Isotopes of gold: Difference between revisions
mNo edit summary |
XinaNicole (talk | contribs) Added info from http://www.nucleonica.net/unc.aspx |
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'''[[Gold]]''' ('''Au''') has one stable [[isotope]], <sup>197</sup>Au, and 18 [[radioisotope]]s with <sup>195</sup>Au being the most stable with a [[half-life]] of 186 days. |
'''[[Gold]]''' ('''Au''') has one stable [[isotope]], <sup>197</sup>Au, and 18 [[radioisotope]]s with <sup>195</sup>Au being the most stable with a [[half-life]] of 186 days. |
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Gold is the heaviest [[Monoisotopic element|element that has exactly one stable isotope]] |
Gold is the heaviest [[Monoisotopic element|element that has exactly one stable isotope]] ([[Bismuth]] was formerly believed to hold that distinction, but [[Bismuth-209]] has been found to be slightly radioactive). |
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Gold has been proposed as a material for creating a [[salted bomb|salted nuclear weapon]] ([[cobalt]] is another, better-known salting material). A jacket of natural <sup>197</sup>Au, irradiated by the intense high-energy neutron flux from an exploding thermonuclear weapon, would transmute into the radioactive isotope <sup>198</sup>Au with a half-life of 2.697 days and produce approximately .411 [[MeV]] of [[Gamma ray|gamma radiation]], significantly increasing the radioactivity of the weapon's [[Nuclear fallout|fallout]] for several days. Such a weapon is not known to have ever been built, tested, or used.<ref> |
Gold has been proposed as a material for creating a [[salted bomb|salted nuclear weapon]] ([[cobalt]] is another, better-known salting material). A jacket of natural <sup>197</sup>Au, irradiated by the intense high-energy neutron flux from an exploding thermonuclear weapon, would transmute into the radioactive isotope <sup>198</sup>Au with a half-life of 2.697 days and produce approximately .411 [[MeV]] of [[Gamma ray|gamma radiation]], significantly increasing the radioactivity of the weapon's [[Nuclear fallout|fallout]] for several days. Such a weapon is not known to have ever been built, tested, or used.<ref> |
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! <br />isotopic mass (u)<br /> |
! <br />isotopic mass (u)<br /> |
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! rowspan="2" | half-life |
! rowspan="2" | half-life |
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! rowspan="2" | decay mode(s)<ref>http://www.nucleonica.net/unc.aspx</ref> |
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! rowspan="2" | daughter<br>isotope(s) |
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! rowspan="2" | nuclear<br />spin |
! rowspan="2" | nuclear<br />spin |
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! rowspan="2" | representative<br />isotopic<br />composition<br />(mole fraction) |
! rowspan="2" | representative<br />isotopic<br />composition<br />(mole fraction) |
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| 168.99808(32)# |
| 168.99808(32)# |
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| 150# µs |
| 150# µs |
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| 1/2+# |
| 1/2+# |
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| style="text-align:right" | 91 |
| style="text-align:right" | 91 |
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| 169.99612(22)# |
| 169.99612(22)# |
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| 310(50) µs |
| 310(50) µs<br>[286(+50-40) µs] |
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| (2-) |
| (2-) |
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| style="text-indent:1em" | <sup>170m</sup>Au |
| style="text-indent:1em" | <sup>170m</sup>Au |
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| colspan="3" style="text-indent:2em" | 275(14) keV |
| colspan="3" style="text-indent:2em" | 275(14) keV |
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| 630(60) µs |
| 630(60) µs<br>[0.62(+6-5) ms] |
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| (9+) |
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| |
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| (9+) |
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|- |
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| <sup>171</sup>Au |
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| style="text-align:right" | 79 |
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| style="text-align:right" | 92 |
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| 170.991879(28) |
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| 30(5) µs |
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| (1/2+) |
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|- |
|- |
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| rowspan=2|<sup>171</sup>Au |
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| rowspan=2 style="text-align:right" | 79 |
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| rowspan=2 style="text-align:right" | 92 |
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| 1.014(19) ms |
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| rowspan=2|170.991879(28) |
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| 11/2- |
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| rowspan=2|30(5) µs |
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| [[proton emission|p]] |
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| |
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| <sup>170</sup>Pt |
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| rowspan=2|(1/2+) |
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| rowspan=2| |
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| rowspan=2| |
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|- |
|- |
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| [[alpha decay|α]] (rare) |
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| <sup>172</sup>Au |
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| <sup>167</sup>Ir |
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| style="text-align:right" | 79 |
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| style="text-align:right" | 93 |
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| 171.99004(17)# |
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| 4.7(11) ms |
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| high |
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|- |
|- |
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| <sup> |
| rowspan=2 style="text-indent:1em" | <sup>171m</sup>Au |
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| style="text- |
| rowspan=2 colspan="3" style="text-indent:2em" | 250(16) keV |
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| rowspan=2|1.014(19) ms |
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| style="text-align:right" | 94 |
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| α (54%) |
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| <sup>167</sup>Ir |
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| 25(1) ms |
