释义 |
- List of isotopes Notes
- References
{{infobox radon isotopes}}There are 35 known isotopes of radon (86Rn) from 195Rn to 229Rn; all are radioactive. The most stable isotope is 222Rn with a half-life of 3.823 days, which decays into {{SimpleNuclide2|Polonium|218|link=yes}}. Four isotopes of radon, 218, 219, 220, 222Rn occur in trace quantities in nature as decay products of, respectively, 218At, 223Ra, 224Ra, and 226Ra. 218Rn and 222Rn are intermediate steps in the decay chain for 238U, 219Rn is an intermediate step in the decay chain for 235U, and 220Rn occurs in the decay chain for 232Th. List of isotopes nuclide symbol | historic name | Z(p) | N(n) | isotopic mass (u) | half-life | decay mode(s)[1][2] | daughter isotope(s) | nuclear spin and parity | representative isotopic composition (mole fraction) | range of natural variation (mole fraction) | excitation energy |
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195Rn | 86 | 109 | 195.00544(5) | 6 ms | 3/2−# | 195mRn | 50(50) keV | 6 ms | 13/2+# | 196Rn | | 86 | 110 | 196.002115(16) | 4.7(11) ms [4.4(+13−9) ms] | α | 192Po | 0+ | | | β+ (rare) | 196At | 197Rn | | 86 | 111 | 197.00158(7) | 66(16) ms [65(+23−14) ms] | α | 193Po | 3/2−# | | | β+ (rare) | 197At | 197mRn | | 200(60)# keV | 21(5) ms [19(+8−4) ms] | α | 193Po | (13/2+) | | | β+ (rare) | 197At | 198Rn | | 86 | 112 | 197.998679(14) | 65(3) ms | α (99%) | 194Po | 0+ | | | β+ (1%) | 198At | 199Rn | | 86 | 113 | 198.99837(7) | 620(30) ms | α (94%) | 195Po | 3/2−# | | | β+ (6%) | 199At | 199mRn | | 180(70) keV | 320(20) ms | α (97%) | 195Po | 13/2+# | | | β+ (3%) | 199At | 200Rn | | 86 | 114 | 199.995699(14) | 0.96(3) s | α (98%) | 196Po | 0+ | | | β+ (2%) | 200At | 201Rn | | 86 | 115 | 200.99563(8) | 7.0(4) s | α (80%) | 197Po | (3/2−) | | | β+ (20%) | 201At | 201mRn | | 280(90)# keV | 3.8(1) s | α (90%) | 197Po | (13/2+) | | | β+ (10%) | 201At | IT (<1%) | 201Rn | 202Rn | | 86 | 116 | 201.993263(19) | 9.94(18) s | α (85%) | 198Po | 0+ | | | β+ (15%) | 202At | 203Rn | | 86 | 117 | 202.993387(25) | 44.2(16) s | α (66%) | 199Po | (3/2−) | | | β+ (34%) | 203At | 203mRn | | 363(4) keV | 26.7(5) s | α (80%) | 199Po | 13/2(+) | | | β+ (20%) | 203At | 204Rn | | 86 | 118 | 203.991429(16) | 1.17(18) min | α (73%) | 200Po | 0+ | | | β+ (27%) | 204At | 205Rn | | 86 | 119 | 204.99172(5) | 170(4) s | β+ (77%) | 205At | 5/2− | | | α (23%) | 201Po | 206Rn | | 86 | 120 | 205.990214(16) | 5.67(17) min | α (62%) | 202Po | 0+ | | | β+ (38%) | 206At | 207Rn | | 86 | 121 | 206.990734(28) | 9.25(17) min | β+ (79%) | 207At | 5/2− | | | α (21%) | 203Po | 207mRn | 899.0(10) keV | 181(18) µs | (13/2+) | 208Rn | | 86 | 122 | 207.989642(12) | 24.35(14) min | α (62%) | 204Po | 0+ | | | β+ (38%) | 208At | 209Rn | | 86 | 123 | 208.990415(21) | 28.5(10) min | β+ (83%) | 209At | 5/2− | | | α (17%) | 205Po | 209m1Rn | 1173.98(13) keV | 13.4(13) µs | 13/2+ | 209m2Rn | 3636.78(23) keV | 3.0(3) µs | (35/2+) | 210Rn | | 86 | 124 | 209.989696(9) | 2.4(1) h | α (96%) | 206Po | 0+ | | | β+ (4%) | 210At | 210m1Rn | 1690(15) keV | 644(40) ns | 8+# | 210m2Rn | 3837(15) keV | 1.06(5) µs | (17)− | 210m3Rn | 6493(15) keV | 1.04(7) µs | (22)+ | 211Rn | | 86 | 125 | 210.990601(7) | 14.6(2) h | α (72.6%) | 207Po | 1/2− | | | β+ (27.4%) | 211At | 212Rn | | 86 | 126 | 211.990704(3) | 