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Isotopes of platinum: Difference between revisions

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Table: Added info from http://www.nucleonica.net/unc.aspx
Line 10: Line 10:
! &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)
Line 21: Line 23:
| 165.99486(54)#
| 165.99486(54)#
| 300(100) µs
| 300(100) µs
|
|
| 0+
| 0+
|
|
Line 30: Line 34:
| 166.99298(44)#
| 166.99298(44)#
| 700(200) µs
| 700(200) µs
| 7/2-#
|
|
|
|
|-
| 7/2-#
| <sup>168</sup>Pt
| style="text-align:right" | 78
| style="text-align:right" | 90
| 167.98815(22)
| 2.00(18) ms
| 0+
|
|
|
|
|-
|-
| <sup>169</sup>Pt
| rowspan=2|<sup>168</sup>Pt
| style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 78
| style="text-align:right" | 91
| rowspan=2 style="text-align:right" | 90
| 168.98672(22)#
| rowspan=2|167.98815(22)
| 3.7(15) ms
| rowspan=2|2.00(18) ms
| [[alpha decay|α]]
| 3/2-#
| <sup>164</sup>Os
|
| rowspan=2|0+
|
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>170</sup>Pt
| [[beta decay|β<sup>+</sup>]] (rare)
| <sup>168</sup>Ir
| style="text-align:right" | 78
| style="text-align:right" | 92
| 169.982495(20)
| 14.0(2) ms
| 0+
|
|
|-
|-
| <sup>171</sup>Pt
| rowspan=2|<sup>169</sup>Pt
| style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 78
| style="text-align:right" | 93
| rowspan=2 style="text-align:right" | 91
| rowspan=2|168.98672(22)#
| 170.98124(9)
| 51(2) ms
| rowspan=2|3.7(15) ms
| 3/2-#
| α
| <sup>165</sup>Os
|
| rowspan=2|3/2-#
|
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>172</sup>Pt
| β<sup>+</sup> (rare)
| <sup>169</sup>Ir
| style="text-align:right" | 78
| style="text-align:right" | 94
| 171.977347(14)
| 98.4(24) ms
| 0+
|
|
|-
|-
| <sup>173</sup>Pt
| rowspan=2|<sup>170</sup>Pt
| style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 78
| style="text-align:right" | 95
| rowspan=2 style="text-align:right" | 92
| rowspan=2|169.982495(20)
| 172.97644(6)
| 365(7) ms
| rowspan=2|14.0(2) ms
| α (98%)
| 5/2-#
| <sup>166</sup>Os
|
| rowspan=2|0+
|
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>174</sup>Pt
| β<sup>+</sup> (2%)
| <sup>170</sup>Ir
| style="text-align:right" | 78
| style="text-align:right" | 96
| 173.972819(13)
| 0.889(17) s
| 0+
|
|
|-
|-
| <sup>175</sup>Pt
| rowspan=2|<sup>171</sup>Pt
| style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 78
| style="text-align:right" | 97
| rowspan=2 style="text-align:right" | 93
| rowspan=2|170.98124(9)
| 174.972421(20)
| 2.53(6) s
| rowspan=2|51(2) ms
| α (99%)
| 5/2-#
| <sup>167</sup>Os
|
| rowspan=2|3/2-#
|
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>176</sup>Pt
| β<sup>+</sup> (1%)
| <sup>171</sup>Ir
| style="text-align:right" | 78