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| rowspan=2|11/2- |
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| rowspan=2| |
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| rowspan=2| |
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|- |
|- |
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| p (46%) |
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| style="text-indent:1em" | <sup>173m</sup>Au |
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| <sup>170</sup>Pt |
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| colspan="3" style="text-indent:2em" | 214(23) keV |
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| 14.0(9) ms |
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| (11/2-) |
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| |
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|- |
|- |
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| <sup> |
| rowspan=2|<sup>172</sup>Au |
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| style="text-align:right" | 79 |
| rowspan=2 style="text-align:right" | 79 |
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| style="text-align:right" | |
| rowspan=2 style="text-align:right" | 93 |
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| rowspan=2|171.99004(17)# |
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| rowspan=2|4.7(11) ms |
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| α (98%) |
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| low |
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| <sup>168</sup>Ir |
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| rowspan=2|high |
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| rowspan=2| |
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| rowspan=2| |
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|- |
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| p (2%) |
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| <sup>171</sup>Pt |
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|- |
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| rowspan=2|<sup>173</sup>Au |
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| rowspan=2 style="text-align:right" | 79 |
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| rowspan=2 style="text-align:right" | 94 |
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| rowspan=2|172.986237(28) |
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| rowspan=2|25(1) ms |
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| α |
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| <sup>169</sup>Ir |
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| rowspan=2|(1/2+) |
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| rowspan=2| |
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| rowspan=2| |
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|- |
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| [[beta decay|β<sup>+</sup>]] (rare) |
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| <sup>173</sup>Pt |
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|- |
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| rowspan=2 style="text-indent:1em" | <sup>173m</sup>Au |
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| rowspan=2 colspan="3" style="text-indent:2em" | 214(23) keV |
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| rowspan=2|14.0(9) ms |
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| α (96%) |
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| <sup>169</sup>Ir |
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| rowspan=2|(11/2-) |
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| rowspan=2| |
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| rowspan=2| |
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|- |
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| β<sup>+</sup> (4%) |
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| <sup>173</sup>Pt |
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|- |
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| rowspan=2|<sup>174</sup>Au |
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| rowspan=2 style="text-align:right" | 79 |
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| rowspan=2 style="text-align:right" | 95 |
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| rowspan=2|173.98476(11)# |
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| rowspan=2|139(3) ms |
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| α |
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| <sup>170</sup>Ir |
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| rowspan=2|low |
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| rowspan=2| |
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| rowspan=2| |
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|- |
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| β<sup>+</sup> (rare) |
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| <sup>174</sup>Pt |
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|- |
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| style="text-indent:1em" | <sup>174m</sup>Au |
| style="text-indent:1em" | <sup>174m</sup>Au |
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| colspan="3" style="text-indent:2em" | 360(70)# keV |
| colspan="3" style="text-indent:2em" | 360(70)# keV |
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| 171(29) ms |
| 171(29) ms |
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| high |
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| |
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| |
| |
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| high |
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|- |
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| <sup>175</sup>Au |
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| style="text-align:right" | 79 |
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| style="text-align:right" | 96 |
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| 174.98127(5) |
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| 100# ms |
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| 1/2+# |
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| |
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| |
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|- |
|- |
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| rowspan=2|<sup>175</sup>Au |
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| |
| rowspan=2 style="text-align:right" | 79 |
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| rowspan=2 style="text-align:right" | 96 |
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| 156(3) ms |
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| rowspan=2|174.98127(5) |
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| 11/2-# |
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| rowspan=2|100# ms |
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| α (82%) |
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| |
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| <sup>171</sup>Ir |
