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Isotopes of thallium: Difference between revisions

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Added info from http://www.nucleonica.net/unc.aspx
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Thallium-202 (half life 12.23 days) can be made in a cyclotron<ref>[http://www.eh.doe.gov/ohre/roadmap/histories/0472/0472d.html Thallium Research] from [[United States Department of Energy|Department of Energy]]</ref> while thallium-204 (half life 3.78 years) is made by the [[neutron activation]] of stable thallium in a [[nuclear reactor]].<ref>[http://www-pub.iaea.org/MTCD/publications/PDF/te_1340_web.pdf Manual for reactor produced radioisotopes] from the [[International Atomic Energy Agency]]</ref>
Thallium-202 (half life 12.23 days) can be made in a cyclotron<ref>[http://www.eh.doe.gov/ohre/roadmap/histories/0472/0472d.html Thallium Research] from [[United States Department of Energy|Department of Energy]]</ref> while thallium-204 (half life 3.78 years) is made by the [[neutron activation]] of stable thallium in a [[nuclear reactor]].<ref>[http://www-pub.iaea.org/MTCD/publications/PDF/te_1340_web.pdf Manual for reactor produced radioisotopes] from the [[International Atomic Energy Agency]]</ref>

Standard atomic mass: 204.3833(2) [[unified atomic mass unit|u]]


Isotopes of thallium occurring within the radioactive [[disintegration chain]]s of [[actinium]], [[radium]] and [[thorium]] were known as:
Isotopes of thallium occurring within the radioactive [[disintegration chain]]s of [[actinium]], [[radium]] and [[thorium]] were known as:
Line 11: Line 9:
* ''radium C<sup>II</sup>'' : <sup>210</sup>Tl
* ''radium C<sup>II</sup>'' : <sup>210</sup>Tl


Standard atomic mass: 204.3833(2) [[unified atomic mass unit|u]]

==Thallium-203==
'''Thallium-203''' is an [[isotope]] of [[thallium]].

atomic mass: 202.9723291 u
binding energy: 1600883 keV

spin: 1/2+
isotope is stable
possible parent nuclides: beta from Hg-203, EC from Pb-203

==Thallium-205==
'''Thallium-205''' is an [[isotope]] of [[thallium]].

It is stable and [[radiogenic]], produced from [[mercury-205]] by [[beta decay]], the extremely long half-lived [[bismuth-209]] by [[alpha decay]], or [[lead-205]] by [[electron capture]].

==Thallium-208==

'''Thallium-208''' is an [[isotope]] of [[thallium]].

It has a [[half-life]] of 3 minutes. It may be produced from [[mercury-208]] by beta decay or [[bismuth-212]] by alpha decay.


