(5) keV
| colspan="3" style="text-indent:2em" | 2929.5(5) keV
| 209(30) ns
| 209(30) ns
|
|
| (31/2-)
| (31/2-)
|
|
Line 319: Line 472:
| 197.97921(3)
| 197.97921(3)
| 10.3(3) min
| 10.3(3) min
| β<sup>+</sup>
| <sup>198</sup>Pb
| (2+,3+)
| (2+,3+)
|
|
Line 326: Line 481:
| colspan="3" style="text-indent:2em" | 280(40) keV
| colspan="3" style="text-indent:2em" | 280(40) keV
| 11.6(3) min
| 11.6(3) min
| β<sup>+</sup>
| <sup>198</sup>Pb
| (7+)
| (7+)
|
|
Line 333: Line 490:
| colspan="3" style="text-indent:2em" | 530(40) keV
| colspan="3" style="text-indent:2em" | 530(40) keV
| 7.7(5) s
| 7.7(5) s
|
|
| 10-
| 10-
|
|
Line 342: Line 501:
| 198.977672(13)
| 198.977672(13)
| 27(1) min
| 27(1) min
| β<sup>+</sup>
| <sup>199</sup>Pb
| 9/2-
| 9/2-
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>199m1</sup>Bi
| rowspan=3 style="text-indent:1em" | <sup>199m1</sup>Bi
| colspan="3" style="text-indent:2em" | 667(4) keV
| rowspan=3 colspan="3" style="text-indent:2em" | 667(4) keV
| 24.70(15) min
| rowspan=3|24.70(15) min
| β<sup>+</sup> (98%)
| (1/2+)
| <sup>199</sup>Pb
|
| rowspan=3|(1/2+)
|
| rowspan=3|
| rowspan=3|
|-
| IT
| <sup>199</sup>Bi
|-
| α (.01%)
| <sup>195</sup>Tl
|-
|-
| style="text-indent:1em" | <sup>199m2</sup>Bi
| style="text-indent:1em" | <sup>199m2</sup>Bi
| colspan="3" style="text-indent:2em" | 1947(25) keV
| colspan="3" style="text-indent:2em" | 1947(25) keV
| 0.10(3) µs
| 0.10(3) µs
|
|
| (25/2+)
| (25/2+)
|
|
Line 363: Line 534:
| colspan="3" style="text-indent:2em" | ~2547.0 keV
| colspan="3" style="text-indent:2em" | ~2547.0 keV
| 168(13) ns
| 168(13) ns
|
|
| 29/2-
| 29/2-
|
|
Line 372: Line 545:
| 199.978132(26)
| 199.978132(26)
| 36.4(5) min
| 36.4(5) min
| β<sup>+</sup>
| <sup>200</sup>Pb
| 7+
| 7+
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>200m1</sup>Bi
| rowspan=2 style="text-indent:1em" | <sup>200m1</sup>Bi
| colspan="3" style="text-indent:2em" | 100(70)# keV
| rowspan=2 colspan="3" style="text-indent:2em" | 100(70)# keV
| 31(2) min
| rowspan=2|31(2) min
| [[Electron capture|EC]] (90%)
| (2+)
| <sup>200</sup>Pb
|
| rowspan=2|(2+)
|
| rowspan=2|
| rowspan=2|
|-
| IT (10%)
| <sup>200</sup>Bi
|-
|-
| style="text-indent:1em" | <sup>200m2</sup>Bi
| style="text-indent:1em" | <sup>200m2</sup>Bi
| colspan="3" style="text-indent:2em" | 428.20(10) keV
| colspan="3" style="text-indent:2em" | 428.20(10) keV
| 400(50) ms
| 400(50) ms
|
|
| (10-)
| (10-)
|
|
|
|
|-
|-
| rowspan=2|<sup>201</sup>Bi
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 118
| rowspan=2|200.977009(16)
| rowspan=2|108(3) min
| β<sup>+</sup> (99.99%)
| <sup>201</sup>Pb
| rowspan=2|9/2-
| rowspan=2|
| rowspan=2|
|-
| α (.0001%)
| <sup>197</sup>Tl
|-
| rowspan=3 style="text-indent:1em" | <sup>201m1</sup>Bi
| rowspan=3 colspan="3" style="text-indent:2em" | 846.34(21) keV
| rowspan=3|59.1(6) min
| EC (92.9%)
| <sup>201</sup>Pb
| rowspan=3|1/2+
| rowspan=3|
| rowspan=3|
|-
| IT (6.8%)
| <sup>201</sup>Bi