|-
| style="text-align:right" | 98
| rowspan=2|<sup>172</sup>Pt
| 175.968945(15)
| rowspan=2 style="text-align:right" | 78
| 6.33(15) s
| rowspan=2 style="text-align:right" | 94
| 0+
| rowspan=2|171.977347(14)
|
| rowspan=2|98.4(24) ms
|
| α (77%)
| <sup>168</sup>Os
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (23%)
| <sup>172</sup>Ir
|-
| rowspan=2|<sup>173</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 95
| rowspan=2|172.97644(6)
| rowspan=2|365(7) ms
| α (84%)
| <sup>169</sup>Os
| rowspan=2|5/2-#
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>177</sup>Pt
| β<sup>+</sup> (16%)
| <sup>173</sup>Ir
| style="text-align:right" | 78
|-
| style="text-align:right" | 99
| rowspan=2|<sup>174</sup>Pt
| 176.968469(16)
| rowspan=2 style="text-align:right" | 78
| 10.6(4) s
| rowspan=2 style="text-align:right" | 96
| 5/2-
| rowspan=2|173.972819(13)
|
| rowspan=2|0.889(17) s
|
| α (83%)
| <sup>170</sup>Os
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (17%)
| <sup>174</sup>Ir
|-
| rowspan=2|<sup>175</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 97
| rowspan=2|174.972421(20)
| rowspan=2|2.53(6) s
| α (64%)
| <sup>171</sup>Os
| rowspan=2|5/2-#
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (36%)
| <sup>175</sup>Ir
|-
| rowspan=2|<sup>176</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 98
| rowspan=2|175.968945(15)
| rowspan=2|6.33(15) s
| β<sup>+</sup> (62%)
| <sup>176</sup>Ir
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (38%)
| <sup>172</sup>Os
|-
| rowspan=2|<sup>177</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 99
| rowspan=2|176.968469(16)
| rowspan=2|10.6(4) s
| β<sup>+</sup> (94.4%)
| <sup>177</sup>Ir
| rowspan=2|5/2-
| rowspan=2|
| rowspan=2|
|-
| α (5.6%)
| <sup>173</sup>Os
|-
|-
| style="text-indent:1em" | <sup>177m</sup>Pt
| style="text-indent:1em" | <sup>177m</sup>Pt
| colspan="3" style="text-indent:2em" | 147.4(4) keV
| colspan="3" style="text-indent:2em" | 147.4(4) keV
| 2.2(3) µs
| 2.2(3) µs
| 1/2-
|
|
|
|
|-
| <sup>178</sup>Pt
| style="text-align:right" | 78
| style="text-align:right" | 100
| 177.965649(12)
| 21.1(6) s
| 0+
|
|
|-
| <sup>179</sup>Pt
| style="text-align:right" | 78
| style="text-align:right" | 101
| 178.965363(10)
| 21.2(4) s
| 1/2-
| 1/2-
|
|
|
|
|-
|-
| <sup>180</sup>Pt
| rowspan=2|<sup>178</sup>Pt
| style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 78
| style="text-align:right" | 102
| rowspan=2 style="text-align:right" | 100
| 179.963031(12)
| rowspan=2|177.965649(12)
| 56(2) s
| rowspan=2|21.1(6) s
| β<sup>+</sup> (92.3%)
| 0+
| <sup>178</sup>Ir
|
| rowspan=2|0+
|
| rowspan=2|
| rowspan=2|
|-
|-
| α (7.7%)
| <sup>181</sup>Pt
| <sup>174</sup>Os