== Table ==
== Table ==
Line 40: Line 18:
! &nbsp;<br />isotopic mass (u)<br />&nbsp;
! &nbsp;<br />isotopic mass (u)<br />&nbsp;
! rowspan="2" | half-life
! rowspan="2" | half-life
! 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)
! rowspan="2" | range of natural<br />variation<br />(mole fraction)
! rowspan="2" | range of natural<br />variation<br />(mole fraction)
! rowspan="2" | other features
|-
|-
! colspan="3" | excitation energy
! colspan="3" | excitation energy
Line 52: Line 31:
| 176.00059(21)#
| 176.00059(21)#
| 5.2(+30-14) ms
| 5.2(+30-14) ms
| (3-,4-,5-)
|
|
|
|
| (3-,4-,5-)
|-
| <sup>177</sup>Tl
| style="text-align:right" | 81
| style="text-align:right" | 100
| 176.996427(27)
| 18(5) ms
| (1/2+)
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>177m</sup>Tl
| rowspan=2|<sup>177</sup>Tl
| colspan="3" style="text-indent:2em" | 807(18) keV
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 100
| 230(40) µs
| rowspan=2|176.996427(27)
| (11/2-)
| rowspan=2|18(5) ms
|
| [[proton emission|p]]
|
| <sup>176</sup>Hg
| rowspan=2|(1/2+)
| rowspan=2|
| rowspan=2|
|-
|-
| [[alpha decay|α]] (rare)
| <sup>178</sup>Tl
| <sup>173</sup>Au
| style="text-align:right" | 81
| style="text-align:right" | 97
| 177.99490(12)#
| 255(10) ms
|
|
|
|-
|-
| rowspan=2 style="text-indent:1em" | <sup>177m</sup>Tl
| rowspan=2 colspan="3" style="text-indent:2em" | 807(18) keV
| rowspan=2|230(40) µs
| p
| <sup>176</sup>Hg
| rowspan=2|(11/2-)
| rowspan=2|
| rowspan=2|
|-
| α
| <sup>173</sup>Au
|-
| rowspan=2|<sup>178</sup>Tl
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 97
| rowspan=2|177.99490(12)#
| rowspan=2|255(10) ms
| α
| <sup>174</sup>Au
| rowspan=2|
| rowspan=2|
| rowspan=2|
|-
| p (rare)
| <sup>177</sup>Hg
|-
| rowspan=2|<sup>179</sup>Tl
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 98
| rowspan=2|178.99109(5)
| rowspan=2|270(30) ms
| α
| <sup>175</sup>Au
| rowspan=2|(1/2+)
| rowspan=2|
| rowspan=2|
|-
| p (rare)
| <sup>178</sup>Hg
|-
| rowspan=2 style="text-indent:1em" | <sup>179m</sup>Tl
| rowspan=2 colspan="3" style="text-indent:2em" | 860(30)# keV
| rowspan=2|1.60(16) ms
| α
| <sup>175</sup>Au
| rowspan=2|(9/2-)
| rowspan=2|
| rowspan=2|
|-
| [[Isomeric transition|IT]] (rare)
| <sup>179</sup>Tl
| <sup>179</sup>Tl
| style="text-align:right" | 81
| style="text-align:right" | 98
| 178.99109(5)
| 270(30) ms
| (1/2+)
|
|
|-
|-
| style="text-indent:1em" | <sup>179m</sup>Tl
| rowspan=3|<sup>180</sup>Tl
| colspan="3" style="text-indent:2em" | 860(30)# keV
| rowspan=3 style="text-align:right" | 81
| rowspan=3 style="text-align:right" | 99
| 1.60(16) ms
| rowspan=3|179.98991(13)#
| (9/2-)
| rowspan=3|1.5(2) s
|
| α (75%)
|
| <sup>176</sup>Au
| rowspan=3|
| rowspan=3|
| rowspan=3|
|-
|-
| <sup>180</sup>Tl
| [[beta decay|β<sup>+</sup>]] (25%)
| <sup>176</sup>Hg
| style="text-align:right" | 81
| style="text-align:right" | 99
| 179.98991(13)#
| 1.5(2) s
|
|
|
|-
|-
| <sup>181</sup>Tl
| β<sup>+</sup>, [[Spontaneous Fission|SF]] (.0001%)
| <sup>100</sup>Ru, <sup>80</sup>Kr<ref>http://www.scientificamerican.com/article.cfm?id=mercury-serves-up-a-nuclear-su</ref>
| style="text-align:right" | 81
| style="text-align:right" | 100
| 180.986257(10)
| 3.2(3) s
| 1/2+#
|
|
|-
|-
| style="text-indent:1em" | <sup>181m</sup>Tl
| rowspan=2|<sup>181</sup>Tl
| colspan="3" style="text-indent:2em" | 857(29) keV
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 100
| 1.7(4) ms
| rowspan=2|180.986257(10)
| 9/2-#
| rowspan=2|3.2(3) s
|
|
| α
| <sup>177</sup>Au
| rowspan=2|1/2+#
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>182</sup>Tl
| β<sup>+</sup>
| <sup>181</sup>Hg
| style="text-align:right" | 81
| style="text-align:right" | 101
| 181.98567(8)
