Jump to content

Isotopes of gold: Difference between revisions

From Wikipedia, the free encyclopedia
Content deleted Content added
mNo edit summary
Added info from http://www.nucleonica.net/unc.aspx
Line 1: Line 1:
'''[[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.


Gold is the heaviest [[Monoisotopic element|element that has exactly one stable isotope]], (now that [[bismuth]]-209 is found to be very slightly radioactive).
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).


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>
Line 34: Line 34:
! &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 45: Line 47:
| 168.99808(32)#
| 168.99808(32)#
| 150# µs
| 150# µs
|
|
| 1/2+#
| 1/2+#
|
|
Line 53: Line 57:
| style="text-align:right" | 91
| style="text-align:right" | 91
| 169.99612(22)#
| 169.99612(22)#
| 310(50) µs [286(+50-40) µs]
| 310(50) µs<br>[286(+50-40) µs]
|
|
| (2-)
| (2-)
|
|
Line 60: Line 66:
| style="text-indent:1em" | <sup>170m</sup>Au
| style="text-indent:1em" | <sup>170m</sup>Au
| colspan="3" style="text-indent:2em" | 275(14) keV
| colspan="3" style="text-indent:2em" | 275(14) keV
| 630(60) µs [0.62(+6-5) ms]
| 630(60) µs<br>[0.62(+6-5) ms]
| (9+)
|
|
|
|
| (9+)
|-
| <sup>171</sup>Au
| style="text-align:right" | 79
| style="text-align:right" | 92
| 170.991879(28)
| 30(5) µs
| (1/2+)
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>171m</sup>Au
| rowspan=2|<sup>171</sup>Au
| colspan="3" style="text-indent:2em" | 250(16) keV
| rowspan=2 style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 92
| 1.014(19) ms
| rowspan=2|170.991879(28)
| 11/2-
| rowspan=2|30(5) µs
|
| [[proton emission|p]]
|
| <sup>170</sup>Pt
| rowspan=2|(1/2+)
| rowspan=2|
| rowspan=2|
|-
|-
| [[alpha decay|α]] (rare)
| <sup>172</sup>Au
| <sup>167</sup>Ir
| style="text-align:right" | 79
| style="text-align:right" | 93
| 171.99004(17)#
| 4.7(11) ms
| high
|
|
|-
|-
| <sup>173</sup>Au
| rowspan=2 style="text-indent:1em" | <sup>171m</sup>Au
| style="text-align:right" | 79
| rowspan=2 colspan="3" style="text-indent:2em" | 250(16) keV
| rowspan=2|1.014(19) ms
| style="text-align:right" | 94
| 172.986237(28)
| α (54%)
| <sup>167</sup>Ir
| 25(1) ms
| (1/2+)
| rowspan=2|11/2-
| rowspan=2|
|
| rowspan=2|
|
|-
|-
| p (46%)
| style="text-indent:1em" | <sup>173m</sup>Au
| <sup>170</sup>Pt
| colspan="3" style="text-indent:2em" | 214(23) keV
| 14.0(9) ms
| (11/2-)
|
|
|-
|-
| <sup>174</sup>Au
| rowspan=2|<sup>172</sup>Au
| style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 79
| style="text-align:right" | 95
| rowspan=2 style="text-align:right" | 93
| 173.98476(11)#
| rowspan=2|171.99004(17)#
| 139(3) ms
| rowspan=2|4.7(11) ms
| α (98%)
| low
| <sup>168</sup>Ir
|
| rowspan=2|high
|
| rowspan=2|
| rowspan=2|
|-
| p (2%)
| <sup>171</sup>Pt
|-
| rowspan=2|<sup>173</sup>Au
| rowspan=2 style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 94
| rowspan=2|172.986237(28)
| rowspan=2|25(1) ms
| α
| <sup>169</sup>Ir
| rowspan=2|(1/2+)
| rowspan=2|
| rowspan=2|
|-
| [[beta decay|β<sup>+</sup>]] (rare)
| <sup>173</sup>Pt
|-
| rowspan=2 style="text-indent:1em" | <sup>173m</sup>Au
| rowspan=2 colspan="3" style="text-indent:2em" | 214(23) keV
| rowspan=2|14.0(9) ms
| α (96%)
| <sup>169</sup>Ir
| rowspan=2|(11/2-)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (4%)
| <sup>173</sup>Pt
|-
| rowspan=2|<sup>174</sup>Au