| style="text-align:right" | 78
| style="text-align:right" | 103
| 180.963097(16)
| 52.0(22) s
| 1/2-
|
|
|-
|-
| <sup>182</sup>Pt
| rowspan=2|<sup>179</sup>Pt
| style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 78
| style="text-align:right" | 104
| rowspan=2 style="text-align:right" | 101
| rowspan=2|178.965363(10)
| 181.961171(17)
| 2.2(1) min
| rowspan=2|21.2(4) s
| β<sup>+</sup> (99.76%)
| 0+
| <sup>179</sup>Ir
|
| rowspan=2|1/2-
|
| rowspan=2|
| rowspan=2|
|-
| α (0.24%)
| <sup>175</sup>Os
|-
| rowspan=2|<sup>180</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 102
| rowspan=2|179.963031(12)
| rowspan=2|56(2) s
| β<sup>+</sup> (99.7%)
| <sup>180</sup>Ir
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
|-
| α (0.3%)
| <sup>176</sup>Os
|-
| rowspan=2|<sup>181</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 103
| rowspan=2|180.963097(16)
| rowspan=2|52.0(22) s
| β<sup>+</sup> (99.93%)
| <sup>181</sup>Ir
| rowspan=2|1/2-
| rowspan=2|
| rowspan=2|
|-
| α (0.074%)
| <sup>177</sup>Os
|-
| rowspan=2|<sup>182</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 104
| rowspan=2|181.961171(17)
| rowspan=2|2.2(1) min
| β<sup>+</sup> (99.96%)
| <sup>182</sup>Ir
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (.038%)
| <sup>178</sup>Os
|-
| rowspan=2|<sup>183</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 105
| rowspan=2|182.961597(17)
| rowspan=2|6.5(10) min
| β<sup>+</sup> (99.99%)
| <sup>183</sup>Ir
| rowspan=2|1/2-
| rowspan=2|
| rowspan=2|
|-
| α (.0096%)
| <sup>179</sup>Os
|-
| rowspan=3 style="text-indent:1em" | <sup>183m1</sup>Pt
| rowspan=3 colspan="3" style="text-indent:2em" | 34.50(8) keV
| rowspan=3|43(5) s
| β<sup>+</sup> (99.99%)
| <sup>183</sup>Ir
| rowspan=3|(7/2)-
| rowspan=3|
| rowspan=3|
|-
| α (.0004%)
| <sup>179</sup>Os
|-
| [[Isomeric transition|IT]]
| <sup>183</sup>Pt
| <sup>183</sup>Pt
| style="text-align:right" | 78
| style="text-align:right" | 105
| 182.961597(17)
| 6.5(10) min
| 1/2-
|
|
|-
| style="text-indent:1em" | <sup>183m1</sup>Pt
| colspan="3" style="text-indent:2em" | 34.50(8) keV
| 43(5) s
| (7/2)-
|
|
|-
|-
| style="text-indent:1em" | <sup>183m2</sup>Pt
| style="text-indent:1em" | <sup>183m2</sup>Pt
| colspan="3" style="text-indent:2em" | 195.68(11) keV
| colspan="3" style="text-indent:2em" | 195.68(11) keV
| >150 ns
| >150 ns
| (9/2)+
|
|
|
|
| (9/2)+
|-
| <sup>184</sup>Pt
| style="text-align:right" | 78
| style="text-align:right" | 106
| 183.959922(19)
| 17.3(2) min
| 0+
|
|
|
|
|-
| rowspan=2|<sup>184</sup>Pt
| rowspan=2 style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 106
| rowspan=2|183.959922(19)
| rowspan=2|17.3(2) min
| β<sup>+</sup> (99.99%)
| <sup>184</sup>Ir