| 2.0(3) s
| 2-#
|
|
|-
|-
| style="text-indent:1em" | <sup>182m1</sup>Tl
| rowspan=2 style="text-indent:1em" | <sup>181m</sup>Tl
| colspan="3" style="text-indent:2em" | 100(100)# keV
| rowspan=2 colspan="3" style="text-indent:2em" | 857(29) keV
| 2.9(5) s
| rowspan=2|1.7(4) ms
| (7+)
| α
| <sup>177</sup>Au
|
| rowspan=2|9/2-#
|
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup>
| <sup>181</sup>Hg
|-
| rowspan=2|<sup>182</sup>Tl
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 101
| rowspan=2|181.98567(8)
| rowspan=2|2.0(3) s
| β<sup>+</sup> (96%)
| <sup>182</sup>Hg
| rowspan=2|2-#
| rowspan=2|
| rowspan=2|
|-
| α (4%)
| <sup>178</sup>Au
|-
| rowspan=2 style="text-indent:1em" | <sup>182m1</sup>Tl
| rowspan=2 colspan="3" style="text-indent:2em" | 100(100)# keV
| rowspan=2|2.9(5) s
| α
| <sup>178</sup>Au
| rowspan=2|(7+)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (rare)
| <sup>182</sup>Hg
|-
|-
| style="text-indent:1em" | <sup>182m2</sup>Tl
| style="text-indent:1em" | <sup>182m2</sup>Tl
| colspan="3" style="text-indent:2em" | 600(140)# keV
| colspan="3" style="text-indent:2em" | 600(140)# keV
|
|
|
|
| 10-
| 10-
Line 145: Line 181:
|
|
|-
|-
| rowspan=2|<sup>183</sup>Tl
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 102
| rowspan=2|182.982193(10)
| rowspan=2|6.9(7) s
| β<sup>+</sup> (98%)
| <sup>183</sup>Hg
| rowspan=2|1/2+#
| rowspan=2|
| rowspan=2|
|-
| α (2%)
| <sup>179</sup>Au
|-
| rowspan=2 style="text-indent:1em" | <sup>183m1</sup>Tl
| rowspan=2 colspan="3" style="text-indent:2em" | 630(17) keV
| rowspan=2|53.3(3) ms
| IT (99.99%)
| <sup>183</sup>Tl
| <sup>183</sup>Tl
| rowspan=2|9/2-#
| style="text-align:right" | 81
| rowspan=2|
| style="text-align:right" | 102
| rowspan=2|
| 182.982193(10)
| 6.9(7) s
| 1/2+#
|
|
|-
|-
| α (.01%)
| style="text-indent:1em" | <sup>183m1</sup>Tl
| <sup>179</sup>Au
| colspan="3" style="text-indent:2em" | 630(17) keV
| 53.3(3) ms
| 9/2-#
|
|
|-
|-
| style="text-indent:1em" | <sup>183m2</sup>Tl
| style="text-indent:1em" | <sup>183m2</sup>Tl
| colspan="3" style="text-indent:2em" | 976.8(3) keV
| colspan="3" style="text-indent:2em" | 976.8(3) keV
| 1.48(10) µs
| 1.48(10) µs
|
|
| (13/2+)
| (13/2+)
|
|
Line 173: Line 221:
| 183.98187(5)
| 183.98187(5)
| 9.7(6) s
| 9.7(6) s
| β<sup>+</sup>
| <sup>184</sup>Hg
| 2-#
| 2-#
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>184m1</sup>Tl
| rowspan=2 style="text-indent:1em" | <sup>184m1</sup>Tl
| colspan="3" style="text-indent:2em" | 100(100)# keV
| rowspan=2 colspan="3" style="text-indent:2em" | 100(100)# keV
| 10# s
| rowspan=2|10# s
| β<sup>+</sup> (97.9%)
| 7+#
| <sup>184</sup>Hg
|
| rowspan=2|7+#
|
| rowspan=2|
| rowspan=2|
|-
| α (2.1%)
| <sup>180</sup>Au
|-
|-
| style="text-indent:1em" | <sup>184m2</sup>Tl
| style="text-indent:1em" | <sup>184m2</sup>Tl
| colspan="3" style="text-indent:2em" | 500(140)# keV
| colspan="3" style="text-indent:2em" | 500(140)# keV
| >20 ns
| >20 ns
|
|
| (10-)
| (10-)
|
|
|
|
|-
|-
| rowspan=2|<sup>185</sup>Tl
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 104
| rowspan=2|184.97879(6)
| rowspan=2|19.5(5) s
| α
| <sup>181</sup>Au
| rowspan=2|1/2+#
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup>
| <sup>185</sup>Hg
|-
| rowspan=3 style="text-indent:1em" | <sup>185m</sup>Tl
| rowspan=3 colspan="3" style="text-indent:2em" | 452.8(20) keV
| rowspan=3|1.93(8) s
| IT (99.99%)
| <sup>185</sup>Tl
| <sup>185</sup>Tl
| rowspan=3|9/2-#
| style="text-align:right" | 81
| rowspan=3|
| style="text-align:right" | 104
| rowspan=3|
| 184.97879(6)
| 19.5(5) s
| 1/2+#
|
|
|-
|-
| α (.01%)
| style="text-indent:1em" | <sup>185m</sup>Tl
| <sup>181</sup>Au
| colspan="3" style="text-indent:2em" | 452.8(20) keV
| 1.93(8) s