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| rowspan=2|1/2+# |
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| rowspan=2| |
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| rowspan=2| |
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|- |
|- |
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| <sup> |
| β<sup>+</sup> (18%) |
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| <sup>175</sup>Pt |
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| style="text-align:right" | 79 |
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|- |
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| style="text-align:right" | 97 |
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| rowspan=2 style="text-indent:1em" | <sup>175m</sup>Au |
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| 175.98010(11)# |
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| rowspan=2 colspan="3" style="text-indent:2em" | 200(30)# keV |
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| 1.08(17) s [0.84(+17-14) s] |
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| rowspan=2|156(3) ms |
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| (5-) |
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| |
| α |
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| <sup>171</sup>Ir |
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| |
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| rowspan=2|11/2-# |
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| rowspan=2| |
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| rowspan=2| |
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|- |
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| β<sup>+</sup> |
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| <sup>175</sup>Pt |
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|- |
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| rowspan=2|<sup>176</sup>Au |
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| rowspan=2 style="text-align:right" | 79 |
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| rowspan=2 style="text-align:right" | 97 |
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| rowspan=2|175.98010(11)# |
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| rowspan=2|1.08(17) s<br>[0.84(+17-14) s] |
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| α (60%) |
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| <sup>172</sup>Ir |
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| rowspan=2|(5-) |
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| rowspan=2| |
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| rowspan=2| |
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|- |
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| β<sup>+</sup> (40%) |
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| <sup>176</sup>Pt |
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|- |
|- |
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| style="text-indent:1em" | <sup>176m</sup>Au |
| style="text-indent:1em" | <sup>176m</sup>Au |
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| colspan="3" style="text-indent:2em" | 150(100)# keV |
| colspan="3" style="text-indent:2em" | 150(100)# keV |
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| 860(160) ms |
| 860(160) ms |
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| (7+) |
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| |
| |
||
| |
| |
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| (7+) |
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|- |
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| <sup>177</sup>Au |
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| style="text-align:right" | 79 |
|||
| style="text-align:right" | 98 |
|||
| 176.976865(14) |
|||
| 1462(32) ms |
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| (1/2+,3/2+) |
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| |
| |
||
| |
| |
||
|- |
|||
| rowspan=2|<sup>177</sup>Au |
|||
| rowspan=2 style="text-align:right" | 79 |
|||
| rowspan=2 style="text-align:right" | 98 |
|||
| rowspan=2|176.976865(14) |
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| rowspan=2|1462(32) ms |
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| β<sup>+</sup> (60%) |
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| <sup>177</sup>Pt |
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| rowspan=2|(1/2+,3/2+) |
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| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
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| α (40%) |
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| <sup>173</sup>Ir |
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|- |
|- |
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| style="text-indent:1em" | <sup>177m</sup>Au |
| style="text-indent:1em" | <sup>177m</sup>Au |
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| colspan="3" style="text-indent:2em" | 216(26) keV |
| colspan="3" style="text-indent:2em" | 216(26) keV |
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| 1.180(12) s |
| 1.180(12) s |
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| 11/2- |
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| |
| |
||
| |
| |
||
|- |
| 11/2- |
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| <sup>178</sup>Au |
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| style="text-align:right" | 79 |
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| style="text-align:right" | 99 |
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| 177.97603(6) |
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| 2.6(5) s |
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| |
|||
| |
| |
||
| |
| |
||
|- |
|- |
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| <sup> |
| rowspan=2|<sup>178</sup>Au |
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| style="text-align:right" | 79 |
| rowspan=2 style="text-align:right" | 79 |
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| style="text-align:right" | |
| rowspan=2 style="text-align:right" | 99 |
||
| rowspan=2|177.97603(6) |
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| 178.973213(18) |
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| |
| rowspan=2|2.6(5) s |
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| β<sup>+</sup> (60%) |
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| 5/2-# |
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| <sup>178</sup>Pt |
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| |
|||
| rowspan=2| |
|||
| |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
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| α (40%) |
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| <sup>174</sup>Ir |
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|- |
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| rowspan=2|<sup>179</sup>Au |
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| rowspan=2 style="text-align:right" | 79 |
|||
| rowspan=2 style="text-align:right" | 100 |
|||
| rowspan=2|178.973213(18) |
|||
| rowspan=2|7.1(3) s |