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (.00169%)
| <sup>180</sup>Os
|-
|-
| style="text-indent:1em" | <sup>184m</sup>Pt
| style="text-indent:1em" | <sup>184m</sup>Pt
| colspan="3" style="text-indent:2em" | 1839.4(16) keV
| colspan="3" style="text-indent:2em" | 1839.4(16) keV
| 1.01(5) ms
| 1.01(5) ms
| IT
| <sup>184</sup>Pt
| 8-
| 8-
|
|
|
|
|-
|-
| <sup>185</sup>Pt
| rowspan=2|<sup>185</sup>Pt
| style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 78
| style="text-align:right" | 107
| rowspan=2 style="text-align:right" | 107
| 184.96062(4)
| rowspan=2|184.96062(4)
| 70.9(24) min
| rowspan=2|70.9(24) min
| β<sup>+</sup> (99.99%)
| (9/2+)
| <sup>185</sup>Ir
|
| rowspan=2|(9/2+)
|
| rowspan=2|
| rowspan=2|
|-
|-
| α (.005%)
| style="text-indent:1em" | <sup>185m</sup>Pt
| <sup>181</sup>Os
| colspan="3" style="text-indent:2em" | 103.4(2) keV
|-
| 33.0(8) min
| rowspan=2 style="text-indent:1em" | <sup>185m</sup>Pt
| (1/2-)
| rowspan=2 colspan="3" style="text-indent:2em" | 103.4(2) keV
|
| rowspan=2|33.0(8) min
|
| β<sup>+</sup> (98%)
| <sup>185</sup>Ir
| rowspan=2|(1/2-)
| rowspan=2|
| rowspan=2|
|-
|-
| α (2%)
| <sup>186</sup>Pt
| <sup>181</sup>Os
| style="text-align:right" | 78
|-
| style="text-align:right" | 108
| rowspan=2|<sup>186</sup>Pt
| 185.959351(23)
| rowspan=2 style="text-align:right" | 78
| 2.08(5) h
| rowspan=2 style="text-align:right" | 108
| 0+
| rowspan=2|185.959351(23)
|
| rowspan=2|2.08(5) h
|
| β<sup>+</sup> (99.99%)
| <sup>186</sup>Ir
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (.00014%)
| <sup>182</sup>Os
|-
|-
| <sup>187</sup>Pt
| <sup>187</sup>Pt
Line 245: Line 365:
| 186.96059(3)
| 186.96059(3)
| 2.35(3) h
| 2.35(3) h
| β<sup>+</sup>
| <sup>187</sup>Ir
| 3/2-
| 3/2-
|
|
|
|
|-
|-
| <sup>188</sup>Pt
| rowspan=2|<sup>188</sup>Pt
| style="text-align:right" | 78
| rowspan=2 style="text-align:right" | 78
| style="text-align:right" | 110
| rowspan=2 style="text-align:right" | 110
| 187.959395(6)
| rowspan=2|187.959395(6)
| 10.2(3) d
| rowspan=2|10.2(3) d
| [[Electron capture|EC]] (99.99%)
| 0+
| <sup>188</sup>Ir
|
| rowspan=2|0+
|
| rowspan=2|
| rowspan=2|
|-
| α (.000026%)
| <sup>184</sup>Os
|-
|-
| <sup>189</sup>Pt
| <sup>189</sup>Pt
Line 263: Line 390:
| 188.960834(12)
| 188.960834(12)
| 10.87(12) h
| 10.87(12) h
| β<sup>+</sup>
| <sup>189</sup>Ir
| 3/2-
| 3/2-
|
|
Line 270: Line 399:
| colspan="3" style="text-indent:2em" | 172.80(6) keV
| colspan="3" style="text-indent:2em" | 172.80(6) keV
| 464(25) ns
| 464(25) ns
|
|
| 9/2-
| 9/2-
|
|
Line 277: Line 408:
| colspan="3" style="text-indent:2em" | 191.6(4) keV
| colspan="3" style="text-indent:2em" | 191.6(4) keV
| 143(5) µs
| 143(5) µs
|
|
| (13/2+)
| (13/2+)
|
|