| 9/2-#
|
|
|-
|-
| <sup>186</sup>Tl
| β<sup>+</sup>
| <sup>185</sup>Hg
| style="text-align:right" | 81
|-
| style="text-align:right" | 105
| rowspan=2|<sup>186</sup>Tl
| 185.97833(20)
| rowspan=2 style="text-align:right" | 81
| 40# s
| rowspan=2 style="text-align:right" | 105
| (2-)
| rowspan=2|185.97833(20)
|
| rowspan=2|40# s
|
| β<sup>+</sup>
| <sup>186</sup>Hg
| rowspan=2|(2-)
| rowspan=2|
| rowspan=2|
|-
| α (.006%)
| <sup>182</sup>Au
|-
|-
| style="text-indent:1em" | <sup>186m1</sup>Tl
| style="text-indent:1em" | <sup>186m1</sup>Tl
| colspan="3" style="text-indent:2em" | 320(180) keV
| colspan="3" style="text-indent:2em" | 320(180) keV
| 27.5(10) s
| 27.5(10) s
| β<sup>+</sup>
| <sup>186</sup>Hg
| (7+)
| (7+)
|
|
Line 226: Line 303:
| colspan="3" style="text-indent:2em" | 690(180) keV
| colspan="3" style="text-indent:2em" | 690(180) keV
| 2.9(2) s
| 2.9(2) s
|
|
| (10-)
| (10-)
|
|
|
|
|-
|-
| rowspan=2|<sup>187</sup>Tl
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 106
| rowspan=2|186.975906(9)
| rowspan=2|~51 s
| β<sup>+</sup>
| <sup>187</sup>Hg
| rowspan=2|(1/2+)
| rowspan=2|
| rowspan=2|
|-
| α (rare)
| <sup>183</sup>Au
|-
| rowspan=3 style="text-indent:1em" | <sup>187m</sup>Tl
| rowspan=3 colspan="3" style="text-indent:2em" | 335(3) keV
| rowspan=3|15.60(12) s
| α
| <sup>183</sup>Au
| rowspan=3|(9/2-)
| rowspan=3|
| rowspan=3|
|-
| IT
| <sup>187</sup>Tl
| <sup>187</sup>Tl
| style="text-align:right" | 81
| style="text-align:right" | 106
| 186.975906(9)
| ~51 s
| (1/2+)
|
|
|-
|-
| style="text-indent:1em" | <sup>187m</sup>Tl
| β<sup>+</sup>
| <sup>187</sup>Hg
| colspan="3" style="text-indent:2em" | 335(3) keV
| 15.60(12) s
| (9/2-)
|
|
|-
|-
| <sup>188</sup>Tl
| <sup>188</sup>Tl
Line 251: Line 343:
| 187.97601(4)
| 187.97601(4)
| 71(2) s
| 71(2) s
| β<sup>+</sup>
| <sup>188</sup>Hg
| (2-)
| (2-)
|
|
Line 258: Line 352:
| colspan="3" style="text-indent:2em" | 40(30) keV
| colspan="3" style="text-indent:2em" | 40(30) keV
| 71(1) s
| 71(1) s
| β<sup>+</sup>
| <sup>188</sup>Hg
| (7+)
| (7+)
|
|
Line 265: Line 361:
| colspan="3" style="text-indent:2em" | 310(30) keV
| colspan="3" style="text-indent:2em" | 310(30) keV
| 41(4) ms
| 41(4) ms
|
|
| (9-)
| (9-)
|
|
Line 274: Line 372:
| 188.973588(12)
| 188.973588(12)
| 2.3(2) min
| 2.3(2) min
| β<sup>+</sup>
| <sup>189</sup>Hg
| (1/2+)
| (1/2+)
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>189m</sup>Tl
| rowspan=2 style="text-indent:1em" | <sup>189m</sup>Tl
| colspan="3" style="text-indent:2em" | 257.6(13) keV
| rowspan=2 colspan="3" style="text-indent:2em" | 257.6(13) keV
| 1.4(1) min
| rowspan=2|1.4(1) min
| β<sup>+</sup> (96%)
| (9/2-)
| <sup>189</sup>Hg
|
| rowspan=2|(9/2-)
|
| rowspan=2|
| rowspan=2|
|-
| IT (4%)
| <sup>189</sup>Tl
|-
|-
| <sup>190</sup>Tl
| <sup>190</sup>Tl
Line 290: Line 395:
| 189.97388(5)
| 189.97388(5)
| 2.6(3) min
| 2.6(3) min
| β<sup>+</sup>
| <sup>190</sup>Hg
| 2(-)
| 2(-)
|
|
Line 297: Line 404:
| colspan="3" style="text-indent:2em" | 130(90)# keV
| colspan="3" style="text-indent:2em" | 130(90)# keV
| 3.7(3) min
| 3.7(3) min
| β<sup>+</sup>
| <sup>190</sup>Hg
| 7(+#)
| 7(+#)
|
|
Line 304: Line 413:
| colspan="3" style="text-indent:2em" | 290(70)# keV
| colspan="3" style="text-indent:2em" | 290(70)# keV
| 750(40) µs
| 750(40) µs
|
|
| (8-)
| (8-)
|
|
Line 311: Line 422:
| colspan="3" style="text-indent:2em" | 410(70)# keV
| colspan="3" style="text-indent:2em" | 410(70)# keV
| >1 µs
| >1 µs
|
|
| 9-
| 9-
|
|
Line 320: Line 433:
| 190.971786(8)
| 190.971786(8)
| 20# min
| 20# min
| β<sup>+</sup>
| <sup>191</sup>Hg
| (1/2+)
| (1/2+)
|
|
Line 327: Line 442:
| colspan="3" style="text-indent:2em" | 297(7) keV
| colspan="3" style="text-indent:2em" | 297(7) keV
