鍅的同位素

鍅沒有穩定的同位素，因此無法得到其標準原子量，但鍅存在有兩個天然放射性同位素。目前已知的有35種鍅的同位素，原子量從199到233，其中最穩定的同位素是鍅-223（），半衰期為22分鐘，由於是鈾-235（）的衰變產物，因此在地殼中微量存在，而另一個自然同位素是，半衰期較短，只有4.9分鐘，目前已知穩定性最差的鍅同位素是，半衰期為86奈秒。

钫在前105个元素之中最不稳定。106号元素𬭳和之后的元素虽然比钫更不稳定，但因为目前发现的同位素数量不多，所以以后可能会发现更长寿的同位素。

 圖表 

|-
| 199Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 112
| 199.00726(4)
| 16(7) ms
|
|
| 1/2+#
|
|-
| 200Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 113
| 200.00657(8)
| 24(10) ms
| 
| 196At
| 3+#
|
|-
| rowspan=2 style="text-indent:1em" | 200mFr
| rowspan=2|
| rowspan=2 colspan="3" style="text-indent:2em" | 60(110) keV
| rowspan=2|650(210) ms
| 
| 196At
| rowspan=2|10−#
| rowspan=2|
|-
| IT （不常見）
| 200Fr
|-
| rowspan=2|201Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 114
| rowspan=2|201.00386(8)
| rowspan=2|67(3) ms
|  (99%)
| 197At
| rowspan=2|(9/2−)
| rowspan=2|
|-
|  (1%)
| 201Rn
|-
| rowspan=2|202Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 115
| rowspan=2|202.00337(5)
| rowspan=2|290(30) ms
|  (97%)
| 198At
| rowspan=2|(3+)
| rowspan=2|
|-
|  (3%)
| 202Rn
|-
| rowspan=2 style="text-indent:1em" | 202mFr
| rowspan=2|
| rowspan=2 colspan="3" style="text-indent:2em" | 330(90)# keV
| rowspan=2|340(40) ms
|  (97%)
| 198At
| rowspan=2|(10−)
| rowspan=2|
|-
|  (3%)
| 202Rn
|-
| rowspan=2|203Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 116
| rowspan=2|203.000925(17)
| rowspan=2|0.55(2) s
|  (95%)
| 199At
| rowspan=2|(9/2−)#
| rowspan=2|
|-
|  (5%)
| 203Rn
|-
| rowspan=2|204Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 117
| rowspan=2|204.000653(26)
| rowspan=2|1.7(3) s
|  (96%)
| 200At
| rowspan=2|(3+)
| rowspan=2|
|-
|  (4%)
| 204Rn
|-
| rowspan=2 style="text-indent:1em" | 204m1Fr
| rowspan=2|
| rowspan=2 colspan="3" style="text-indent:2em" | 50(4) keV
| rowspan=2|2.6(3) s
|  (90%)
| 200At
| rowspan=2|(7+)
| rowspan=2|
|-
|  (10%)
| 204Rn
|-
| style="text-indent:1em" | 204m2Fr
| 
| colspan="3" style="text-indent:2em" | 326(4) keV
| 1.7(6) s
|
|
| (10−)
| 
|-
| rowspan=2|205Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 118
| rowspan=2|204.998594(8)
| rowspan=2|3.80(3) s
|  (99%)
| 201At
| rowspan=2|(9/2−)
| rowspan=2|
|-
|  (1%)
| 205Rn
|-
| rowspan=2|206Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 119
| rowspan=2|205.99867(3)
| rowspan=2|~16 s
|  (58%)
| 206Rn
| rowspan=2|(2+,3+)
| rowspan=2|
|-
|  (42%)
| 202At
|-
| style="text-indent:1em" | 206m1Fr
| 
| colspan="3" style="text-indent:2em" | 190(40) keV
| 15.9(1) s
|
|
| (7+)
| 
|-
| style="text-indent:1em" | 206m2Fr
|
| colspan="3" style="text-indent:2em" | 730(40) keV
| 700(100) ms
|
|
| (10−)
|
|-
| rowspan=2|207Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 120
| rowspan=2|206.99695(5)
| rowspan=2|14.8(1) s
|  (95%)
| 203At
| rowspan=2|9/2−
| rowspan=2|
|-
|  (5%)
| 207Rn
|-
| rowspan=2|208Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 121
| rowspan=2|207.99714(5)
| rowspan=2|59.1(3) s
|  (90%)
| 204At
| rowspan=2|7+
| rowspan=2|
|-
|  (10%)
| 208Rn
|-
| rowspan=2|209Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 122
| rowspan=2|208.995954(16)
| rowspan=2|50.0(3) s
|  (89%)
| 205At
| rowspan=2|9/2−
| rowspan=2|
|-
|  (11%)
| 209Rn
|-
| rowspan=2|210Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 123
| rowspan=2|209.996408(24)
| rowspan=2|3.18(6) min
|  (60%)
| 206At
| rowspan=2|6+
| rowspan=2|
|-
|  (40%)
| 210Rn
|-
| rowspan=2|211Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 124
| rowspan=2|210.995537(23)
| rowspan=2|3.10(2) min
|  (80%)
| 207At
| rowspan=2|9/2−
| rowspan=2|
|-
|  (20%)
| 211Rn
|-
| rowspan=2|212Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 125
| rowspan=2|211.996202(28)
| rowspan=2|20.0(6) min
|  (57%)
| 212Rn
| rowspan=2|5+
| rowspan=2|
|-
|  (43%)
| 208At
|-
| rowspan=2|213Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 126
| rowspan=2|212.996189(8)
| rowspan=2|34.6(3) s
|  (99.45%)
| 209At
| rowspan=2|9/2−
| rowspan=2|
|-
|  (.55%)
| 213Rn
|-
| 214Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 127
| 213.998971(9)
| 5.0(2) ms
| 
| 210At
| (1−)
|
|-
| style="text-indent:1em" | 214m1Fr
|