Line 286: Line 419:
| 189.959932(6)
| 189.959932(6)
| '''6.5(3)E+11 a'''
| '''6.5(3)E+11 a'''
| α
| <sup>186</sup>Os
| 0+
| 0+
| 0.00014(1)
| 0.00014(1)
Line 295: Line 430:
| 190.961677(5)
| 190.961677(5)
| 2.862(7) d
| 2.862(7) d
| EC
| <sup>191</sup>Ir
| 3/2-
| 3/2-
|
|
Line 302: Line 439:
| colspan="3" style="text-indent:2em" | 100.67(2) keV
| colspan="3" style="text-indent:2em" | 100.67(2) keV
| >1 µs
| >1 µs
|
|
| (9/2)-
| (9/2)-
|
|
Line 309: Line 448:
| colspan="3" style="text-indent:2em" | 149.04(2) keV
| colspan="3" style="text-indent:2em" | 149.04(2) keV
| 95(5) µs
| 95(5) µs
|
|
| (13/2)+
| (13/2)+
|
|
Line 317: Line 458:
| style="text-align:right" | 114
| style="text-align:right" | 114
| 191.9610380(27)
| 191.9610380(27)
| '''Stable'''<ref group="n">Believed to undergo α decay to <sup>188</sup>Os</ref>
| colspan=3 align=center|'''Stable'''<ref group="n">Believed to undergo α decay to <sup>188</sup>Os</ref>
| 0+
| 0+
| 0.00782(7)
| 0.00782(7)
Line 327: Line 468:
| 192.9629874(18)
| 192.9629874(18)
| 50(6) a
| 50(6) a
| EC
| <sup>193</sup>Ir
| 1/2-
| 1/2-
|
|
Line 334: Line 477:
| colspan="3" style="text-indent:2em" | 149.78(4) keV
| colspan="3" style="text-indent:2em" | 149.78(4) keV
| 4.33(3) d
| 4.33(3) d
| IT
| <sup>193</sup>Pt
| 13/2+
| 13/2+
|
|
Line 342: Line 487:
| style="text-align:right" | 116
| style="text-align:right" | 116
| 193.9626803(9)
| 193.9626803(9)
| '''Stable'''<ref group="n">Believed to undergo α decay to <sup>190</sup>Os</ref>
| colspan=3 align=center|'''Stable'''<ref group="n">Believed to undergo α decay to <sup>190</sup>Os</ref>
| 0+
| 0+
| 0.32967(99)
| 0.32967(99)
Line 351: Line 496:
| style="text-align:right" | 117
| style="text-align:right" | 117
| 194.9647911(9)
| 194.9647911(9)
| '''Stable'''<ref group="n">Believed to undergo α decay to <sup>191</sup>Os</ref>
| colspan=3 align=center|'''Stable'''<ref group="n">Believed to undergo α decay to <sup>191</sup>Os</ref>
| 1/2-
| 1/2-
| 0.33832(10)
| 0.33832(10)
Line 359: Line 504:
| colspan="3" style="text-indent:2em" | 259.30(8) keV
| colspan="3" style="text-indent:2em" | 259.30(8) keV
| 4.010(5) d
| 4.010(5) d
| IT
| <sup>195</sup>Pt
| 13/2+
| 13/2+
|
|
Line 367: Line 514:
| style="text-align:right" | 118
| style="text-align:right" | 118
| 195.9649515(9)
| 195.9649515(9)
| '''Stable'''<ref group="n">Believed to undergo α decay to <sup>192</sup>Os</ref>
| colspan=3 align=center|'''Stable'''<ref group="n">Believed to undergo α decay to <sup>192</sup>Os</ref>
| 0+
| 0+
| 0.25242(41)
| 0.25242(41)
Line 377: Line 524:
| 196.9673402(9)
| 196.9673402(9)
| 19.8915(19) h
| 19.8915(19) h
| β<sup>-</sup>
| <sup>197</sup>Au
| 1/2-
| 1/2-
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>197m</sup>Pt