| 5.22(16) min
| 5.22(16) min
| β<sup>+</sup>
| <sup>191</sup>Hg
| 9/2(-)
| 9/2(-)
|
|
Line 336: Line 453:
| 191.97223(3)
| 191.97223(3)
| 9.6(4) min
| 9.6(4) min
| β<sup>+</sup>
| <sup>192</sup>Hg
| (2-)
| (2-)
|
|
Line 343: Line 462:
| colspan="3" style="text-indent:2em" | 160(50) keV
| colspan="3" style="text-indent:2em" | 160(50) keV
| 10.8(2) min
| 10.8(2) min
| β<sup>+</sup>
| <sup>192</sup>Hg
| (7+)
| (7+)
|
|
Line 350: Line 471:
| colspan="3" style="text-indent:2em" | 407(54) keV
| colspan="3" style="text-indent:2em" | 407(54) keV
| 296(5) ns
| 296(5) ns
|
|
| (8-)
| (8-)
|
|
Line 359: Line 482:
| 192.97067(12)
| 192.97067(12)
| 21.6(8) min
| 21.6(8) min
| β<sup>+</sup>
| <sup>193</sup>Hg
| 1/2(+#)
| 1/2(+#)
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>193m</sup>Tl
| rowspan=2 style="text-indent:1em" | <sup>193m</sup>Tl
| colspan="3" style="text-indent:2em" | 369(4) keV
| rowspan=2 colspan="3" style="text-indent:2em" | 369(4) keV
| 2.11(15) min
| rowspan=2|2.11(15) min
| IT (75%)
| 9/2-
| <sup>193</sup>Tl
|
| rowspan=2|9/2-
|
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>194</sup>Tl
| β<sup>+</sup> (25%)
| <sup>193</sup>Hg
| style="text-align:right" | 81
|-
| style="text-align:right" | 113
| rowspan=2|<sup>194</sup>Tl
| 193.97120(15)
| rowspan=2 style="text-align:right" | 81
| 33.0(5) min
| rowspan=2 style="text-align:right" | 113
| 2-
| rowspan=2|193.97120(15)
|
| rowspan=2|33.0(5) min
|
| β<sup>+</sup>
| <sup>194</sup>Hg
| rowspan=2|2-
| rowspan=2|
| rowspan=2|
|-
| α (1E-7%)
| <sup>190</sup>Au
|-
|-
| style="text-indent:1em" | <sup>194m</sup>Tl
| style="text-indent:1em" | <sup>194m</sup>Tl
| colspan="3" style="text-indent:2em" | 300(200)# keV
| colspan="3" style="text-indent:2em" | 300(200)# keV
| 32.8(2) min
| 32.8(2) min
| β<sup>+</sup>
| <sup>194</sup>Hg
| (7+)
| (7+)
|
|
Line 391: Line 528:
| 194.969774(15)
| 194.969774(15)
| 1.16(5) h
| 1.16(5) h
| β<sup>+</sup>
| <sup>195</sup>Hg
| 1/2+
| 1/2+
|
|
Line 398: Line 537:
| colspan="3" style="text-indent:2em" | 482.63(17) keV
| colspan="3" style="text-indent:2em" | 482.63(17) keV
| 3.6(4) s
| 3.6(4) s
| IT
| <sup>195</sup>Tl
| 9/2-
| 9/2-
|
|
Line 407: Line 548:
| 195.970481(13)
| 195.970481(13)
| 1.84(3) h
| 1.84(3) h
| β<sup>+</sup>
| <sup>196</sup>Hg
| 2-
| 2-
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>196m</sup>Tl
| rowspan=2 style="text-indent:1em" | <sup>196m</sup>Tl
| colspan="3" style="text-indent:2em" | 394.2(5) keV
| rowspan=2 colspan="3" style="text-indent:2em" | 394.2(5) keV
| 1.41(2) h
| rowspan=2|1.41(2) h
| β<sup>+</sup> (95.5%)
| (7+)
| <sup></sup>Hg
|
| rowspan=2|(7+)
|
| rowspan=2|
| rowspan=2|
|-
| IT (4.5%)
| <sup>196</sup>Tl
|-
|-
| <sup>197</sup>Tl
| <sup>197</sup>Tl
Line 423: Line 571:
| 196.969575(18)
| 196.969575(18)
| 2.84(4) h
| 2.84(4) h
| β<sup>+</sup>
| <sup>197</sup>Hg
| 1/2+
| 1/2+
|
|
Line 430: Line 580:
| colspan="3" style="text-indent:2em" | 608.22(8) keV
| colspan="3" style="text-indent:2em" | 608.22(8) keV
| 540(10) ms
| 540(10) ms
| IT
| <sup>197</sup>Tl
| 9/2-
| 9/2-
|
|
Line 439: Line 591:
| 197.97048(9)
| 197.97048(9)
| 5.3(5) h
| 5.3(5) h
| β<sup>+</sup>
| <sup>198</sup>Hg
| 2-
| 2-
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>198m1</sup>Tl
| rowspan=2 style="text-indent:1em" | <sup>198m1</sup>Tl
| colspan="3" style="text-indent:2em" | 543.5(4) keV
| rowspan=2 colspan="3" style="text-indent:2em" | 543.5(4) keV
| 1.87(3) h
| rowspan=2|1.87(3) h
| β<sup>+</sup> (54%)
| 7+
| <sup>198</sup>Hg
|
| rowspan=2|7+
|
| rowspan=2|
| rowspan=2|
|-
| IT (46%)
| <sup>198</sup>Tl
|-
|-
| style="text-indent:1em" | <sup>198m2</sup>Tl
| style="text-indent:1em" | <sup>198m2</sup>Tl
| colspan="3" style="text-indent:2em" | 687.2(5) keV