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| β<sup>+</sup> (78%) |
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| <sup>179</sup>Pt |
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| rowspan=2|5/2-# |
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| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
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| α (22%) |
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| <sup>175</sup>Ir |
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|- |
|- |
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| style="text-indent:1em" | <sup>179m</sup>Au |
| style="text-indent:1em" | <sup>179m</sup>Au |
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| colspan="3" style="text-indent:2em" | 99(16) keV |
| colspan="3" style="text-indent:2em" | 99(16) keV |
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| |
| |
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| (11/2-) |
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| |
| |
||
| |
| |
||
|- |
| (11/2-) |
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| <sup>180</sup>Au |
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| style="text-align:right" | 79 |
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| style="text-align:right" | 101 |
|||
| 179.972521(23) |
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| 8.1(3) s |
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| |
|||
| |
| |
||
| |
| |
||
|- |
|- |
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| <sup> |
| rowspan=2|<sup>180</sup>Au |
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| style="text-align:right" | 79 |
| rowspan=2 style="text-align:right" | 79 |
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| style="text-align:right" | |
| rowspan=2 style="text-align:right" | 101 |
||
| rowspan=2|179.972521(23) |
|||
| 180.970079(21) |
|||
| |
| rowspan=2|8.1(3) s |
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| |
| β<sup>+</sup> (98.2%) |
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| <sup>180</sup>Pt |
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| |
|||
| rowspan=2| |
|||
| |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|- |
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| α (1.8%) |
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| <sup>182</sup>Au |
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| <sup>176</sup>Ir |
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| style="text-align:right" | 79 |
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| style="text-align:right" | 103 |
|||
| 181.969618(22) |
|||
| 15.5(4) s |
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| (2+) |
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| |
|||
| |
|||
|- |
|- |
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| <sup> |
| rowspan=2|<sup>181</sup>Au |
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| style="text-align:right" | 79 |
| rowspan=2 style="text-align:right" | 79 |
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| style="text-align:right" | |
| rowspan=2 style="text-align:right" | 102 |
||
| rowspan=2|180.970079(21) |
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| 182.967593(11) |
|||
| |
| rowspan=2|13.7(14) s |
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| β<sup>+</sup> (97.3%) |
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| (5/2)- |
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| <sup>181</sup>Pt |
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| |
|||
| rowspan=2|(3/2-) |
|||
| |
|||
| rowspan=2| |
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| rowspan=2| |
|||
|- |
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| α (2.7%) |
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| <sup>177</sup>Ir |
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|- |
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| rowspan=2|<sup>182</sup>Au |
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| rowspan=2 style="text-align:right" | 79 |
|||
| rowspan=2 style="text-align:right" | 103 |
|||
| rowspan=2|181.969618(22) |
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| rowspan=2|15.5(4) s |
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| β<sup>+</sup> (99.87%) |
|||
| <sup>182</sup>Pt |
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| rowspan=2|(2+) |
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| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
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| α (.13%) |
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| <sup>178</sup>Ir |
|||
|- |
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| rowspan=2|<sup>183</sup>Au |
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| rowspan=2 style="text-align:right" | 79 |
|||
| rowspan=2 style="text-align:right" | 104 |
|||
| rowspan=2|182.967593(11) |
|||
| rowspan=2|42.8(10) s |
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| β<sup>+</sup> (99.2%) |
|||
| <sup>183</sup>Pt |
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| rowspan=2|(5/2)- |
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| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
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| α (.8%) |
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| <sup>179</sup>Ir |
|||
|- |
|- |
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| style="text-indent:1em" | <sup>183m1</sup>Au |
| style="text-indent:1em" | <sup>183m1</sup>Au |
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| colspan="3" style="text-indent:2em" | 73.3(4) keV |
| colspan="3" style="text-indent:2em" | 73.3(4) keV |
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| >1 µs |
| >1 µs |
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| |
|||
| |
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| (1/2)+ |
| (1/2)+ |
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| |
| |
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Line 241: | Line 339: | ||
| colspan="3" style="text-indent:2em" | 230.6(6) keV |
| colspan="3" style="text-indent:2em" | 230.6(6) keV |
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| <1 µs |
| <1 µs |
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| |
|||
| |
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| (11/2)- |
| (11/2)- |
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| |
| |
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Line 250: | Line 350: | ||
| 183.967452(24) |
| 183.967452(24) |
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| 20.6(9) s |
| 20.6(9) s |
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| β<sup>+</sup> |
|||
| <sup>184</sup>Pt |
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| 5+ |
| 5+ |
||
| |
| |
||
| |
| |
||
|- |
|- |
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| style="text-indent:1em" | <sup>184m</sup>Au |
| rowspan=3 style="text-indent:1em" | <sup>184m</sup>Au |
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| colspan="3" style="text-indent:2em" | 68.46(1) keV |
| rowspan=3 colspan="3" style="text-indent:2em" | 68.46(1) keV |
