Redigerer Kvikksølvisotoper (avsnitt)

==Tabell==
{| class="wikitable" style="font-size:95%; white-space:nowrap"
! rowspan="2" | Atomkjerne-<br />symbol
! Z([[proton|p]])
! N([[nøytron|n]])
! &nbsp;<br />isotopmasse (u)<br />&nbsp;
! rowspan="2" | halveringstid
! rowspan="2" | Nedbrytings<br />metode(r)<ref>{{Kilde www |url=http://www.nucleonica.net/unc.aspx |tittel=Arkivert kopi |besøksdato=2011-07-01 |arkiv-dato=2017-02-19 |arkiv-url=https://web.archive.org/web/20170219043412/http://www.nucleonica.net/unc.aspx |url-status=yes }}</ref><ref group="n">Abbreviations:<br />EC: [[Elektroninnfanging]]<br />IT: [[Isomerisk transisjon]]</ref>
! rowspan="2" | Nedbrytings<br />produkt(er)<ref group="n">Uthevet for stabile isotoper</ref>
! rowspan="2" | Spinn
! rowspan="2" | Forholdsvis<br />isotopisk<br />sammensetning<br />(molfraksjon)
! rowspan="2" | spenn for naturlig<br />variasjon<br />(molfraksjon)
|-
! colspan="3" | [[Eksitasjon]]senergi
|-
| <sup>171</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 91
| 171,00376(32)#
| 80(30) µs<br />[59(+36-16) µs]
|
|
| 3/2-#
|
|
|-
| <sup>172</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 92
| 171,99883(22)
| 420(240) µs<br />[0,25(+35-9) ms]
|
|
| 0
|
|
|-
| <sup>173</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 93
| 172,99724(22)#
| 1,1(4) ms<br />[0,6(+5-2) ms]
|
|
| 3/2-#
|
|
|-
| <sup>174</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 94
| 173,992864(21)
| 2,0(4) ms<br />[2,1(+18-7) ms]
|
|
| 0+
|
|
|-
| <sup>175</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 95
| 174,99142(11)
| 10,8(4) ms
| [[alfastråling|α]]
| <sup>171</sup>Pt
| 5/2-#
|
|
|-
| rowspan=2|<sup>176</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 96
| rowspan=2|175,987355(15)
| rowspan=2|20,4(15) ms
| α (98,6 %)
| <sup>172</sup>Pt
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| [[betastråling|β<sup>+</sup>]] (1,4 %)
| <sup>176</sup>Au
|-
| rowspan=2|<sup>177</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 97
| rowspan=2|176,98628(8)
| rowspan=2|127,3(18) ms
| α (85 %)
| <sup>173</sup>Pt
| rowspan=2|5/2-#
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (15 %)
| <sup>177</sup>Au
|-
| rowspan=2|<sup>178</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 98
| rowspan=2|177,982483(14)
| rowspan=2|0,269(3) s
| α (70 %)
| <sup>174</sup>Pt
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (30 %)
| <sup>178</sup>Au
|-
| rowspan=3|<sup>179</sup>Hg
| rowspan=3 style="text-align:right" | 80
| rowspan=3 style="text-align:right" | 99
| rowspan=3|178,981834(29)
| rowspan=3|1,09(4) s
| α (53 %)
| <sup>175</sup>Pt
| rowspan=3|5/2-#
| rowspan=3|
| rowspan=3|
|-
| β<sup>+</sup> (47 %)
| <sup>179</sup>Au
|-
| β<sup>+</sup>, [[protonstråling|p]] (0,15 %)
| <sup>178</sup>Pt
|-
| rowspan=2|<sup>180</sup>Hg<ref group="n">Når framstilt fra <sup>180</sup>Tl kan isotopen også gjennomgå fisjon til '''<sup>100</sup>Ru''' and '''<sup>80</sup>Kr'''</ref>
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 100
| rowspan=2|179,978266(15)
| rowspan=2|2,58(1) s
| β<sup>+</sup> (52 %)
| <sup>180</sup>Au
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (48 %)
| <sup>176</sup>Pt
|-
| rowspan=4|<sup>181</sup>Hg
| rowspan=4 style="text-align:right" | 80
| rowspan=4 style="text-align:right" | 101
| rowspan=4|180,977819(17)
| rowspan=4|3,6(1) s
| β<sup>+</sup> (64 %)
| <sup>181</sup>Au