| rowspan=2 style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 95
| rowspan=2|173.98476(11)#
| rowspan=2|139(3) ms
| α
| <sup>170</sup>Ir
| rowspan=2|low
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (rare)
| <sup>174</sup>Pt
|-
|-
| style="text-indent:1em" | <sup>174m</sup>Au
| style="text-indent:1em" | <sup>174m</sup>Au
| colspan="3" style="text-indent:2em" | 360(70)# keV
| colspan="3" style="text-indent:2em" | 360(70)# keV
| 171(29) ms
| 171(29) ms
| high
|
|
|
|
| high
|-
| <sup>175</sup>Au
| style="text-align:right" | 79
| style="text-align:right" | 96
| 174.98127(5)
| 100# ms
| 1/2+#
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>175m</sup>Au
| rowspan=2|<sup>175</sup>Au
| colspan="3" style="text-indent:2em" | 200(30)# keV
| rowspan=2 style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 96
| 156(3) ms
| rowspan=2|174.98127(5)
| 11/2-#
| rowspan=2|100# ms
|
| α (82%)
|
| <sup>171</sup>Ir
| rowspan=2|1/2+#
| rowspan=2|
| rowspan=2|
|-
|-
| <sup>176</sup>Au
| β<sup>+</sup> (18%)
| <sup>175</sup>Pt
| style="text-align:right" | 79
|-
| style="text-align:right" | 97
| rowspan=2 style="text-indent:1em" | <sup>175m</sup>Au
| 175.98010(11)#
| rowspan=2 colspan="3" style="text-indent:2em" | 200(30)# keV
| 1.08(17) s [0.84(+17-14) s]
| rowspan=2|156(3) ms
| (5-)
|
| α
| <sup>171</sup>Ir
|
| rowspan=2|11/2-#
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup>
| <sup>175</sup>Pt
|-
| rowspan=2|<sup>176</sup>Au
| rowspan=2 style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 97
| rowspan=2|175.98010(11)#
| rowspan=2|1.08(17) s<br>[0.84(+17-14) s]
| α (60%)
| <sup>172</sup>Ir
| rowspan=2|(5-)
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (40%)
| <sup>176</sup>Pt
|-
|-
| style="text-indent:1em" | <sup>176m</sup>Au
| style="text-indent:1em" | <sup>176m</sup>Au
| colspan="3" style="text-indent:2em" | 150(100)# keV
| colspan="3" style="text-indent:2em" | 150(100)# keV
| 860(160) ms
| 860(160) ms
| (7+)
|
|
|
|
| (7+)
|-
| <sup>177</sup>Au
| style="text-align:right" | 79
| style="text-align:right" | 98
| 176.976865(14)
| 1462(32) ms
| (1/2+,3/2+)
|
|
|
|
|-
| 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)
| rowspan=2|1462(32) ms
| β<sup>+</sup> (60%)
| <sup>177</sup>Pt
| rowspan=2|(1/2+,3/2+)
| rowspan=2|
| rowspan=2|
|-
| α (40%)
| <sup>173</sup>Ir
|-
|-
| style="text-indent:1em" | <sup>177m</sup>Au
| style="text-indent:1em" | <sup>177m</sup>Au
| colspan="3" style="text-indent:2em" | 216(26) keV
| colspan="3" style="text-indent:2em" | 216(26) keV
| 1.180(12) s
| 1.180(12) s
| 11/2-
|
|
|
|
|-
| 11/2-
| <sup>178</sup>Au
| style="text-align:right" | 79
| style="text-align:right" | 99
| 177.97603(6)
| 2.6(5) s
|
|
|
|
|
|-
|-
| <sup>179</sup>Au
| rowspan=2|<sup>178</sup>Au
| style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 79
| style="text-align:right" | 100
| rowspan=2 style="text-align:right" | 99
| rowspan=2|177.97603(6)
| 178.973213(18)
| 7.1(3) s
| rowspan=2|2.6(5) s
| β<sup>+</sup> (60%)
| 5/2-#
| <sup>178</sup>Pt
|
| rowspan=2|
|
| rowspan=2|
| rowspan=2|
|-
| α (40%)
| <sup>174</sup>Ir
|-
| rowspan=2|<sup>179</sup>Au
| 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
| β<sup>+</sup> (78%)
| <sup>179</sup>Pt
| rowspan=2|5/2-#
| rowspan=2|
| rowspan=2|
|-
| α (22%)
| <sup>175</sup>Ir
|-
|-
| style="text-indent:1em" | <sup>179m</sup>Au
| style="text-indent:1em" | <sup>179m</sup>Au