||
| 47.6(14) s |
| rowspan=3|47.6(14) s |
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| β<sup>+</sup> (70%) |
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| 2+ |
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| <sup>184</sup>Pt |
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| |
|||
| rowspan=3|2+ |
|||
| |
|||
| rowspan=3| |
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| rowspan=3| |
|||
|- |
|- |
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| [[Isomeric transition|IT]] (30%) |
|||
| <sup>185</sup>Au |
|||
| <sup>184</sup>Au |
|||
| style="text-align:right" | 79 |
|||
|- |
|||
| style="text-align:right" | 106 |
|||
| |
| α (.013%) |
||
| <sup>180</sup>Ir |
|||
| 4.25(6) min |
|||
| |
|- |
||
| rowspan=2|<sup>185</sup>Au |
|||
| |
|||
| rowspan=2 style="text-align:right" | 79 |
|||
| |
|||
| rowspan=2 style="text-align:right" | 106 |
|||
| rowspan=2|184.965789(28) |
|||
| rowspan=2|4.25(6) min |
|||
| β<sup>+</sup> (99.74%) |
|||
| <sup>185</sup>Pt |
|||
| rowspan=2|5/2- |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| α (.26%) |
|||
| <sup>181</sup>Ir |
|||
|- |
|- |
||
| style="text-indent:1em" | <sup>185m</sup>Au |
| style="text-indent:1em" | <sup>185m</sup>Au |
||
| colspan="3" style="text-indent:2em" | 100(100)# keV |
| colspan="3" style="text-indent:2em" | 100(100)# keV |
||
| 6.8(3) min |
| 6.8(3) min |
||
| 1/2+# |
|||
| |
| |
||
| |
| |
||
| 1/2+# |
|||
|- |
|||
| <sup>186</sup>Au |
|||
| style="text-align:right" | 79 |
|||
| style="text-align:right" | 107 |
|||
| 185.965953(23) |
|||
| 10.7(5) min |
|||
| 3- |
|||
| |
| |
||
| |
| |
||
|- |
|||
| rowspan=2|<sup>186</sup>Au |
|||
| rowspan=2 style="text-align:right" | 79 |
|||
| rowspan=2 style="text-align:right" | 107 |
|||
| rowspan=2|185.965953(23) |
|||
| rowspan=2|10.7(5) min |
|||
| β<sup>+</sup> (99.9992%) |
|||
| <sup>186</sup>Pt |
|||
| rowspan=2|3- |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| α (.0008%) |
|||
| <sup>182</sup>Ir |
|||
|- |
|- |
||
| style="text-indent:1em" | <sup>186m</sup>Au |
| style="text-indent:1em" | <sup>186m</sup>Au |
||
| colspan="3" style="text-indent:2em" | 227.77(7) keV |
| colspan="3" style="text-indent:2em" | 227.77(7) keV |
||
| 110(10) ns |
| 110(10) ns |
||
| |
|||
| |
|||
| 2+ |
| 2+ |
||
| |
| |
||
| |
| |
||
|- |
|- |
||
| <sup>187</sup>Au |
| rowspan=2|<sup>187</sup>Au |
||
| style="text-align:right" | 79 |
| rowspan=2 style="text-align:right" | 79 |
||
| style="text-align:right" | 108 |
| rowspan=2 style="text-align:right" | 108 |
||
| 186.964568(27) |
| rowspan=2|186.964568(27) |
||
| 8.4(3) min |
| rowspan=2|8.4(3) min |
||
| β<sup>+</sup> (99.997%) |
|||
| 1/2+ |
|||
| <sup>187</sup>Pt |
|||
| |
|||
| rowspan=2|1/2+ |
|||
| |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| α (.003%) |
|||
| <sup>183</sup>Ir |
|||
|- |
|- |
||
| style="text-indent:1em" | <sup>187m</sup>Au |
| style="text-indent:1em" | <sup>187m</sup>Au |
||
| colspan="3" style="text-indent:2em" | 120.51(16) keV |
| colspan="3" style="text-indent:2em" | 120.51(16) keV |
||
| 2.3(1) s |
| 2.3(1) s |
||
| IT |
|||
| <sup>187</sup>Au |
|||
| 9/2- |
| 9/2- |
||
| |
| |
||
Line 314: | Line 445: | ||
| 187.965324(22) |
| 187.965324(22) |
||
| 8.84(6) min |
| 8.84(6) min |
||
| β<sup>+</sup> |
|||
| <sup>188</sup>Pt |
|||
| 1(-) |
| 1(-) |
||
| |
| |
||
| |
| |
||
|- |
|- |
||
| rowspan=2|<sup>189</sup>Au |
|||
| rowspan=2 style="text-align:right" | 79 |
|||
| rowspan=2 style="text-align:right" | 110 |
|||
| rowspan=2|188.963948(22) |
|||
| rowspan=2|28.7(3) min |
|||
| β<sup>+</sup> (99.9997%) |
|||
| <sup>189</sup>Pt |
|||
| rowspan=2|1/2+ |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| α (.0003%) |
|||
| <sup>185</sup>Ir |
|||
|- |
|||
| rowspan=2 style="text-indent:1em" | <sup>189m1</sup>Au |
|||
| rowspan=2 colspan="3" style="text-indent:2em" | 247.23(16) keV |
|||
| rowspan=2|4.59(11) min |
|||
| β<sup>+</sup> |
|||
| <sup>189</sup>Pt |
|||
| rowspan=2|11/2- |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| IT (rare) |
|||
| <sup>189</sup>Au |
| <sup>189</sup>Au |
||
| style="text-align:right" | 79 |
|||
| style="text-align:right" | 110 |
|||
| 188.963948(22) |
|||
| 28.7(3) min |
|||
| 1/2+ |
|||
| |
|||
| |
|||
|- |
|||
| style="text-indent:1em" | <sup>189m1</sup>Au |
|||
| colspan="3" style="text-indent:2em" | 247.23(16) keV |
|||
| 4.59(11) min |
|||
| 11/2- |
|||
| |
|||
| |
|||
|- |
|- |
||
| style="text-indent:1em" | <sup>189m2</sup>Au |
| style="text-indent:1em" | <sup>189m2</sup>Au |
||
| colspan="3" style="text-indent:2em" | 325.11(16) keV |
| colspan="3" style="text-indent:2em" | 325.11(16) keV |
||
| 190(15) ns |
| 190(15) ns |
||
| |
|||
| |
|||
| 9/2- |
| 9/2- |
||
| |
| |
||
Line 344: | Line 489: | ||
| colspan="3" style="text-indent:2em" | 2554.7(12) keV |
| colspan="3" style="text-indent:2em" | 2554.7(12) keV |
||
| 242(10) ns |
| 242(10) ns |
||
| |
|||
| |
|||
| 31/2+ |
| 31/2+ |
||
| |
| |
||
| |
| |
||
|- |
|- |
||
| rowspan=2|<sup>190</sup>Au |
|||
| rowspan=2 style="text-align:right" | 79 |
|||
| rowspan=2 style="text-align:right" | 111 |
|||
| rowspan=2|189.964700(17) |
|||
| rowspan=2|42.8(10) min |
|||
| β<sup>+</sup> |
|||
| <sup>186</sup>Pt |
|||
| rowspan=2|1- |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| α (1E-6%) |
|||
|- |
|||
| rowspan=2 style="text-indent:1em" | <sup>190m</sup>Au |
|||
| rowspan=2 colspan="3" style="text-indent:2em" | 200(150)# keV |
|||
| rowspan=2|125(20) ms |
|||
| IT |
|||
| <sup>190</sup>Au |
| <sup>190</sup>Au |
||
| rowspan=2|11-# |
|||
| style="text-align:right" | 79 |
|||
| rowspan=2| |
|||
| style="text-align:right" | 111 |
|||
| rowspan=2| |
|||
| 189.964700(17) |
|||
| 42.8(10) min |
|||
| 1- |
|||
| |
|||
| |
|||
|- |
|- |
||
| |
| β<sup>+</sup> (rare) |
||
| <sup>190</sup>Pt |
|||
| colspan="3" style="text-indent:2em" | 200(150)# keV |
|||
| 125(20) ms |
|||
| 11-# |
|||
| |
|||
| |
|||
|- |
|- |
||
| <sup>191</sup>Au |
| <sup>191</sup>Au |
||
Line 369: | Line 525: | ||
| 190.96370(4) |
| 190.96370(4) |
||
| 3.18(8) h |
| 3.18(8) h |
||
| β<sup>+</sup> |
|||
| <sup>191</sup>Pt |
|||
| 3/2+ |
| 3/2+ |
||
| |
| |
||
Line 376: | Line 534: | ||
| colspan="3" style="text-indent:2em" | 266.2(5) keV |
| colspan="3" style="text-indent:2em" | 266.2(5) keV |
||
| 920(110) ms |
| 920(110) ms |
||
| IT |
|||
| <sup>191</sup>Au |
|||
| (11/2-) |
| (11/2-) |
||
| |
| |
||
Line 383: | Line 543: | ||
| colspan="3" style="text-indent:2em" | 2490(1) keV |
| colspan="3" style="text-indent:2em" | 2490(1) keV |
||
| >400 ns |
| >400 ns |
||
| |
|||
| |
|||
| |
| |
||
| |
| |
||
Line 392: | Line 554: | ||
| 191.964813(17) |
| 191.964813(17) |
||
| 4.94(9) h |
| 4.94(9) h |
||
| β<sup>+</sup> |
|||
| <sup>192</sup>Pt |
|||
| 1- |
| 1- |
||
| |
| |
||
Line 399: | Line 563: | ||
| colspan="3" style="text-indent:2em" | 135.41(25) keV |
| colspan="3" style="text-indent:2em" | 135.41(25) keV |
||
| 29 ms |
| 29 ms |
||
| IT |
|||
| <sup>192</sup>Au |
|||
| (5#)+ |
| (5#)+ |
||
| |
| |
||
Line 406: | Line 572: | ||
| colspan="3" style="text-indent:2em" | 431.6(5) keV |
| colspan="3" style="text-indent:2em" | 431.6(5) keV |