| rowspan=4|1/2(-)
| rowspan=4|
| rowspan=4|
|-
| α (36 %)
| <sup>177</sup>Pt
|-
| β<sup>+</sup>, p (0,014 %)
| <sup>180</sup>Pt
|-
| β<sup>+</sup>, α (9&times;10<sup>−6</sup> %)
| <sup>177</sup>Ir
|-
| style="text-indent:1em" | <sup>181m</sup>Hg
| colspan="3" style="text-indent:2em" | 210(40)# keV
|
|
|
| 13/2+
|
|
|-
| rowspan=3|<sup>182</sup>Hg
| rowspan=3 style="text-align:right" | 80
| rowspan=3 style="text-align:right" | 102
| rowspan=3|181,97469(1)
| rowspan=3|10,83(6) s
| β<sup>+</sup> (84,8 %)
| <sup>182</sup>Au
| rowspan=3|0+
| rowspan=3|
| rowspan=3|
|-
| α (15,2 %)
| <sup>178</sup>Pt
|-
| β<sup>+</sup>, p (10<sup>−5</sup> %)
| <sup>181</sup>Pt
|-
| rowspan=3|<sup>183</sup>Hg
| rowspan=3 style="text-align:right" | 80
| rowspan=3 style="text-align:right" | 103
| rowspan=3|182,974450(9)
| rowspan=3|9,4(7) s
| β<sup>+</sup> (74,5 %)
| <sup>183</sup>Au
| rowspan=3|1/2-
| rowspan=3|
| rowspan=3|
|-
| α (25,5 %)
| <sup>179</sup>Pt
|-
| β<sup>+</sup>, p (5.6&times;10<sup>−4</sup> %)
| <sup>182</sup>Pt
|-
| style="text-indent:1em" | <sup>183m1</sup>Hg
| colspan="3" style="text-indent:2em" | 198(14) keV
|
|
|
| 13/2+#
|
|
|-
| style="text-indent:1em" | <sup>183m2</sup>Hg
| colspan="3" style="text-indent:2em" | 240(40)# keV
| 5# s
| β<sup>+</sup>
| <sup>183</sup>Au
| 13/2+#
|
|
|-
| rowspan=2|<sup>184</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 104
| rowspan=2|183,971713(11)
| rowspan=2|30,6(3) s
| β<sup>+</sup> (98,89 %)
| <sup>184</sup>Au
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (1,11 %)
| <sup>180</sup>Pt
|-
| rowspan=2|<sup>185</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 105
| rowspan=2|184,971899(17)
| rowspan=2|49,1(10) s
| β<sup>+</sup> (94 %)
| <sup>185</sup>Au
| rowspan=2|1/2-
| rowspan=2|
| rowspan=2|
|-
| α (6 %)
| <sup>181</sup>Pt
|-
| rowspan=3 style="text-indent:1em" | <sup>185m</sup>Hg
| rowspan=3 colspan="3" style="text-indent:2em" | 99.3(5) keV
| rowspan=3|21,6(15) s
| [[Isomeric transition|IT]] (54 %)
| <sup>185</sup>Hg
| rowspan=3|13/2+
| rowspan=3|
| rowspan=3|
|-
| β<sup>+</sup> (46 %)
| <sup>185</sup>Au
|-
| α (0,03 %)
| <sup>181</sup>Pt
|-
| rowspan=2|<sup>186</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 106
| rowspan=2|185,969362(12)
| rowspan=2|1,38(6) min
| β<sup>+</sup> (99,92 %)
| <sup>186</sup>Au
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (0,016 %)
| <sup>182</sup>Pt
|-
| style="text-indent:1em" | <sup>186m</sup>Hg
| colspan="3" style="text-indent:2em" | 2217.3(4) keV
| 82(5) µs
|
|
| (8-)
|
|
|-
| rowspan=2|<sup>187</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 107
| rowspan=2|186,969814(15)
| rowspan=2|1,9(3) min
| β<sup>+</sup>
| <sup>187</sup>Au
| rowspan=2|3/2-
| rowspan=2|
| rowspan=2|
|-
| α (1.2&times;10<sup>−4</sup> %)
| <sup>183</sup>Pt
|-
| rowspan=2 style="text-indent:1em" | <sup>187m</sup>Hg
| rowspan=2 colspan="3" style="text-indent:2em" | 59(16) keV
| rowspan=2|2,4(3) min
| β<sup>+</sup>
| <sup>187</sup>Au
| rowspan=2|13/2+
| rowspan=2|
| rowspan=2|
|-
| α (2,5&times;10<sup>−4</sup> %)
| <sup>183</sup>Pt
|-
| rowspan=2|<sup>188</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 108
| rowspan=2|187,967577(12)
| rowspan=2|3,25(15) min
| β<sup>+</sup>
| <sup>188</sup>Au
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (3,7&times;10<sup>−5</sup> %)
| <sup>184</sup>Pt
|-
| style="text-indent:1em" | <sup>188m</sup>Hg