| colspan="3" style="text-indent:2em" | 99(16) keV
| colspan="3" style="text-indent:2em" | 99(16) keV
|
|
| (11/2-)
|
|
|
|
|-
| (11/2-)
| <sup>180</sup>Au
| style="text-align:right" | 79
| style="text-align:right" | 101
| 179.972521(23)
| 8.1(3) s
|
|
|
|
|
|-
|-
| <sup>181</sup>Au
| rowspan=2|<sup>180</sup>Au
| style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 79
| style="text-align:right" | 102
| rowspan=2 style="text-align:right" | 101
| rowspan=2|179.972521(23)
| 180.970079(21)
| 13.7(14) s
| rowspan=2|8.1(3) s
| (3/2-)
| β<sup>+</sup> (98.2%)
| <sup>180</sup>Pt
|
| rowspan=2|
|
| rowspan=2|
| rowspan=2|
|-
|-
| α (1.8%)
| <sup>182</sup>Au
| <sup>176</sup>Ir
| style="text-align:right" | 79
| style="text-align:right" | 103
| 181.969618(22)
| 15.5(4) s
| (2+)
|
|
|-
|-
| <sup>183</sup>Au
| rowspan=2|<sup>181</sup>Au
| style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 79
| style="text-align:right" | 104
| rowspan=2 style="text-align:right" | 102
| rowspan=2|180.970079(21)
| 182.967593(11)
| 42.8(10) s
| rowspan=2|13.7(14) s
| β<sup>+</sup> (97.3%)
| (5/2)-
| <sup>181</sup>Pt
|
| rowspan=2|(3/2-)
|
| rowspan=2|
| rowspan=2|
|-
| α (2.7%)
| <sup>177</sup>Ir
|-
| rowspan=2|<sup>182</sup>Au
| rowspan=2 style="text-align:right" | 79
| rowspan=2 style="text-align:right" | 103
| rowspan=2|181.969618(22)
| rowspan=2|15.5(4) s
| β<sup>+</sup> (99.87%)
| <sup>182</sup>Pt
| rowspan=2|(2+)
| rowspan=2|
| rowspan=2|
|-
| α (.13%)
| <sup>178</sup>Ir
|-
| rowspan=2|<sup>183</sup>Au
| 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
| β<sup>+</sup> (99.2%)
| <sup>183</sup>Pt
| rowspan=2|(5/2)-
| rowspan=2|
| rowspan=2|
|-
| α (.8%)
| <sup>179</sup>Ir
|-
|-
| style="text-indent:1em" | <sup>183m1</sup>Au
| style="text-indent:1em" | <sup>183m1</sup>Au
| colspan="3" style="text-indent:2em" | 73.3(4) keV
| colspan="3" style="text-indent:2em" | 73.3(4) keV
| >1 µs
| >1 µs
|
|
| (1/2)+
| (1/2)+
|
|
Line 241: Line 339:
| colspan="3" style="text-indent:2em" | 230.6(6) keV
| colspan="3" style="text-indent:2em" | 230.6(6) keV
| <1 µs
| <1 µs
|
|
| (11/2)-
| (11/2)-
|
|
Line 250: Line 350:
| 183.967452(24)
| 183.967452(24)
| 20.6(9) s
| 20.6(9) s
| β<sup>+</sup>
| <sup>184</sup>Pt
| 5+
| 5+
|
|
|
|
|-
|-
| style="text-indent:1em" | <sup>184m</sup>Au
| rowspan=3 style="text-indent:1em" | <sup>184m</sup>Au
| 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
| β<sup>+</sup> (70%)
| 2+
| <sup>184</sup>Pt
|
| rowspan=3|2+
|
| rowspan=3|
| rowspan=3|
|-
|-
| [[Isomeric transition|IT]] (30%)
| <sup>185</sup>Au
| <sup>184</sup>Au
| style="text-align:right" | 79
|-
| style="text-align:right" | 106
| 184.965789(28)
| α (.013%)
| <sup>180</sup>Ir
| 4.25(6) min
| 5/2-
|-
| 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-
|
|
|-
|-
| style="text-indent:1em" | <sup>190m</sup>Au
| 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+
|
|
|-
|-
| style="text-indent:1em" | <sup>193m1</sup>Au
| 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-
|
|
|
|
|-
|-
| [[Gold-197|<sup>197</sup>Au]]
| <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+
  1. ^ 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

  1. ^ D. T. Win, M. Al Masum (2003). "Weapons of Mass Destruction" (PDF). Assumption University Journal of Technology. 6 (4): 199–219.
  2. ^ 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.
  3. ^ http://www.nucleonica.net/unc.aspx