||
| 160(20) ms |
| 160(20) ms |
||
| |
|||
| |
|||
| (11-) |
| (11-) |
||
| |
| |
||
| |
| |
||
|- |
|- |
||
| rowspan=2|<sup>193</sup>Au |
|||
| rowspan=2 style="text-align:right" | 79 |
|||
| rowspan=2 style="text-align:right" | 114 |
|||
| rowspan=2|192.964150(11) |
|||
| rowspan=2|17.65(15) h |
|||
| β<sup>+</sup> (100%) |
|||
| <sup>189</sup>Pt |
|||
| rowspan=2|3/2+ |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| α (.00001%) |
|||
| <sup>189</sup>It |
|||
|- |
|||
| rowspan=2 style="text-indent:1em" | <sup>193m1</sup>Au |
|||
| rowspan=2 colspan="3" style="text-indent:2em" | 290.19(3) keV |
|||
| rowspan=2|3.9(3) s |
|||
| IT (99.97%) |
|||
| <sup>193</sup>Au |
| <sup>193</sup>Au |
||
| rowspan=2|11/2- |
|||
| style="text-align:right" | 79 |
|||
| rowspan=2| |
|||
| style="text-align:right" | 114 |
|||
| rowspan=2| |
|||
| 192.964150(11) |
|||
| 17.65(15) h |
|||
| 3/2+ |
|||
| |
|||
| |
|||
|- |
|- |
||
| |
| β<sup>+</sup> (.03%) |
||
| <sup>193</sup>Pt |
|||
| colspan="3" style="text-indent:2em" | 290.19(3) keV |
|||
| 3.9(3) s |
|||
| 11/2- |
|||
| |
|||
| |
|||
|- |
|- |
||
| style="text-indent:1em" | <sup>193m2</sup>Au |
| style="text-indent:1em" | <sup>193m2</sup>Au |
||
| colspan="3" style="text-indent:2em" | 2486.5(6) keV |
| colspan="3" style="text-indent:2em" | 2486.5(6) keV |
||
| 150(50) ns |
| 150(50) ns |
||
| |
|||
| |
|||
| (31/2+) |
| (31/2+) |
||
| |
| |
||
Line 438: | Line 618: | ||
| 193.965365(11) |
| 193.965365(11) |
||
| 38.02(10) h |
| 38.02(10) h |
||
| β<sup>+</sup> |
|||
| <sup>194</sup>Pt |
|||
| 1- |
| 1- |
||
| |
| |
||
Line 445: | Line 627: | ||
| colspan="3" style="text-indent:2em" | 107.4(5) keV |
| colspan="3" style="text-indent:2em" | 107.4(5) keV |
||
| 600(8) ms |
| 600(8) ms |
||
| IT |
|||
| <sup>194</sup>Au |
|||
| (5+) |
| (5+) |
||
| |
| |
||
Line 452: | Line 636: | ||
| colspan="3" style="text-indent:2em" | 475.8(6) keV |
| colspan="3" style="text-indent:2em" | 475.8(6) keV |
||
| 420(10) ms |
| 420(10) ms |
||
| |
|||
| |
|||
| (11-) |
| (11-) |
||
| |
| |
||
Line 461: | Line 647: | ||
| 194.9650346(14) |
| 194.9650346(14) |
||
| 186.098(47) d |
| 186.098(47) d |
||
| [[Electron capture|EC]] |
|||
| <sup>195</sup>Pt |
|||
| 3/2+ |
| 3/2+ |
||
| |
| |
||
Line 468: | Line 656: | ||
| colspan="3" style="text-indent:2em" | 318.58(4) keV |
| colspan="3" style="text-indent:2em" | 318.58(4) keV |
||
| 30.5(2) s |
| 30.5(2) s |
||
| IT |
|||
| <sup>195</sup>Au |
|||
| 11/2- |
| 11/2- |
||
| |
| |
||
| |
| |
||
|- |
|- |
||
| <sup>196</sup>Au |
| rowspan=2|<sup>196</sup>Au |
||
| style="text-align:right" | 79 |
| rowspan=2 style="text-align:right" | 79 |
||
| style="text-align:right" | 117 |
| rowspan=2 style="text-align:right" | 117 |
||
| 195.966570(3) |
| rowspan=2|195.966570(3) |
||
| 6.1669(6) d |
| rowspan=2|6.1669(6) d |
||
| β<sup>+</sup> (93.05%) |
|||
| 2- |
|||
| <sup>196</sup>Pt |
|||
| |
|||
| rowspan=2|2- |
|||
| |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| β<sup>-</sup> (6.95%) |
|||
| <sup>196</sup>Hg |
|||
|- |
|- |
||
| style="text-indent:1em" | <sup>196m1</sup>Au |
| style="text-indent:1em" | <sup>196m1</sup>Au |
||
| colspan="3" style="text-indent:2em" | 84.660(20) keV |
| colspan="3" style="text-indent:2em" | 84.660(20) keV |
||
| 8.1(2) s |
| 8.1(2) s |
||
| IT |
|||
| <sup>196</sup>Au |
|||
| 5+ |
| 5+ |
||
| |
| |
||
Line 491: | Line 688: | ||
| colspan="3" style="text-indent:2em" | 595.66(4) keV |
| colspan="3" style="text-indent:2em" | 595.66(4) keV |
||
| 9.6(1) h |
| 9.6(1) h |
||
| |
|||
| |
|||
| 12- |
| 12- |
||
| |
| |
||
| |
| |
||
|- |
|- |
||
| |
| <sup>197</sup>Au |
||
| style="text-align:right" | 79 |
| style="text-align:right" | 79 |
||
| style="text-align:right" | 118 |
| style="text-align:right" | 118 |
||
| 196.9665687(6) |
| 196.9665687(6) |
||
| colspan=3 align=center|'''Stable'''<ref group="n">Believed to undergo α decay to <sup>193</sup>Ir</ref> |
|||
| '''STABLE''' |
|||
| 3/2+ |
| 3/2+ |
||
| 1.0000 |
| 1.0000 |
||
Line 507: | Line 706: | ||
| colspan="3" style="text-indent:2em" | 409.15(8) keV |
| colspan="3" style="text-indent:2em" | 409.15(8) keV |
||
| 7.73(6) s |
| 7.73(6) s |
||
| IT |
|||
| <sup>197</sup>Au |
|||
| 11/2- |
| 11/2- |
||
| |
| |
||
Line 516: | Line 717: | ||
| 197.9682423(6) |
| 197.9682423(6) |
||
| 2.69517(21) d |
| 2.69517(21) d |
||
| β<sup>-</sup> |
|||
| <sup>198</sup>Hg |
|||
| 2- |
| 2- |
||
| |
| |
||
Line 523: | Line 726: | ||
| colspan="3" style="text-indent:2em" | 312.2200(20) keV |
| colspan="3" style="text-indent:2em" | 312.2200(20) keV |
||
| 124(4) ns |
| 124(4) ns |
||
| |
|||
| |
|||
| 5+ |
| 5+ |
||
| |
| |
||
Line 530: | Line 735: | ||
| colspan="3" style="text-indent:2em" | 811.7(15) keV |
| colspan="3" style="text-indent:2em" | 811.7(15) keV |
||
| 2.27(2) d |
| 2.27(2) d |
||
| IT |
|||
| <sup>198</sup>Au |
|||
| (12-) |
| (12-) |
||
| |
| |
||
Line 539: | Line 746: | ||
| 198.9687652(6) |
| 198.9687652(6) |
||
| 3.139(7) d |
| 3.139(7) d |
||
| β<sup>-</sup> |
|||
| <sup>199</sup>Hg |
|||
| 3/2+ |
| 3/2+ |
||
| |
| |
||
Line 546: | Line 755: | ||
| colspan="3" style="text-indent:2em" | 548.9368(21) keV |
| colspan="3" style="text-indent:2em" | 548.9368(21) keV |
||
| 440(30) µs |
| 440(30) µs |
||
| |
|||
| |
|||
| (11/2)- |
| (11/2)- |
||
| |
| |
||
Line 555: | Line 766: | ||
| 199.97073(5) |
| 199.97073(5) |
||
| 48.4(3) min |
| 48.4(3) min |
||
| β<sup>-</sup> |
|||
| <sup>200</sup>Hg |
|||
| 1(-) |
| 1(-) |
||
| |
| |
||
| |
| |
||
|- |
|- |
||
| style="text-indent:1em" | <sup>200m</sup>Au |
| rowspan=2 style="text-indent:1em" | <sup>200m</sup>Au |
||
| colspan="3" style="text-indent:2em" | 970(70) keV |
| rowspan=2 colspan="3" style="text-indent:2em" | 970(70) keV |
||
| 18.7(5) h |
| rowspan=2|18.7(5) h |
||
| β<sup>-</sup> (82%) |
|||
| 12- |
|||
| <sup>200</sup>Hg |
|||
| |
|||
| rowspan=2|12- |
|||
| |
|||
| rowspan=2| |
|||
| rowspan=2| |
|||
|- |
|||
| IT (18%) |
|||
| <sup>200</sup>Au |
|||
|- |
|- |
||
| <sup>201</sup>Au |
| <sup>201</sup>Au |
||
Line 571: | Line 789: | ||
| 200.971657(3) |
| 200.971657(3) |
||
| 26(1) min |
| 26(1) min |
||
| β<sup>-</sup> |
|||
| <sup>201</sup>Hg |
|||
| 3/2+ |
| 3/2+ |
||
| |
| |
||
Line 580: | Line 800: | ||
| 201.97381(18) |
| 201.97381(18) |
||
| 28.8(19) s |
| 28.8(19) s |
||
| β<sup>-</sup> |
|||
| <sup>202</sup>Hg |
|||
| (1-) |
| (1-) |
||
| |
| |
||
Line 589: | Line 811: | ||
| 202.975155(3) |
| 202.975155(3) |
||
| 53(2) s |
| 53(2) s |
||
| β<sup>-</sup> |
|||
| <sup>203</sup>Hg |
|||
| 3/2+ |
| 3/2+ |
||
| |
| |
||
Line 598: | Line 822: | ||
| 203.97772(22)# |
| 203.97772(22)# |
||
| 39.8(9) s |
| 39.8(9) s |
||
| β<sup>-</sup> |
|||
| <sup>204</sup>Hg |
|||
| (2-) |
| (2-) |
||
| |
| |
||
Line 607: | Line 833: | ||
| 204.97987(32)# |
| 204.97987(32)# |
||
| 31(2) s |
| 31(2) s |
||
| β<sup>-</sup> |
|||
| <sup>205</sup>Hg |
|||
| 3/2+ |
| 3/2+ |
||
| |
| |
||
| |
| |
||
|} |
|} |
||
<references group="n" /> |
|||
=== Notes === |
=== Notes === |
Revision as of 17:55, 12 May 2011
Gold (Au) has one stable isotope, 197Au, and 18 radioisotopes with 195Au being the most stable with a half-life of 186 days.