23.9(12) min | α | 208Po | 0+ | | | β+β+ (rare) | 212Po | 213Rn | 86 | 127 | 212.993883(6) | 19.5(1) ms | α | 209Po | (9/2+) | 214Rn | | 86 | 128 | 213.995363(10) | 0.27(2) µs | α | 210Po | 0+ | | | β+β+ (rare) | 214Po | 214mRn | 4595.4 keV | 245(30) ns | (22+) | 215Rn | 86 | 129 | 214.998745(8) | 2.30(10) µs | α | 211Po | 9/2+ | 216Rn | 86 | 130 | 216.000274(8) | 45(5) µs | α | 212Po | 0+ | 217Rn | 86 | 131 | 217.003928(5) | 0.54(5) ms | α | 213Po | 9/2+ | 218Rn | 86 | 132 | 218.0056013(25) | 35(5) ms | α | 214Po | 0+ | Trace[3] | 219Rn | Actinon Actinium emanation | 86 | 133 | 219.0094802(27) | 3.96(1) s | α | 215Po | 5/2+ | Trace[4] | 220Rn | Thoron Thorium emanation | 86 | 134 | 220.0113940(24) | 55.6(1) s | α | 216Po | 0+ | Trace[5] | | β−β− (rare) | 220Ra | 221Rn | | 86 | 135 | 221.015537(6) | 25.7(5) min | β− (78%) | 221Fr | 7/2(+) | | | α (22%) | 217Po | 222Rn | Radon[6] Radium emanation Emanation Emanon Niton | 86 | 136 | 222.0175777(25) | 3.8235(3) d | α | 218Po | 0+ | Trace[3] | 223Rn | 86 | 137 | 223.02179(32)# | 24.3(4) min | β− | 223Fr | 7/2 | 224Rn | 86 | 138 | 224.02409(32)# | 107(3) min | β− | 224Fr | 0+ | 225Rn | 86 | 139 | 225.02844(32)# | 4.66(4) min | β− | 225Fr | 7/2− | 226Rn | 86 | 140 | 226.03089(43)# | 7.4(1) min | β− | 226Fr | 0+ | 227Rn | 86 | 141 | 227.03541(45)# | 20.8(7) s | β− | 227Fr | 5/2(+#) | 228Rn | 86 | 142 | 228.03799(44)# | 65(2) s | β− | 228Fr | 0+ | 229Rn[7] | 86 | 143 | 229.0426536(141) | 12(1) s | β− | 229Fr |
1. ^{{cite web |url=http://www.nucleonica.net/unc.aspx |title=Universal Nuclide Chart |publisher=nucleonica |registration=yes}} 2. ^Abbreviations: IT: Isomeric transition 3. ^1 Intermediate decay product of 238U 4. ^Intermediate decay product of 235U 5. ^Intermediate decay product of 232Th 6. ^Source of element's name 7. ^{{cite journal |last1=Neidherr |first1=D. |last2=Audi |first2=G. |first3=D. |last3=Beck |first4=K. |last4=Baum |first5=Ch. |last5=Böhm |first6=M. |last6=Breitenfeldt |first7=R. B. |last7=Cakirli |first8=R. F. |last8=Casten |first9=S. |last9=George |first10=F. |last10=Herfurth |first11=A. |last11=Herlert |first12=A. |last12=Kellerbauer |first13=M. |last13=Kowalska |first14=D. |last14=Lunney |first15=E. |last15=Minaya-Ramirez |first16=S. |last16=Naimi |first17=E. |last17=Noah |first18=L. |last18=Penescu |first19=M. |last19=Rosenbusch |first20=S. |last20=Schwarz |first21=L. |last21=Schweikhard |first22=T. |last22=Stora |date=19 March 2009 |title=Discovery of 229Rn and the Structure of the Heaviest Rn and Ra Isotopes from Penning-Trap Mass Measurements |journal=Physical Review Letters |volume=102 |issue=11 |pages=112501–1–112501–5 |doi=10.1103/PhysRevLett.102.112501|pmid=19392194 |bibcode=2009PhRvL.102k2501N |url=http://cds.cern.ch/record/1190495/files/PhysRevLett.102.112501.pdf }}
Notes - Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
- Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use expanded uncertainties.
References - Isotope masses from:
- Isotopic compositions and standard atomic masses from:
- {{CAWIA 2003}}
- {{CIAAW 2005}}
- Half-life, spin, and isomer data selected from the following sources. See editing notes on this article's talk page.
- {{NUBASE 2003}}
- {{NNDC}}
- {{CRC85|chapter=11}}
{{Navbox element isotopes}} 3 : Radon|Isotopes of radon|Lists of isotopes by element |