| colspan="3" style="text-indent:2em" | 2724.3(4) keV
| 134(15) ns
|
|
| (12+)
|
|
|-
| rowspan=2|<sup>189</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 109
| rowspan=2|188,96819(4)
| rowspan=2|7,6(1) min
| β<sup>+</sup>
| <sup>189</sup>Au
| rowspan=2|3/2-
| rowspan=2|
| rowspan=2|
|-
| α (3&times;10<sup>−5</sup> %)
| <sup>185</sup>Pt
|-
| rowspan=2 style="text-indent:1em" | <sup>189m</sup>Hg
| rowspan=2 colspan="3" style="text-indent:2em" | 80(30) keV
| rowspan=2|8,6(1) min
| β<sup>+</sup>
| <sup>189</sup>Au
| rowspan=2|13/2+
| rowspan=2|
| rowspan=2|
|-
| α (3&times;10<sup>−5</sup> %)
| <sup>185</sup>Pt
|-
| rowspan=2|<sup>190</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 110
| rowspan=2|189,966322(17)
| rowspan=2|20,0(5) min
| β<sup>+</sup>
| <sup>190</sup>Au
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (5&times;10<sup>−5</sup> %)
| <sup>186</sup>Pt
|-
| <sup>191</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 111
| 190,967157(24)
| 49(10) min
| β<sup>+</sup>
| <sup>191</sup>Au
| 3/2(-)
|
|
|-
| style="text-indent:1em" | <sup>191m</sup>Hg
| colspan="3" style="text-indent:2em" | 128(22) keV
| 50,8(15) min
| β<sup>+</sup>
| <sup>191</sup>Au
| 13/2+
|
|
|-
| rowspan=2|<sup>192</sup>Hg
| rowspan=2 style="text-align:right" | 80
| rowspan=2 style="text-align:right" | 112
| rowspan=2|191,965634(17)
| rowspan=2|4,85(20) h
| [[Elektroninnfanging|EC]]
| <sup>192</sup>Au
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| α (4&times;10<sup>−6</sup> %)
| <sup>188</sup>Pt
|-
| <sup>193</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 113
| 192,966665(17)
| 3,80(15) h
| β<sup>+</sup>
| <sup>193</sup>Au
| 3/2-
|
|
|-
| rowspan=2 style="text-indent:1em" | <sup>193m</sup>Hg
| rowspan=2 colspan="3" style="text-indent:2em" | 140.76(5) keV
| rowspan=2|11,8(2) h
| β<sup>+</sup> (92,9 %)
| <sup>193</sup>Au
| rowspan=2|13/2+
| rowspan=2|
| rowspan=2|
|-
| IT (7,1 %)
| <sup>193</sup>Hg
|-
| <sup>194</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 114
| 193,965439(13)
| 444(77) a
| EC
| <sup>194</sup>Au
| 0+
|
|
|-
| <sup>195</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 115
| 194,966720(25)
| 10,53(3) h
| β<sup>+</sup>
| <sup>195</sup>Au
| 1/2-
|
|
|-
| rowspan=2 style="text-indent:1em" | <sup>195m</sup>Hg
| rowspan=2 colspan="3" style="text-indent:2em" | 176.07(4) keV
| rowspan=2|41,6(8) h
| IT (54,2 %)
| <sup>195</sup>Hg
| rowspan=2|13/2+
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup> (45,8 %)
| <sup>195</sup>Au
|-
| <sup>196</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 116
| 195,965833(3)
| colspan=3 align=center|'''Stabilt'''<ref group="n">Antas å gjennomgå en α-nedbrytning til '''<sup>192</sup>Pt''' eller β<sup>+</sup>β<sup>+</sup>-nedbryting til '''<sup>196</sup>Pt''', med en halveringstid på 2,5&times;10<sup>18</sup> år</ref>
| 0+ 
| 0,0015(1)
|
|-
| <sup>197</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 117
| 196,967213(3)
| 64,14(5) h
| EC
| '''<sup>197</sup>Au'''
| 1/2-
|
|
|-
| rowspan=2 style="text-indent:1em" | <sup>197m</sup>Hg
| rowspan=2 colspan="3" style="text-indent:2em" | 298.93(8) keV
| rowspan=2|23,8(1) h
| IT (91,4 %)
| <sup>197</sup>Hg
| rowspan=2|13/2+
| rowspan=2|
| rowspan=2|
|-
| EC (8,6 %)
| '''<sup>197</sup>Au'''
|-
| <sup>198</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 118
| 197,9667690(4)