Gold is the heaviest element that has exactly one stable isotope (Bismuth was formerly believed to hold that distinction, but Bismuth-209 has been found to be slightly radioactive).
Gold has been proposed as a material for creating a salted nuclear weapon (cobalt is another, better-known salting material). A jacket of natural 197Au, irradiated by the intense high-energy neutron flux from an exploding thermonuclear weapon, would transmute into the radioactive isotope 198Au with a half-life of 2.697 days and produce approximately .411 MeV of gamma radiation, significantly increasing the radioactivity of the weapon's fallout for several days. Such a weapon is not known to have ever been built, tested, or used.[1]
The highest amount of 198Au detected in any United States nuclear test was in shot "Sedan" detonated at Nevada Test Site on July 6, 1962.[2]
Standard atomic mass: 196.966569(4) 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 | |||||||||
169Au | 79 | 90 | 168.99808(32)# | 150# µs | 1/2+# | ||||
170Au | 79 | 91 | 169.99612(22)# | 310(50) µs [286(+50-40) µs] |
(2-) | ||||
170mAu | 275(14) keV | 630(60) µs [0.62(+6-5) ms] |
(9+) | ||||||
171Au | 79 | 92 | 170.991879(28) | 30(5) µs | p | 170Pt | (1/2+) | ||
α (rare) | 167Ir | ||||||||
171mAu | 250(16) keV | 1.014(19) ms | α (54%) | 167Ir | 11/2- | ||||
p (46%) | 170Pt | ||||||||
172Au | 79 | 93 | 171.99004(17)# | 4.7(11) ms | α (98%) | 168Ir | high | ||
p (2%) | 171Pt | ||||||||
173Au | 79 | 94 | 172.986237(28) | 25(1) ms | α | 169Ir | (1/2+) | ||
β+ (rare) | 173Pt | ||||||||
173mAu | 214(23) keV | 14.0(9) ms | α (96%) | 169Ir | (11/2-) | ||||
β+ (4%) | 173Pt | ||||||||
174Au | 79 | 95 | 173.98476(11)# | 139(3) ms | α | 170Ir | low | ||
β+ (rare) | 174Pt | ||||||||
174mAu | 360(70)# keV | 171(29) ms | high | ||||||
175Au | 79 | 96 | 174.98127(5) | 100# ms | α (82%) | 171Ir | 1/2+# | ||
β+ (18%) | 175Pt | ||||||||
175mAu | 200(30)# keV | 156(3) ms | α | 171Ir | 11/2-# | ||||
β+ | 175Pt | ||||||||
176Au | 79 | 97 | 175.98010(11)# | 1.08(17) s [0.84(+17-14) s] |
α (60%) | 172Ir | (5-) | ||
β+ (40%) | 176Pt | ||||||||
176mAu | 150(100)# keV | 860(160) ms | (7+) | ||||||
177Au | 79 | 98 | 176.976865(14) | 1462(32) ms | β+ (60%) | 177Pt | (1/2+,3/2+) | ||
α (40%) | 173Ir | ||||||||
177mAu | 216(26) keV | 1.180(12) s | 11/2- | ||||||
178Au | 79 | 99 | 177.97603(6) | 2.6(5) s | β+ (60%) | 178Pt | |||
α (40%) | 174Ir | ||||||||
179Au | 79 | 100 | 178.973213(18) | 7.1(3) s | β+ (78%) | 179Pt | 5/2-# | ||
α (22%) | 175Ir | ||||||||
179mAu | 99(16) keV | (11/2-) | |||||||
180Au | 79 | 101 | 179.972521(23) | 8.1(3) s | β+ (98.2%) | 180Pt | |||
α (1.8%) | 176Ir | ||||||||
181Au | 79 | 102 | 180.970079(21) | 13.7(14) s | β+ (97.3%) | 181Pt | (3/2-) | ||
α (2.7%) | 177Ir | ||||||||
182Au | 79 | 103 | 181.969618(22) | 15.5(4) s | β+ (99.87%) | 182Pt | (2+) | ||
α (.13%) | 178Ir | ||||||||
183Au | 79 | 104 | 182.967593(11) | 42.8(10) s | β+ (99.2%) | 183Pt | (5/2)- | ||
α (.8%) | 179Ir | ||||||||
183m1Au | 73.3(4) keV | >1 µs | (1/2)+ | ||||||
183m2Au | 230.6(6) keV | <1 µs | (11/2)- | ||||||
184Au | 79 | 105 | 183.967452(24) | 20.6(9) s | β+ | 184Pt | 5+ | ||
184mAu | 68.46(1) keV | 47.6(14) s | β+ (70%) | 184Pt | 2+ | ||||
IT (30%) | 184Au | ||||||||
α (.013%) | 180Ir | ||||||||
185Au | 79 | 106 | 184.965789(28) | 4.25(6) min | β+ (99.74%) | 185Pt | 5/2- | ||
α (.26%) | 181Ir | ||||||||
185mAu | 100(100)# keV | 6.8(3) min | 1/2+# | ||||||
186Au | 79 | 107 | 185.965953(23) | 10.7(5) min | β+ (99.9992%) | 186Pt | 3- | ||
α (.0008%) | 182Ir | ||||||||
186mAu | 227.77(7) keV | 110(10) ns | 2+ | ||||||
187Au | 79 | 108 | 186.964568(27) | 8.4(3) min | β+ (99.997%) | 187Pt | 1/2+ | ||
α (.003%) | 183Ir | ||||||||
187mAu | 120.51(16) keV | 2.3(1) s | IT | 187Au | 9/2- | ||||
188Au | 79 | 109 | 187.965324(22) | 8.84(6) min | β+ | 188Pt | 1(-) | ||
189Au | 79 | 110 | 188.963948(22) | 28.7(3) min | β+ (99.9997%) | 189Pt | 1/2+ | ||
α (.0003%) | 185Ir | ||||||||
189m1Au | 247.23(16) keV | 4.59(11) min | β+ | 189Pt | 11/2- | ||||
IT (rare) | 189Au | ||||||||
189m2Au | 325.11(16) keV | 190(15) ns | 9/2- | ||||||
189m3Au | 2554.7(12) keV | 242(10) ns | 31/2+ | ||||||
190Au | 79 | 111 | 189.964700(17) | 42.8(10) min | β+ | 186Pt | 1- | ||
α (1E-6%) | |||||||||
190mAu | 200(150)# keV | 125(20) ms | IT | 190Au | 11-# | ||||
β+ (rare) | 190Pt | ||||||||
191Au | 79 | 112 | 190.96370(4) | 3.18(8) h | β+ | 191Pt | 3/2+ | ||