| colspan="3" style="text-indent:2em" | 687.2(5) keV
| 150(40) ns
| 150(40) ns
|
|
| (5+)
| (5+)
|
|
Line 460: Line 621:
| colspan="3" style="text-indent:2em" | 742.3(4) keV
| colspan="3" style="text-indent:2em" | 742.3(4) keV
| 32.1(10) ms
| 32.1(10) ms
|
|
| (10-)#
| (10-)#
|
|
Line 469: Line 632:
| 198.96988(3)
| 198.96988(3)
| 7.42(8) h
| 7.42(8) h
| β<sup>+</sup>
| <sup>199</sup>Hg
| 1/2+
| 1/2+
|
|
Line 476: Line 641:
| colspan="3" style="text-indent:2em" | 749.7(3) keV
| colspan="3" style="text-indent:2em" | 749.7(3) keV
| 28.4(2) ms
| 28.4(2) ms
| IT
| <sup>199</sup>Tl
| 9/2-
| 9/2-
|
|
Line 485: Line 652:
| 199.970963(6)
| 199.970963(6)
| 26.1(1) h
| 26.1(1) h
| β<sup>+</sup>
| <sup>200</sup>Hg
| 2-
| 2-
|
|
Line 492: Line 661:
| colspan="3" style="text-indent:2em" | 753.6(2) keV
| colspan="3" style="text-indent:2em" | 753.6(2) keV
| 34.3(10) ms
| 34.3(10) ms
| IT
| <sup>200</sup>Tl
| 7+
| 7+
|
|
Line 499: Line 670:
| colspan="3" style="text-indent:2em" | 762.0(2) keV
| colspan="3" style="text-indent:2em" | 762.0(2) keV
| 0.33(5) µs
| 0.33(5) µs
|
|
| 5+
| 5+
|
|
|
|
|-
|-
| <sup>201</sup>Tl
| <sup>201</sup>Tl<ref group="n">Main isotope used in [[scintigraphy]]</ref>
| style="text-align:right" | 81
| style="text-align:right" | 81
| style="text-align:right" | 120
| style="text-align:right" | 120
| 200.970819(16)
| 200.970819(16)
| 72.912(17) h
| 72.912(17) h
| [[Electron capture|EC]]
| <sup>201</sup>Hg
| 1/2+
| 1/2+
|
|
|
|
| Main isotope used in [[scintigraphy]]
|-
|-
| style="text-indent:1em" | <sup>201m</sup>Tl
| style="text-indent:1em" | <sup>201m</sup>Tl
| colspan="3" style="text-indent:2em" | 919.50(9) keV
| colspan="3" style="text-indent:2em" | 919.50(9) keV
| 2.035(7) ms
| 2.035(7) ms
| IT
| <sup>201</sup>Tl
| (9/2-)
| (9/2-)
|
|
Line 525: Line 701:
| 201.972106(16)
| 201.972106(16)
| 12.23(2) d
| 12.23(2) d
| β<sup>+</sup>
| <sup>202</sup>Hg
| 2-
| 2-
|
|
Line 532: Line 710:
| colspan="3" style="text-indent:2em" | 950.19(10) keV
| colspan="3" style="text-indent:2em" | 950.19(10) keV
| 572(7) µs
| 572(7) µs
|
|
| 7+
| 7+
|
|
Line 540: Line 720:
| style="text-align:right" | 122
| style="text-align:right" | 122
| 202.9723442(14)
| 202.9723442(14)
| colspan=3 align=center|'''Stable'''<ref group="n">Believed to undergo α decay to <sup>199</sup>Au</ref>
| STABLE
| 1/2+
| 1/2+
| 0.2952(1)
| 0.2952(1)
| 0.29494-0.29528
| 0.29494-0.29528
| One of the two stable thallium isotopes
|-
|-
| style="text-indent:1em" | <sup>203m</sup>Tl
| style="text-indent:1em" | <sup>203m</sup>Tl
| colspan="3" style="text-indent:2em" | 3400(300) keV
| colspan="3" style="text-indent:2em" | 3400(300) keV
| 7.7(5) µs
| 7.7(5) µs
| (25/2+)
|
|
|
|
| (25/2+)
|-
| <sup>204</sup>Tl
| style="text-align:right" | 81
| style="text-align:right" | 123
| 203.9738635(13)
| 3.78(2) a
| 2-
|
|
|
|
|-
| Most stable thallium radioisotope
| rowspan=2|<sup>204</sup>Tl
| rowspan=2 style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 123
| rowspan=2|203.9738635(13)
| rowspan=2|3.78(2) a
| β<sup>-</sup> (97.1%)
| <sup>204</sup>Pb
| rowspan=2|2-
| rowspan=2|
| rowspan=2|
|-
| EC (2.9%)
| <sup>204</sup>Hg
|-
|-
| style="text-indent:1em" | <sup>204m1</sup>Tl
| style="text-indent:1em" | <sup>204m1</sup>Tl
| colspan="3" style="text-indent:2em" | 1104.0(4) keV
| colspan="3" style="text-indent:2em" | 1104.0(4) keV
| 63(2) µs
| 63(2) µs
|
|
| (7)+
| (7)+
|
|
Line 573: Line 760:
| colspan="3" style="text-indent:2em" | 2500(500) keV
| colspan="3" style="text-indent:2em" | 2500(500) keV
| 2.6(2) µs
| 2.6(2) µs
|
|
| (12-)
| (12-)
|
|
Line 580: Line 769:
| colspan="3" style="text-indent:2em" | 3500(500) keV
| colspan="3" style="text-indent:2em" | 3500(500) keV
| 1.6(2) µs