| <sup>201</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 118
| 200.977009(16)
| 108(3) min
| 9/2-
|
|
|-
|-
| α (.3%)
| style="text-indent:1em" | <sup>201m1</sup>Bi
| <sup>197</sup>Tl
| colspan="3" style="text-indent:2em" | 846.34(21) keV
| 59.1(6) min
| 1/2+
|
|
|-
|-
| style="text-indent:1em" | <sup>201m2</sup>Bi
| style="text-indent:1em" | <sup>201m2</sup>Bi
| colspan="3" style="text-indent:2em" | 1932.2+X keV
| colspan="3" style="text-indent:2em" | 1932.2+X keV
| 118(28) ns
| 118(28) ns
|
|
| (25/2+)
| (25/2+)
|
|
Line 416: Line 613:
| colspan="3" style="text-indent:2em" | 1971.2+X keV
| colspan="3" style="text-indent:2em" | 1971.2+X keV
| 105(75) ns
| 105(75) ns
|
|
| (27/2+)
| (27/2+)
|
|
Line 423: Line 622:
| colspan="3" style="text-indent:2em" | 2739.90(20)+X keV
| colspan="3" style="text-indent:2em" | 2739.90(20)+X keV
| 124(4) ns
| 124(4) ns
| (29/2-)
|
|
|
|
|-
| (29/2-)
| <sup>202</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 119
| 201.977742(22)
| 1.72(5) h
| 5(+#)
|
|
|
|
|-
| rowspan=2|<sup>202</sup>Bi
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 119
| rowspan=2|201.977742(22)
| rowspan=2|1.72(5) h
| β<sup>+</sup>
| <sup>202</sup>Pb
| rowspan=2|5(+#)
| rowspan=2|
| rowspan=2|
|-
| α (.00001%)
| <sup>198</sup>Tl
|-
|-
| style="text-indent:1em" | <sup>202m1</sup>Bi
| style="text-indent:1em" | <sup>202m1</sup>Bi
| colspan="3" style="text-indent:2em" | 615(7) keV
| colspan="3" style="text-indent:2em" | 615(7) keV
| 3.04(6) µs
| 3.04(6) µs
|
|
| (10#)-
| (10#)-
|
|
Line 446: Line 654:
| colspan="3" style="text-indent:2em" | 2607.1(5) keV
| colspan="3" style="text-indent:2em" | 2607.1(5) keV
| 310(50) ns
| 310(50) ns
| (17+)
|
|
|
|
| (17+)
|-
| <sup>203</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 120
| 202.976876(23)
| 11.76(5) h
| 9/2-
|
|
|
|
|-
| rowspan=2|<sup>203</sup>Bi
| rowspan=2 style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 120
| rowspan=2|202.976876(23)
| rowspan=2|11.76(5) h
| β<sup>+</sup>
| <sup>203</sup>Pb
| rowspan=2|9/2-
| rowspan=2|
| rowspan=2|
|-
| α (.00001%)
| <sup>199</sup>Tl
|-
|-
| style="text-indent:1em" | <sup>203m1</sup>Bi
| style="text-indent:1em" | <sup>203m1</sup>Bi
| colspan="3" style="text-indent:2em" | 1098.14(7) keV
| colspan="3" style="text-indent:2em" | 1098.14(7) keV
| 303(5) ms
| 303(5) ms
| IT
| <sup>203</sup>Bi
| 1/2+
| 1/2+
|
|
Line 469: Line 686:
| colspan="3" style="text-indent:2em" | 2041.5(6) keV
| colspan="3" style="text-indent:2em" | 2041.5(6) keV
| 194(30) ns
| 194(30) ns
|
|
| 25/2+
| 25/2+
|
|
Line 478: Line 697:
| 203.977813(28)
| 203.977813(28)
| 11.22(10) h
| 11.22(10) h
| β<sup>+</sup>
| <sup>204</sup>Pb
| 6+
| 6+
|
|
Line 485: Line 706:
| colspan="3" style="text-indent:2em" | 805.5(3) keV
| colspan="3" style="text-indent:2em" | 805.5(3) keV
| 13.0(1) ms
| 13.0(1) ms
| IT
| <sup>204</sup>Bi
| 10-
| 10-
|
|
Line 492: Line 715:
| colspan="3" style="text-indent:2em" | 2833.4(11) keV
| colspan="3" style="text-indent:2em" | 2833.4(11) keV
| 1.07(3) ms