| colspan="3" style="text-indent:2em" | 123(6) keV
| 3.35(5) ms
| 
| 210At
| (8−)
|
|-
| style="text-indent:1em" | 214m2Fr
|
| colspan="3" style="text-indent:2em" | 638(6) keV
| 103(4) ns
|
|
| (11+)
|
|-
| style="text-indent:1em" | 214m3Fr
|
| colspan="3" style="text-indent:2em" | 6477+Y keV
| 108(7) ns
|
|
| (33+)
|
|-
| 215Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 128
| 215.000341(8)
| 86(5) ns
| 
| 211At
| 9/2−
|
|-
| rowspan=2|216Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 129
| rowspan=2|216.003198(15)
| rowspan=2|0.70(2) µs
| 
| 212At
| rowspan=2|(1−)
| rowspan=2|
|-
|  (2×10−7%)
| 216Rn
|-
| 217Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 130
| 217.004632(7)
| 16.8(19) µs
| 
| 213At
| 9/2−
|
|-
| 218Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 131
| 218.007578(5)
| 1.0(6) ms
| 
| 214At
| 1−
|
|-
| rowspan=2 style="text-indent:1em" | 218m1Fr
| rowspan=2|
| rowspan=2 colspan="3" style="text-indent:2em" | 86(4) keV
| rowspan=2|22.0(5) ms
| 
| 214At
| rowspan=2|
| rowspan=2|
|-
| IT （不常見）
| 218Fr
|-
| style="text-indent:1em" | 218m2Fr
|
| colspan="3" style="text-indent:2em" | 200(150)# keV
|
|
|
| high
|
|-
| 219Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 132
| 219.009252(8)
| 20(2) ms
| 
| 215At
| 9/2−
|
|-
| rowspan=2|220Fr
| rowspan=2|
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 133
| rowspan=2|220.012327(4)
| rowspan=2|27.4(3) s
|  (99.65%)
| 216At
| rowspan=2|1+
| rowspan=2|
|-
|  (.35%)
| 220Ra
|-
| rowspan=3|221Fr
| rowspan=3|
| rowspan=3 style="text-align:right" | 87
| rowspan=3 style="text-align:right" | 134
| rowspan=3|221.014255(5)
| rowspan=3|4.9(2) min
|  (99.9%)
| 217At
| rowspan=3|5/2−
| rowspan=3|TraceIntermediate decay product of 237Np
|-
|  (.1%)
| 221Ra
|-
|  (8.79×10−11%)
| 207Tl
|-
| 222Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 135
| 222.017552(23)
| 14.2(3) min
| 
| 222Ra
| 2−
|
|-
| rowspan=2|223Fr
| rowspan=2|Actinium K
| rowspan=2 style="text-align:right" | 87
| rowspan=2 style="text-align:right" | 136
| rowspan=2|223.0197359(26)
| rowspan=2|22.00(7) min
|  (99.99%)
| 223Ra
| rowspan=2|3/2(−)
| rowspan=2|TraceIntermediate decay product of 235U
|-
|  (.006%)
| 219At
|-
| 224Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 137
| 224.02325(5)
| 3.33(10) min
| 
| 224Ra
| 1−
|
|-
| 225Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 138
| 225.02557(3)
| 4.0(2) min
| 
| 225Ra
| 3/2−
|
|-
| 226Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 139
| 226.02939(11)
| 49(1) s
| 
| 226Ra
| 1−
|
|-
| 227Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 140
| 227.03184(11)
| 2.47(3) min
| 
| 227Ra
| 1/2+
|
|-
| 228Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 141
| 228.03573(22)#
| 38(1) s
| 
| 228Ra
| 2−
|
|-
| 229Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 142
| 229.03845(4)
| 50.2(4) s
| 
| 229Ra
| (1/2+)#
|
|-
| 230Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 143
| 230.04251(48)#
| 19.1(5) s
| 
| 230Ra
|
|
|-
| 231Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 144
| 231.04544(50)#
| 17.6(6) s
| 
| 231Ra
| (1/2+)#
|
|-
| 232Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 145
| 232.04977(69)#
| 5(1) s
| 
| 232Ra
|
|
|-
| 233Fr
|
| style="text-align:right" | 87
| style="text-align:right" | 146
| 233.052518(21)
| 900(100) ms
| 
| 233Ra
| 1/2+ #
|
|}

 参考文獻 

 Isotope masses from Ame2003 Atomic Mass Evaluation by G. Audi, A.H. Wapstra, C. Thibault, J. Blachot and O. Bersillon in Nuclear Physics A729 (2003).
 Half-life, spin, and isomer data selected from these sources. Editing notes on this article's talk page.
 Audi, Bersillon, Blachot, Wapstra. The Nubase2003 evaluation of nuclear and decay properties , Nuc. Phys. A 729, pp. 3-128 (2003).
 National Nuclear Data Center, Brookhaven National Laboratory. Information extracted from the NuDat 2.1 database  (retrieved Sept. 2005).
 David R. Lide (ed.), Norman E. Holden in CRC Handbook of Chemistry and Physics, 85th Edition, online version. CRC Press. Boca Raton, Florida (2005). Section 11, Table of the Isotopes.

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