| 1.6(2) µs
|
|
| (20+)
| (20+)
|
|
|
|
|-
|-
| [[Thallium-205|<sup>205</sup>Tl]]
| <sup>205</sup>Tl
| style="text-align:right" | 81
| style="text-align:right" | 81
| style="text-align:right" | 124
| style="text-align:right" | 124
| 204.9744275(14)
| 204.9744275(14)
| colspan=3 align=center|'''Stable'''<ref group="n">Believed to undergo α decay to <sup>201</sup>Au</ref>
| STABLE
| 1/2+
| 1/2+
| 0.7048(1)
| 0.7048(1)
| 0.70472-0.70506
| 0.70472-0.70506
| One of the two stable thallium isotopes
|-
|-
| style="text-indent:1em" | <sup>205m1</sup>Tl
| style="text-indent:1em" | <sup>205m1</sup>Tl
| colspan="3" style="text-indent:2em" | 3290.63(17) keV
| colspan="3" style="text-indent:2em" | 3290.63(17) keV
| 2.6(2) µs
| 2.6(2) µs
|
|
| 25/2+
| 25/2+
|
|
Line 604: Line 796:
| colspan="3" style="text-indent:2em" | 4835.6(15) keV
| colspan="3" style="text-indent:2em" | 4835.6(15) keV
| 235(10) ns
| 235(10) ns
|
|
| (35/2-)
| (35/2-)
|
|
|
|
|-
|-
| <sup>206</sup>Tl
| <sup>206</sup>Tl<ref group="n">Historic name radium E<sup>II</sup></ref>
| style="text-align:right" | 81
| style="text-align:right" | 81
| style="text-align:right" | 125
| style="text-align:right" | 125
| 205.9761103(15)
| 205.9761103(15)
| 4.200(17) min
| 4.200(17) min
| β<sup>-</sup>
| <sup>206</sup>Pb
| 0-
| 0-
|
|
Line 620: Line 816:
| colspan="3" style="text-indent:2em" | 2643.11(19) keV
| colspan="3" style="text-indent:2em" | 2643.11(19) keV
| 3.74(3) min
| 3.74(3) min
| IT
| <sup>206</sup>Tl
| (12-)
| (12-)
|
|
|
|
|-
|-
| <sup>207</sup>Tl
| <sup>207</sup>Tl<ref group="n">Historic name actinium C<sup>II</sup></ref>
| style="text-align:right" | 81
| style="text-align:right" | 81
| style="text-align:right" | 126
| style="text-align:right" | 126
| 206.977419(6)
| 206.977419(6)
| 4.77(2) min
| 4.77(2) min
| β<sup>-</sup>
| <sup>207</sup>Pb
| 1/2+
| 1/2+
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>207m</sup>Tl
| rowspan=2 style="text-indent:1em" | <sup>207m</sup>Tl
| colspan="3" style="text-indent:2em" | 1348.1(3) keV
| rowspan=2 colspan="3" style="text-indent:2em" | 1348.1(3) keV
| 1.33(11) s
| rowspan=2|1.33(11) s
| IT (99.9%)
| 11/2-
| <sup>207</sup>Tl
|
| rowspan=2|11/2-
|
| rowspan=2|
| rowspan=2|
|-
| β<sup>-</sup> (.1%)
| <sup>207</sup>Pb
|-
|-
| <sup>208</sup>Tl<ref group="n">Historic name thorium C<sup>II</sup></ref>
| [[Thallium-208|<sup>208</sup>Tl]]
| style="text-align:right" | 81
| style="text-align:right" | 81
| style="text-align:right" | 127
| style="text-align:right" | 127
| 207.9820187(21)
| 207.9820187(21)
| 3.053(4) min
| 3.053(4) min
| β<sup>-</sup>
| <sup>208</sup>Pb
| 5(+)
| 5(+)
|
|
Line 654: Line 861:
| 208.985359(8)
| 208.985359(8)
| 2.161(7) min
| 2.161(7) min
| β<sup>-</sup>
| <sup>209</sup>Pb
| (1/2+)
| (1/2+)
|
|
|
|
|-
|-
| <sup>210</sup>Tl
| rowspan=2|<sup>210</sup>Tl<ref group="n">Historic name radium C<sup>II</sup></ref>
| style="text-align:right" | 81
| rowspan=2 style="text-align:right" | 81
| style="text-align:right" | 129
| rowspan=2 style="text-align:right" | 129
| 209.990074(12)
| rowspan=2|209.990074(12)
| 1.30(3) min
| rowspan=2|1.30(3) min
| β<sup>-</sup> (99.991%)
| (5+)#
| <sup>210</sup>Pb
|
| rowspan=2|(5+)#
|
| rowspan=2|
| rowspan=2|
|-
| β<sup>-</sup>, [[neutron emission|n]] (.009%)
| <sup>209</sup>Pb
|-
|-
| <sup>211</sup>Tl
| <sup>211</sup>Tl
Line 671: Line 885:
| style="text-align:right" | 130
| style="text-align:right" | 130
| 210.99348(22)#
| 210.99348(22)#
| 1# min [>300 ns]
| 1# min<br>[>300 ns]
|
|
| 1/2+#
| 1/2+#
|
|
Line 680: Line 896:
| style="text-align:right" | 131
| style="text-align:right" | 131
| 211.99823(32)#
| 211.99823(32)#
| 30# s [>300 ns]
| 30# s<br>[>300 ns]
|
|
| 5+#
| 5+#
|
|
|
|
|}
|}
<references group="n" />