| 1.07(3) ms
|
|
| (17+)
| (17+)
|
|
Line 501: Line 726:
| 204.977389(8)
| 204.977389(8)
| 15.31(4) d
| 15.31(4) d
| β<sup>+</sup>
| <sup>205</sup>Pb
| 9/2-
| 9/2-
|
|
Line 510: Line 737:
| 205.978499(8)
| 205.978499(8)
| 6.243(3) d
| 6.243(3) d
| β<sup>+</sup>
| <sup>206</sup>Pb
| 6(+)
| 6(+)
|
|
Line 517: Line 746:
| colspan="3" style="text-indent:2em" | 59.897(17) keV
| colspan="3" style="text-indent:2em" | 59.897(17) keV
| 7.7(2) µs
| 7.7(2) µs
|
|
| (4+)
| (4+)
|
|
Line 524: Line 755:
| colspan="3" style="text-indent:2em" | 1044.8(5) keV
| colspan="3" style="text-indent:2em" | 1044.8(5) keV
| 890(10) µs
| 890(10) µs
|
|
| (10-)
| (10-)
|
|
Line 533: Line 766:
| 206.9784707(26)
| 206.9784707(26)
| 32.9(14) a
| 32.9(14) a
| β<sup>+</sup>
| <sup>207</sup>Pb
| 9/2-
| 9/2-
|
|
Line 540: Line 775:
| colspan="3" style="text-indent:2em" | 2101.49(16) keV
| colspan="3" style="text-indent:2em" | 2101.49(16) keV
| 182(6) µs
| 182(6) µs
|
|
| 21/2+
| 21/2+
|
|
Line 549: Line 786:
| 207.9797422(25)
| 207.9797422(25)
| 3.68(4)E+5 a
| 3.68(4)E+5 a
| β<sup>+</sup>
| <sup>208</sup>Pb
| (5)+
| (5)+
|
|
Line 556: Line 795:
| colspan="3" style="text-indent:2em" | 1571.1(4) keV
| colspan="3" style="text-indent:2em" | 1571.1(4) keV
| 2.58(4) ms
| 2.58(4) ms
| IT
| <sup>208</sup>Bi
| (10)-
| (10)-
|
|
Line 565: Line 806:
| 208.9803987(16)
| 208.9803987(16)
| '''1.9(2)E+19 a'''
| '''1.9(2)E+19 a'''
| α
| <sup>205</sup>Tl
| 9/2-
| 9/2-
| 1.0000
| 1.0000
|
|
|-
|-
| <sup>210</sup>Bi<ref group="n">Historically known as radium E</ref>
| rowspan=2|<sup>210</sup>Bi<ref group="n">Historically known as radium E</ref>
| style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 83
| style="text-align:right" | 127
| rowspan=2 style="text-align:right" | 127
| 209.9841204(16)
| rowspan=2|209.9841204(16)
| 5.012(5) d
| rowspan=2|5.012(5) d
| β<sup>-</sup>
| 1-
| <sup>210</sup>Po
|
| rowspan=2|1-
|
| rowspan=2|
| rowspan=2|
|-
| α (.000132%)
| <sup>206</sup>Tl
|-
|-
| style="text-indent:1em" | <sup>210m</sup>Bi
| style="text-indent:1em" | <sup>210m</sup>Bi
| colspan="3" style="text-indent:2em" | 271.31(11) keV
| colspan="3" style="text-indent:2em" | 271.31(11) keV
| 3.04(6)E+6 a
| 3.04(6)E+6 a
| α
| <sup>206</sup>Tl
| 9-
| 9-
|
|
|
|
|-
|-
| <sup>211</sup>Bi<ref group="n">Historically known as actinium C</ref>
| rowspan=2|<sup>211</sup>Bi<ref group="n">Historically known as actinium C</ref>
| style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 83
| style="text-align:right" | 128
| rowspan=2 style="text-align:right" | 128
| 210.987269(6)
| rowspan=2|210.987269(6)
| 2.14(2) min
| rowspan=2|2.14(2) min
| α (99.72%)
| 9/2-
| <sup>207</sup>Tl
|
| rowspan=2|9/2-
|
| rowspan=2|
| rowspan=2|
|-
| β<sup>-</sup> (.276%)
| <sup>211</sup>Po
|-
|-
| style="text-indent:1em" | <sup>211m</sup>Bi
| style="text-indent:1em" | <sup>211m</sup>Bi
| colspan="3" style="text-indent:2em" | 1257(10) keV
| colspan="3" style="text-indent:2em" | 1257(10) keV
| 1.4(3) µs
| 1.4(3) µs