| rowspan=2 style="text-indent:1em" | <sup>197m</sup>Pt
| colspan="3" style="text-indent:2em" | 399.59(20) keV
| rowspan=2 colspan="3" style="text-indent:2em" | 399.59(20) keV
| 95.41(18) min
| rowspan=2|95.41(18) min
| IT (96.7%)
| 13/2+
| <sup>197</sup>Pt
|
| rowspan=2|13/2+
|
| rowspan=2|
| rowspan=2|
|-
| β<sup>-</sup> (3.3%)
| <sup>197</sup>Au
|-
|-
| <sup>198</sup>Pt
| <sup>198</sup>Pt
Line 392: Line 546:
| style="text-align:right" | 120
| style="text-align:right" | 120
| 197.967893(3)
| 197.967893(3)
| '''Stable'''<ref group="n">Believed to undergo α decay to <sup>194</sup>Os or double β<sup>-</sup> decay to <sup>198</sup>Hg with a half-life over 320E+12 years</ref>
| colspan=3 align=center|'''Stable'''<ref group="n">Believed to undergo α decay to <sup>194</sup>Os or double β<sup>-</sup> decay to <sup>198</sup>Hg with a half-life over 320E+12 years</ref>
| 0+
| 0+
| 0.07163(55)
| 0.07163(55)
Line 402: Line 556:
| 198.970593(3)
| 198.970593(3)
| 30.80(21) min
| 30.80(21) min
| β<sup>-</sup>
| <sup>199</sup>Au
| 5/2-
| 5/2-
|
|
Line 409: Line 565:
| colspan="3" style="text-indent:2em" | 424(2) keV
| colspan="3" style="text-indent:2em" | 424(2) keV
| 13.6(4) s
| 13.6(4) s
| IT
| <sup>199</sup>Pt
| (13/2)+
| (13/2)+
|
|
Line 418: Line 576:
| 199.971441(22)
| 199.971441(22)
| 12.5(3) h
| 12.5(3) h
| β<sup>-</sup>
| <sup>200</sup>Au
| 0+
| 0+
|
|
Line 427: Line 587:
| 200.97451(5)
| 200.97451(5)
| 2.5(1) min
| 2.5(1) min
| β<sup>-</sup>
| <sup>201</sup>Au
| (5/2-)
| (5/2-)
|
|
Line 436: Line 598:
| 201.97574(32)#
| 201.97574(32)#
| 44(15) h
| 44(15) h
| β<sup>-</sup>
| <sup>202</sup>Au
| 0+
| 0+
|
|

Revision as of 15:15, 6 May 2011

Natural Platinum (Pt) occurs in five stable isotopes (192Pt, 194Pt, 195Pt, 196Pt, 198Pt) and one very-long lived radioisotope (190Pt)

Standard atomic mass: 195.084(9) u

Table

nuclide
symbol
Z(p) N(n)  
isotopic mass (u)
 
half-life decay mode(s)[1] daughter
isotope(s)
nuclear
spin
representative
isotopic
composition
(mole fraction)
range of natural
variation
(mole fraction)
excitation energy
166Pt 78 88 165.99486(54)# 300(100) µs 0+
167Pt 78 89 166.99298(44)# 700(200) µs 7/2-#
168Pt 78 90 167.98815(22) 2.00(18) ms α 164Os 0+
β+ (rare) 168Ir
169Pt 78 91 168.98672(22)# 3.7(15) ms α 165Os 3/2-#
β+ (rare) 169Ir
170Pt 78 92 169.982495(20) 14.0(2) ms α (98%) 166Os 0+
β+ (2%) 170Ir
171Pt 78 93 170.98124(9) 51(2) ms α (99%) 167Os 3/2-#
β+ (1%) 171Ir
172Pt 78 94 171.977347(14) 98.4(24) ms α (77%) 168Os 0+
β+ (23%) 172Ir
173Pt 78 95 172.97644(6) 365(7) ms α (84%) 169Os 5/2-#
β+ (16%) 173Ir
174Pt 78 96 173.972819(13) 0.889(17) s α (83%) 170Os 0+
β+ (17%) 174Ir
175Pt 78 97 174.972421(20) 2.53(6) s α (64%) 171Os 5/2-#