| colspan=3 align=center|'''Stabilt'''<ref group="n">Antas å gjennomgå en α-nedbryting til '''<sup>194</sup>Pt'''</ref>
| 0+
| 0,0997(20)
|
|-
| <sup>199</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 119
| 198,9682799(4)
| colspan=3 align=center|'''Stabilt'''<ref group="n">Antas å gjennomgå en α-nedbryting til '''<sup>195</sup>Pt'''</ref>
| 1/2-
| 0,1687(22)
|
|-
| style="text-indent:1em" | <sup>199m</sup>Hg
| colspan="3" style="text-indent:2em" | 532,48(10) keV
| 42,66(8) min
| IT
| <sup>199</sup>Hg
| 13/2+
|
|
|-
| <sup>200</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 120
| 199,9683260(4)
| colspan=3 align=center|'''Stabilt'''<ref group="n">Antas å gjennomgå en α-nedbryting til '''<sup>196</sup>Pt'''</ref>
| 0+
| 0,2310(19)
|
|-
| <sup>201</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 121
| 200,9703023(6)
| colspan=3 align=center|'''Stabilt'''<ref group="n">Antas å gjennomgå en α-nedbryting til <sup>197</sup>Pt</ref>
| 3/2-
| 0,1318(9)
|
|-
| style="text-indent:1em" | <sup>201m</sup>Hg
| colspan="3" style="text-indent:2em" | 766,22(15) keV
| 94(3) µs
|
|
| 13/2+
|
|
|-
| <sup>202</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 122
| 201,9706430(6)
| colspan=3 align=center|'''Stabilt'''<ref group="n">Antas å gjennomgå en α-nedbryting til '''<sup>198</sup>Pt'''</ref>
| 0+
| 0,2986(26)
|
|-
| <sup>203</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 123
| 202,9728725(18)
| 46,595(6) d
| β<sup>-</sup>
| '''<sup>203</sup>Tl'''
| 5/2-
|
|
|-
| style="text-indent:1em" | <sup>203m</sup>Hg
| colspan="3" style="text-indent:2em" | 933.14(23) keV
| 24(4) µs
|
|
| (13/2+)
|
|
|-
| <sup>204</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 124
| 203,9734939(4)
| colspan=3 align=center|'''Stabilt'''<ref group="n">Antas å gjennomgå en α-nedbryting til <sup>200</sup>Pt eller β<sup>-</sup>β<sup>-</sup>-nedbrytning til '''<sup>204</sup>Pb'''</ref>
| 0+
| 0.0687(15)
|
|-
| <sup>205</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 125
| 204,976073(4)
| 5,14(9) min
| β<sup>-</sup>
| '''<sup>205</sup>Tl'''
| 1/2-
|
|
|-
| style="text-indent:1em" | <sup>205m</sup>Hg
| colspan="3" style="text-indent:2em" | 1556,40(17) keV
| 1,09(4) ms
| IT
| <sup>205</sup>Hg
| 13/2+
|
|
|-
| <sup>206</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 126
| 205,977514(22)
| 8,15(10) min
| β<sup>-</sup>
| <sup>206</sup>Tl
| 0+
|
|
|-
| <sup>207</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 127
| 206,98259(16)
| 2,9(2) min
| β<sup>-</sup>
| <sup>207</sup>Tl
| (9/2+)
|
|
|-
| <sup>208</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 128
| 207,98594(32)#
| 42(5) min<br />[41(+5-4) min]
| β<sup>-</sup>
| <sup>208</sup>Tl
| 0+
|
|
|-
| <sup>209</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 129
| 208,99104(21)#
| 37(8) s
|
|
| 9/2+#
|
|
|-
| <sup>210</sup>Hg
| style="text-align:right" | 80
| style="text-align:right" | 130
| 209,99451(32)#
| 10# min<br />[>300 ns]
|
|
| 0+
|
|
|}

===Fotnoter===
<references group="n" />

===Merknader===
*Verdier merket med # er ikke utelukkende avledet fra forsøksdata, men i det minste delvis fra systematiske trender. Spinn med omdiskuterte verdier er tatt med i parentes.
*Usikre verdier er oppgitte i parentes etter siste siffer. Usikre verdier betegnes med standardavvik, med unntak av isotoper og standard atommasse fra IUPAC, som benytter utvidede sikkerhetsmarginer.