| (25/2-)
|
|
|
|
|-
| (25/2-)
| <sup>212</sup>Bi<ref group="n">Historically known as thorium C</ref>
| style="text-align:right" | 83
| style="text-align:right" | 129
| 211.9912857(21)
| 60.55(6) min
| 1(-)
|
|
|
|
|-
|-
| rowspan=3|<sup>212</sup>Bi<ref group="n">Historically known as thorium C</ref>
| style="text-indent:1em" | <sup>212m1</sup>Bi
| colspan="3" style="text-indent:2em" | 250(30) keV
| rowspan=3 style="text-align:right" | 83
| rowspan=3 style="text-align:right" | 129
| 25.0(2) min
| rowspan=3|211.9912857(21)
| (9-)
| rowspan=3|60.55(6) min
|
| β<sup>-</sup> (64.05%)
|
| <sup>212</sup>Po
| rowspan=3|1(-)
| rowspan=3|
| rowspan=3|
|-
| α (35.94%)
| <sup>208</sup>Tl
|-
| β<sup>-</sup>, α (.014%)
| <sup>208</sup>Pb
|-
| rowspan=3 style="text-indent:1em" | <sup>212m1</sup>Bi
| rowspan=3 colspan="3" style="text-indent:2em" | 250(30) keV
| rowspan=3|25.0(2) min
| α (67%)
| <sup>208</sup>Tl
| rowspan=3|(9-)
| rowspan=3|
| rowspan=3|
|-
| β<sup>-</sup> (33%)
| <sup>212m</sup>Po
|-
| β<sup>-</sup>, α (.3%)
| <sup>208</sup>Pb
|-
|-
| style="text-indent:1em" | <sup>212m2</sup>Bi
| style="text-indent:1em" | <sup>212m2</sup>Bi
| colspan="3" style="text-indent:2em" | 2200(200)# keV
| colspan="3" style="text-indent:2em" | 2200(200)# keV
| 7.0(3) min
| 7.0(3) min
| >15
|
|
|
|
| >15
|-
| <sup>213</sup>Bi
| style="text-align:right" | 83
| style="text-align:right" | 130
| 212.994385(5)
| 45.59(6) min
| 9/2-
|
|
|
|
|-
|-
| rowspan=2|<sup>213</sup>Bi
| <sup>214</sup>Bi<ref group="n">Historically known as radium C</ref>
| style="text-align:right" | 83
| rowspan=2 style="text-align:right" | 83
| style="text-align:right" | 131
| rowspan=2 style="text-align:right" | 130
| rowspan=2|212.994385(5)
| 213.998712(12)
| 19.9(4) min
| rowspan=2|45.59(6) min
| β<sup>-</sup> (97.91%)
| 1-
| <sup>213</sup>Po
|
| rowspan=2|9/2-
|
| rowspan=2|
| rowspan=2|
|-
| α (2.09%)
| <sup>209</sup>Tl
|-
| rowspan=3|<sup>214</sup>Bi<ref group="n">Historically known as radium C</ref>
| rowspan=3 style="text-align:right" | 83
| rowspan=3 style="text-align:right" | 131
| rowspan=3|213.998712(12)
| rowspan=3|19.9(4) min
| β<sup>-</sup> (99.97%)
| <sup>214</sup>Po
| rowspan=3|1-
| rowspan=3|
| rowspan=3|
|-
| α (.021%)
| <sup>210</sup>Tl
|-
| β<sup>-</sup>, α (.003%)
| <sup>210</sup>Pb
|-
|-
| <sup>215</sup>Bi
| <sup>215</sup>Bi
Line 647: Line 935:
| 215.001770(16)
| 215.001770(16)
| 7.6(2) min
| 7.6(2) min
| β<sup>-</sup>
| <sup>215</sup>Po
| (9/2-)
| (9/2-)
|
|
Line 654: Line 944:
| colspan="3" style="text-indent:2em" | 1347.5(25) keV
| colspan="3" style="text-indent:2em" | 1347.5(25) keV
| 36.4(25) min
| 36.4(25) min
|
|
| (25/2-)
| (25/2-)
|
|
Line 663: Line 955:
| 216.006306(12)
| 216.006306(12)
| 2.17(5) min
| 2.17(5) min
| β<sup>-</sup>
| <sup>216</sup>Po
| 1-#
| 1-#
|
|
Line 672: Line 966:
| 217.00947(21)#
| 217.00947(21)#
| 98.5(8) s
| 98.5(8) s
|
|
| 9/2-#
| 9/2-#
|
|
Line 681: Line 977:
| 218.01432(39)#
| 218.01432(39)#
| 33(1) s
| 33(1) s
|
|
| 1-#
| 1-#
|
|