β+ (36%) 175Ir
176Pt 78 98 175.968945(15) 6.33(15) s β+ (62%) 176Ir 0+
α (38%) 172Os
177Pt 78 99 176.968469(16) 10.6(4) s β+ (94.4%) 177Ir 5/2-
α (5.6%) 173Os
177mPt 147.4(4) keV 2.2(3) µs 1/2-
178Pt 78 100 177.965649(12) 21.1(6) s β+ (92.3%) 178Ir 0+
α (7.7%) 174Os
179Pt 78 101 178.965363(10) 21.2(4) s β+ (99.76%) 179Ir 1/2-
α (0.24%) 175Os
180Pt 78 102 179.963031(12) 56(2) s β+ (99.7%) 180Ir 0+
α (0.3%) 176Os
181Pt 78 103 180.963097(16) 52.0(22) s β+ (99.93%) 181Ir 1/2-
α (0.074%) 177Os
182Pt 78 104 181.961171(17) 2.2(1) min β+ (99.96%) 182Ir 0+
α (.038%) 178Os
183Pt 78 105 182.961597(17) 6.5(10) min β+ (99.99%) 183Ir 1/2-
α (.0096%) 179Os
183m1Pt 34.50(8) keV 43(5) s β+ (99.99%) 183Ir (7/2)-
α (.0004%) 179Os
IT 183Pt
183m2Pt 195.68(11) keV >150 ns (9/2)+
184Pt 78 106 183.959922(19) 17.3(2) min β+ (99.99%) 184Ir 0+
α (.00169%) 180Os
184mPt 1839.4(16) keV 1.01(5) ms IT 184Pt 8-
185Pt 78 107 184.96062(4) 70.9(24) min β+ (99.99%) 185Ir (9/2+)
α (.005%) 181Os
185mPt 103.4(2) keV 33.0(8) min β+ (98%) 185Ir (1/2-)
α (2%) 181Os
186Pt 78 108 185.959351(23) 2.08(5) h β+ (99.99%) 186Ir 0+
α (.00014%) 182Os
187Pt 78 109 186.96059(3) 2.35(3) h β+ 187Ir 3/2-
188Pt 78 110 187.959395(6) 10.2(3) d EC (99.99%) 188Ir 0+
α (.000026%) 184Os
189Pt 78 111 188.960834(12) 10.87(12) h β+ 189Ir 3/2-
189m1Pt 172.80(6) keV 464(25) ns 9/2-
189m2Pt 191.6(4) keV 143(5) µs (13/2+)
190Pt 78 112 189.959932(6) 6.5(3)E+11 a α 186Os 0+ 0.00014(1)
191Pt 78 113 190.961677(5) 2.862(7) d EC 191Ir 3/2-
191m1Pt 100.67(2) keV >1 µs (9/2)-
191m2Pt 149.04(2) keV 95(5) µs (13/2)+
192Pt 78 114 191.9610380(27) Stable[n 1] 0+ 0.00782(7)
193Pt 78 115 192.9629874(18) 50(6) a EC 193Ir 1/2-
193mPt 149.78(4) keV 4.33(3) d IT 193Pt 13/2+
194Pt 78 116 193.9626803(9) Stable[n 2] 0+ 0.32967(99)
195Pt 78 117 194.9647911(9) Stable[n 3] 1/2- 0.33832(10)
195mPt 259.30(8) keV 4.010(5) d IT 195Pt 13/2+
196Pt 78 118 195.9649515(9) Stable[n 4] 0+ 0.25242(41)
197Pt 78 119 196.9673402(9) 19.8915(19) h β- 197Au 1/2-
197mPt 399.59(20) keV 95.41(18) min IT (96.7%) 197Pt 13/2+
β- (3.3%) 197Au
198Pt 78 120 197.967893(3) Stable[n 5] 0+ 0.07163(55)
199Pt 78 121 198.970593(3) 30.80(21) min β- 199Au 5/2-
199mPt 424(2) keV 13.6(4) s IT 199Pt (13/2)+
200Pt 78 122 199.971441(22) 12.5(3) h β- 200Au 0+
201Pt 78 123 200.97451(5) 2.5(1) min β- 201Au (5/2-)
202Pt 78 124 201.97574(32)# 44(15) h β- 202Au 0+
  1. ^ Believed to undergo α decay to 188Os
  2. ^ Believed to undergo α decay to 190Os
  3. ^ Believed to undergo α decay to 191Os
  4. ^ Believed to undergo α decay to 192Os
  5. ^ Believed to undergo α decay to 194Os or double β- decay to 198Hg with a half-life over 320E+12 years

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.