=== Notes ===
=== Notes ===

Revision as of 23:27, 12 May 2011

Thallium (Tl) has 25 isotopes which have atomic masses that range from 184 to 210. 203Tl and 205Tl are the only stable isotopes and 204Tl is the most stable radioisotope with a half-life of 3.78 years.

Thallium-202 (half life 12.23 days) can be made in a cyclotron[1] while thallium-204 (half life 3.78 years) is made by the neutron activation of stable thallium in a nuclear reactor.[2]

Isotopes of thallium occurring within the radioactive disintegration chains of actinium, radium and thorium were known as:

  • radium EII : 206Tl
  • actinium CII : 207Tl
  • thorium CII : 208Tl
  • radium CII : 210Tl

Standard atomic mass: 204.3833(2) u

Table

nuclide
symbol
Z(p) N(n)  
isotopic mass (u)
 
half-life decay mode(s)[3] daughter
isotope(s)
nuclear
spin
representative
isotopic
composition
(mole fraction)
range of natural
variation
(mole fraction)
excitation energy
176Tl 81 95 176.00059(21)# 5.2(+30-14) ms (3-,4-,5-)
177Tl 81 100 176.996427(27) 18(5) ms p 176Hg (1/2+)
α (rare) 173Au
177mTl 807(18) keV 230(40) µs p 176Hg (11/2-)
α 173Au
178Tl 81 97 177.99490(12)# 255(10) ms α 174Au
p (rare) 177Hg
179Tl 81 98 178.99109(5) 270(30) ms α 175Au (1/2+)
p (rare) 178Hg
179mTl 860(30)# keV 1.60(16) ms α 175Au (9/2-)
IT (rare) 179Tl
180Tl 81 99 179.98991(13)# 1.5(2) s α (75%) 176Au
β+ (25%) 176Hg
β+, SF (.0001%) 100Ru, 80Kr[4]
181Tl 81 100 180.986257(10) 3.2(3) s α 177Au 1/2+#
β+ 181Hg
181mTl 857(29) keV 1.7(4) ms α 177Au 9/2-#
β+ 181Hg
182Tl 81 101 181.98567(8) 2.0(3) s β+ (96%) 182Hg 2-#
α (4%) 178Au
182m1Tl 100(100)# keV 2.9(5) s α 178Au (7+)
β+ (rare) 182Hg
182m2Tl 600(140)# keV 10-
183Tl 81 102 182.982193(10) 6.9(7) s β+ (98%) 183Hg 1/2+#
α (2%) 179Au
183m1Tl 630(17) keV 53.3(3) ms IT (99.99%) 183Tl 9/2-#
α (.01%) 179Au
183m2Tl 976.8(3) keV 1.48(10) µs (13/2+)
184Tl 81 103 183.98187(5) 9.7(6) s β+ 184Hg 2-#
184m1Tl 100(100)# keV 10# s β+ (97.9%) 184Hg 7+#
α (2.1%) 180Au
184m2Tl 500(140)# keV >20 ns (10-)
185Tl 81 104 184.97879(6) 19.5(5) s α 181Au 1/2+#
β+ 185Hg
185mTl 452.8(20) keV 1.93(8) s IT (99.99%) 185Tl 9/2-#
α (.01%) 181Au
β+ 185Hg
186Tl 81 105 185.97833(20) 40# s β+ 186Hg (2-)
α (.006%) 182Au
186m1Tl 320(180) keV 27.5(10) s β+ 186Hg (7+)
186m2Tl 690(180) keV 2.9(2) s (10-)
187Tl 81 106 186.975906(9) ~51 s β+ 187Hg (1/2+)
α (rare) 183Au
187mTl 335(3) keV 15.60(12) s α 183Au (9/2-)
IT 187Tl
β+ 187Hg
188Tl 81 107 187.97601(4) 71(2) s β+ 188Hg (2-)
188m1Tl 40(30) keV 71(1) s β+ 188Hg (7+)
188m2Tl 310(30) keV 41(4) ms (9-)
189Tl 81 108 188.973588(12) 2.3(2) min β+ 189Hg (1/2+)
189mTl 257.6(13) keV 1.4(1) min β+ (96%) 189Hg (9/2-)
IT (4%) 189Tl
190Tl 81 109 189.97388(5) 2.6(3) min β+ 190Hg 2(-)
190m1Tl 130(90)# keV 3.7(3) min β+ 190Hg 7(+#)
190m2Tl 290(70)# keV 750(40) µs (8-)
190m3Tl 410(70)# keV >1 µs 9-
191Tl 81 110 190.971786(8) 20# min β+ 191Hg (1/2+)
191mTl 297(7) keV 5.22(16) min β+ 191Hg 9/2(-)
192Tl 81 111 191.97223(3) 9.6(4) min β+ 192Hg (2-)
192m1Tl 160(50) keV 10.8(2) min β+ 192Hg (7+)
192m2Tl 407(54) keV 296(5) ns (8-)
193Tl 81 112 192.97067(12) 21.6(8) min β+ 193Hg 1/2(+#)
193mTl 369(4) keV 2.11(15) min IT (75%) 193Tl 9/2-
β+ (25%) 193Hg
194Tl 81 113 193.97120(15) 33.0(5) min β+ 194Hg 2-
α (1E-7%) 190Au
194mTl 300(200)# keV 32.8(2) min β+ 194Hg (7+)
195Tl 81 114 194.969774(15) 1.16(5) h β+ 195Hg 1/2+
195mTl 482.63(17) keV 3.6(4) s IT 195Tl 9/2-
196Tl 81 115 195.970481(13) 1.84(3) h β+ 196Hg 2-
196mTl 394.2(5) keV 1.41(2) h β+ (95.5%) Hg (7+)
IT (4.5%) 196Tl
197Tl 81 116 196.969575(18) 2.84(4) h β+ 197Hg 1/2+
197mTl 608.22(8) keV 540(10) ms IT 197Tl 9/2-
198Tl 81 117 197.97048(9) 5.3(5) h β+ 198Hg 2-
198m1Tl 543.5(4) keV 1.87(3) h β+ (54%) 198Hg 7+
IT (46%) 198Tl
198m2Tl 687.2(5) keV 150(40) ns (5+)
198m3Tl 742.3(4) keV 32.1(10) ms (10-)#
199Tl 81 118 198.96988(3) 7.42(8) h β+ 199Hg 1/2+
199mTl 749.7(3) keV 28.4(2) ms IT 199Tl 9/2-
200Tl 81 119 199.970963(6) 26.1(1) h β+ 200Hg 2-
200m1Tl 753.6(2) keV 34.3(10) ms IT 200Tl 7+
200m2Tl 762.0(2) keV 0.33(5) µs 5+
201Tl[n 1] 81 120 200.970819(16) 72.912(17) h EC 201Hg 1/2+
201mTl 919.50(9) keV 2.035(7) ms IT 201Tl (9/2-)
202Tl 81 121 201.972106(16) 12.23(2) d β+ 202Hg 2-
202mTl 950.19(10) keV 572(7) µs 7+
203Tl 81 122 202.9723442(14) Stable[n 2] 1/2+ 0.2952(1) 0.29494-0.29528
203mTl 3400(300) keV 7.7(5) µs (25/2+)
204Tl 81 123 203.9738635(13) 3.78(2) a β- (97.1%) 204Pb 2-
EC (2.9%) 204Hg
204m1Tl 1104.0(4) keV 63(2) µs (7)+
204m2Tl 2500(500) keV 2.6(2) µs (12-)
204m3Tl 3500(500) keV 1.6(2) µs (20+)
205Tl 81 124 204.9744275(14) Stable[n 3] 1/2+ 0.7048(1) 0.70472-0.70506
205m1Tl 3290.63(17) keV 2.6(2) µs 25/2+
205m2Tl 4835.6(15) keV 235(10) ns (35/2-)
206Tl[n 4] 81 125 205.9761103(15) 4.200(17) min β- 206Pb 0-
206mTl 2643.11(19) keV 3.74(3) min IT 206Tl (12-)
207Tl[n 5] 81 126 206.977419(6) 4.77(2) min β- 207Pb 1/2+
207mTl 1348.1(3) keV 1.33(11) s IT (99.9%) 207Tl 11/2-
β- (.1%) 207Pb
208Tl[n 6] 81 127 207.9820187(21) 3.053(4) min β- 208Pb 5(+)
209Tl 81 128 208.985359(8) 2.161(7) min β- 209Pb (1/2+)
210Tl[n 7] 81 129 209.990074(12) 1.30(3) min β- (99.991%) 210Pb (5+)#
β-, n (.009%) 209Pb
211Tl 81 130 210.99348(22)# 1# min
[>300 ns]
1/2+#
212Tl 81 131 211.99823(32)# 30# s
[>300 ns]
5+#
  1. ^ Main isotope used in scintigraphy
  2. ^ Believed to undergo α decay to 199Au
  3. ^ Believed to undergo α decay to 201Au
  4. ^ Historic name radium EII
  5. ^ Historic name actinium CII
  6. ^ Historic name thorium CII
  7. ^ Historic name radium CII

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.

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.