Revision as of 12:43, 13 May 2011

Bismuth has no stable isotopes, but does have one very long-lived isotope, thus the standard atomic mass can be given. 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 x 1019 years, which is more than a billion (1000 million) times the age of the universe. Besides 209Bi, the most stable radioisotopes are 210mBi with a half life of 3.04 million years and 208Bi with a half-life of 368,000 years and 207Bi, with a half-life of 32.9 years. All other isotopes have half-lives under 1 year, most under a day

Isotopes of bismuth (Bi) that occur within the radioactive disintegration chains of actinium, radium, and thorium were known as:

  • radium E : 210Bi
  • actinium C : 211Bi
  • thorium C : 212Bi
  • radium C : 214Bi

Table

nuclide
symbol
Z(p) N(n)  
isotopic mass (u)
 
half-life[n 1] decay mode(s)[1] daughter
isotope(s)
nuclear
spin
representative
isotopic
composition
(mole fraction)
range of natural
variation
(mole fraction)
excitation energy
184Bi 83 101 184.00112(14)# 6.6(15) ms 3+#
184mBi 150(100)# keV 13(2) ms 10-#
185Bi 83 102 184.99763(6)# 2# ms p 184Pb 9/2-#
α (rare) 181Tl
185mBi 70(50)# keV 49(7) µs α 181Tl 1/2+
p 184Pb
186Bi 83 103 185.99660(8) 14.8(7) ms α 182Tl (3+)
β+ (rare) 186Pb
186mBi 270(140)# keV 9.8(4) ms α 182Tl (10-)
β+ 186Pb
187Bi 83 104 186.993158(16) 32(3) ms α (50%) 183Tl 9/2-#
β+ (50%) 187Pb
187m1Bi 101(20) keV 320(70) µs 1/2+#
187m2Bi 252(1) keV 7(5) µs (13/2+)
188Bi 83 105 187.99227(5) 44(3) ms α 184Tl 3+#
β+ (rare) 188Pb
188mBi 210(140)# keV 220(40) ms α 184Tl (10-)
β+ (rare) 188Pb
189Bi 83 106 188.98920(6) 674(11) ms α (51%) 185Tl (9/2-)
β+ (49%) 189Pb
189m1Bi 181(6) keV 5.0(1) ms (1/2+)
189m2Bi 357(1) keV 880(50) ns (13/2+)
190Bi 83 107 189.9883(2) 6.3(1) s α (77%) 186Tl (3+)
β+ (30%) 190Pb
190m1Bi 420(180) keV 6.2(1) s α (70%) 186Tl (10-)
β+ (30%) 190Pb
190m2Bi 690(180) keV >500(100) ns 7+#
191Bi 83 108 190.985786(8) 12.3(3) s α (60%) 187Tl (9/2-)
β+ (40%) 191Pb
191mBi 240(4) keV 124(5) ms α (75%) 187Tl (1/2+)
β+ (25%) 191Pb
192Bi 83 109 191.98546(4) 34.6(9) s β+ 192Pb (3+)
α (18%) 188Tl
192mBi 150(30) keV 39.6(4) s β+ (90.8%) 192Pb (10-)
α (9.2%) 188Tl
193Bi 83 110 192.98296(1) 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 83 111 193.98283(5) 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 83 112 194.980651(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 83 114 196.978864(9) 9.33(50) min β+ (99.99%) 197Pb (9/2-)
α (.0001%) 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 83 115 197.97921(3) 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 83 116 198.977672(13) 27(1) min β+ 199Pb 9/2-