191m1Au | 266.2(5) keV | 920(110) ms | IT | 191Au | (11/2-) | ||||
191m2Au | 2490(1) keV | >400 ns | |||||||
192Au | 79 | 113 | 191.964813(17) | 4.94(9) h | β+ | 192Pt | 1- | ||
192m1Au | 135.41(25) keV | 29 ms | IT | 192Au | (5#)+ | ||||
192m2Au | 431.6(5) keV | 160(20) ms | (11-) | ||||||
193Au | 79 | 114 | 192.964150(11) | 17.65(15) h | β+ (100%) | 189Pt | 3/2+ | ||
α (.00001%) | 189It | ||||||||
193m1Au | 290.19(3) keV | 3.9(3) s | IT (99.97%) | 193Au | 11/2- | ||||
β+ (.03%) | 193Pt | ||||||||
193m2Au | 2486.5(6) keV | 150(50) ns | (31/2+) | ||||||
194Au | 79 | 115 | 193.965365(11) | 38.02(10) h | β+ | 194Pt | 1- | ||
194m1Au | 107.4(5) keV | 600(8) ms | IT | 194Au | (5+) | ||||
194m2Au | 475.8(6) keV | 420(10) ms | (11-) | ||||||
195Au | 79 | 116 | 194.9650346(14) | 186.098(47) d | EC | 195Pt | 3/2+ | ||
195mAu | 318.58(4) keV | 30.5(2) s | IT | 195Au | 11/2- | ||||
196Au | 79 | 117 | 195.966570(3) | 6.1669(6) d | β+ (93.05%) | 196Pt | 2- | ||
β- (6.95%) | 196Hg | ||||||||
196m1Au | 84.660(20) keV | 8.1(2) s | IT | 196Au | 5+ | ||||
196m2Au | 595.66(4) keV | 9.6(1) h | 12- | ||||||
197Au | 79 | 118 | 196.9665687(6) | Stable[n 1] | 3/2+ | 1.0000 | |||
197mAu | 409.15(8) keV | 7.73(6) s | IT | 197Au | 11/2- | ||||
198Au | 79 | 119 | 197.9682423(6) | 2.69517(21) d | β- | 198Hg | 2- | ||
198m1Au | 312.2200(20) keV | 124(4) ns | 5+ | ||||||
198m2Au | 811.7(15) keV | 2.27(2) d | IT | 198Au | (12-) | ||||
199Au | 79 | 120 | 198.9687652(6) | 3.139(7) d | β- | 199Hg | 3/2+ | ||
199mAu | 548.9368(21) keV | 440(30) µs | (11/2)- | ||||||
200Au | 79 | 121 | 199.97073(5) | 48.4(3) min | β- | 200Hg | 1(-) | ||
200mAu | 970(70) keV | 18.7(5) h | β- (82%) | 200Hg | 12- | ||||
IT (18%) | 200Au | ||||||||
201Au | 79 | 122 | 200.971657(3) | 26(1) min | β- | 201Hg | 3/2+ | ||
202Au | 79 | 123 | 201.97381(18) | 28.8(19) s | β- | 202Hg | (1-) | ||
203Au | 79 | 124 | 202.975155(3) | 53(2) s | β- | 203Hg | 3/2+ | ||
204Au | 79 | 125 | 203.97772(22)# | 39.8(9) s | β- | 204Hg | (2-) | ||
205Au | 79 | 126 | 204.97987(32)# | 31(2) s | β- | 205Hg | 3/2+ |
- ^ Believed to undergo α decay to 193Ir
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
- ^ D. T. Win, M. Al Masum (2003). "Weapons of Mass Destruction" (PDF). Assumption University Journal of Technology. 6 (4): 199–219.
- ^ R. L. Miller (2002). U.S. Atlas of Nuclear Fallout, 1951-1970. Vol. 1 (Abridged General Reader ed.). Two Sixty Press. p. 340. ISBN 1881043134.
- ^ http://www.nucleonica.net/unc.aspx
- 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 (1): 3–128. doi:10.1016/j.nuclphysa.2003.11.001.
{{cite journal}}
: CS1 maint: multiple names: authors list (link)
- 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 (1): 3–128. doi:10.1016/j.nuclphysa.2003.11.001.
- Isotopic compositions and standard atomic masses from:
- J. R. de Laeter, J. K. Böhlke, P. De Bièvre, H. Hidaka, H. S. Peiser, K. J. R. Rosman and P. D. P. Taylor (2003). "Atomic weights of the elements. Review 2000 (IUPAC Technical Report)". Pure and Applied Chemistry. 75 (6): 683–800. doi:10.1351/pac200375060683.
{{cite journal}}
: CS1 maint: multiple names: authors list (link) - M. E. Wieser (2006). "Atomic weights of the elements 2005 (IUPAC Technical Report)". Pure and Applied Chemistry. 78 (11): 2051–2066. doi:10.1351/pac200678112051.
{{cite journal}}
: Unknown parameter|laysummary=
ignored (help)
- J. R. de Laeter, J. K. Böhlke, P. De Bièvre, H. Hidaka, H. S. Peiser, K. J. R. Rosman and P. D. P. Taylor (2003). "Atomic weights of the elements. Review 2000 (IUPAC Technical Report)". Pure and Applied Chemistry. 75 (6): 683–800. doi:10.1351/pac200375060683.
- Half-life, spin, and isomer data selected from the following sources. See editing notes on this article's talk page.
- 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 (1): 3–128. doi:10.1016/j.nuclphysa.2003.11.001.
{{cite journal}}
: CS1 maint: multiple names: authors list (link) - National Nuclear Data Center. "NuDat 2.1 database". Brookhaven National Laboratory. Retrieved September 2005.
{{cite web}}
: Check date values in:|accessdate=
(help) - N. E. Holden (2004). "Table of the Isotopes". In D. R. Lide (ed.). CRC Handbook of Chemistry and Physics (85th ed.). CRC Press. Section 11. ISBN 978-0849304859.
{{cite book}}
: Unknown parameter|nopp=
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suggested) (help)
- 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 (1): 3–128. doi:10.1016/j.nuclphysa.2003.11.001.