199m1Bi 667(4) keV 24.70(15) min β+ (98%) 199Pb (1/2+)
IT 199Bi
α (.01%) 195Tl
199m2Bi 1947(25) keV 0.10(3) µs (25/2+)
199m3Bi ~2547.0 keV 168(13) ns 29/2-
200Bi 83 117 199.978132(26) 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 83 118 200.977009(16) 108(3) min β+ (99.99%) 201Pb 9/2-
α (.0001%) 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 83 119 201.977742(22) 1.72(5) h β+ 202Pb 5(+#)
α (.00001%) 198Tl
202m1Bi 615(7) keV 3.04(6) µs (10#)-
202m2Bi 2607.1(5) keV 310(50) ns (17+)
203Bi 83 120 202.976876(23) 11.76(5) h β+ 203Pb 9/2-
α (.00001%) 199Tl
203m1Bi 1098.14(7) keV 303(5) ms IT 203Bi 1/2+
203m2Bi 2041.5(6) keV 194(30) ns 25/2+
204Bi 83 121 203.977813(28) 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 83 122 204.977389(8) 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 83 124 206.9784707(26) 32.9(14) a β+ 207Pb 9/2-
207mBi 2101.49(16) keV 182(6) µs 21/2+
208Bi 83 125 207.9797422(25) 3.68(4)E+5 a β+ 208Pb (5)+
208mBi 1571.1(4) keV 2.58(4) ms IT 208Bi (10)-
209Bi 83 126 208.9803987(16) 1.9(2)E+19 a α 205Tl 9/2- 1.0000
210Bi[n 2] 83 127 209.9841204(16) 5.012(5) d β- 210Po 1-
α (.000132%) 206Tl
210mBi 271.31(11) keV 3.04(6)E+6 a α 206Tl 9-
211Bi[n 3] 83 128 210.987269(6) 2.14(2) min α (99.72%) 207Tl 9/2-
β- (.276%) 211Po
211mBi 1257(10) keV 1.4(3) µs (25/2-)
212Bi[n 4] 83 129 211.9912857(21) 60.55(6) min β- (64.05%) 212Po 1(-)
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 >15
213Bi 83 130 212.994385(5) 45.59(6) min β- (97.91%) 213Po 9/2-
α (2.09%) 209Tl
214Bi[n 5] 83 131 213.998712(12) 19.9(4) min β- (99.97%) 214Po 1-
α (.021%) 210Tl
β-, α (.003%) 210Pb
215Bi 83 132 215.001770(16) 7.6(2) min β- 215Po (9/2-)
215mBi 1347.5(25) keV 36.4(25) min (25/2-)
216Bi 83 133 216.006306(12) 2.17(5) min β- 216Po 1-#
217Bi 83 134 217.00947(21)# 98.5(8) s 9/2-#
218Bi 83 135 218.01432(39)# 33(1) s 1-#
  1. ^ Bold for isotopes with half-lives longer than the age of the universe (nearly stable)
  2. ^ Historically known as radium E
  3. ^ Historically known as actinium C
  4. ^ Historically known as thorium C
  5. ^ Historically known as radium C

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

Template:Wikipedia-Books

References

  • Isotope masses from:
    • G. Audi, A. H. Wapstra, C. Thibault, J. Blachot and O. Bersillon (2003). "The NUBASE evaluation of nuclear and decay properties" (PDF). Nuclear Physics A. 729: 3–128. doi:10.1016/j.nuclphysa.2003.11.001.{{cite journal}}: CS1 maint: multiple names: authors list (link)
  • Isotopic compositions and standard atomic masses from:
  • Half-life, spin, and isomer data selected from the following sources. See editing notes on this article's talk page.