鉬的同位素

鉬（原子量：95.94(2)）共有33個同位素和四个同核异构体，原子量在83至115之间，其中有6個同位素是穩定的。其中有七个同位素存在于自然界，分别是92Mo、94Mo、95Mo、96Mo、97Mo、98Mo以及放射性的100Mo。

圖表

|-
| rowspan=2|83Mo
| rowspan=2 style="text-align:right" | 42
| rowspan=2 style="text-align:right" | 41
| rowspan=2|82.94874(54)#
| rowspan=2|23(19) ms[6(+30-3) ms]molybdenum-83 :Table of Nuclides  Brookhaven National Laboratory Interactive, nndc.bnl.gov [2015-9-14]
| , 
|  82Zr
| rowspan=2|3/2-#
| rowspan=2|
| rowspan=2|
|-
| 
| 83Nb
|-
| 84Mo
| style="text-align:right" | 42
| style="text-align:right" | 42
| 83.94009(43)#
| 3.8(9) ms[3.7(+10-8) s]
| 
| 84Nb
| 0+
|
|
|-
| 85Mo
| style="text-align:right" | 42
| style="text-align:right" | 43
| 84.93655(30)#
| 3.2(2) s
| 
| 85Nb
| (1/2-)#
|
|
|-
| 86Mo
| style="text-align:right" | 42
| style="text-align:right" | 44
| 85.93070(47)
| 19.6(11) s
| 
| 86Nb
| 0+
|
|
|-
| rowspan=2|87Mo
| rowspan=2 style="text-align:right" | 42
| rowspan=2 style="text-align:right" | 45
| rowspan=2|86.92733(24)
| rowspan=2|14.05(23) s
|  (85%)
| 87Nb
| rowspan=2|7/2+#
| rowspan=2|
| rowspan=2|
|-
| ,  (15%)
| 86Zr
|-
| 88Mo
| style="text-align:right" | 42
| style="text-align:right" | 46
| 87.921953(22)
| 8.0(2) min
| 
| 88Nb
| 0+
|
|
|-
| 89Mo
| style="text-align:right" | 42
| style="text-align:right" | 47
| 88.919480(17)
| 2.11(10) min
| 
| 89Nb
| (9/2+)
|
|
|-
| style="text-indent:1em" | 89mMo
| colspan="3" style="text-indent:2em" | 387.5(2) keV
| 190(15) ms
| IT
| 89Mo
| (1/2-)
|
|
|-
| 90Mo
| style="text-align:right" | 42
| style="text-align:right" | 48
| 89.913937(7)
| 5.56(9) h
| 
| 90Nb
| 0+
|
|
|-
| style="text-indent:1em" | 90mMo
| colspan="3" style="text-indent:2em" | 2874.73(15) keV
| 1.12(5) µs
|
|
| 8+#
|
|
|-
| 91Mo
| style="text-align:right" | 42
| style="text-align:right" | 49
| 90.911750(12)
| 15.49(1) min
| 
| 91Nb
| 9/2+
|
|
|-
| rowspan=2 style="text-indent:1em" | 91mMo
| rowspan=2 colspan="3" style="text-indent:2em" | 653.01(9) keV
| rowspan=2|64.6(6) s
| IT (50.1%)
| 91Mo
| rowspan=2|1/2-
| rowspan=2|
| rowspan=2|
|-
|  (49.9%)
| 91Nb
|-
| 92Mo
| style="text-align:right" | 42
| style="text-align:right" | 50
| 91.906811(4)
| colspan=3 align=center|觀測上穩定Believed to decay by  to 92Zr with a half-life over 1.9×1020 years
| 0+
|  0.14649(106)
|
|-
| style="text-indent:1em" | 92mMo
| colspan="3" style="text-indent:2em" | 2760.46(16) keV
| 190(3) ns
|
|
| 8+
|
|
|-
| 93Mo
| style="text-align:right" | 42
| style="text-align:right" | 51
| 92.906813(4)
| 4,000(800) a
| 
| 93Nb
| 5/2+
|
|
|-
| rowspan=2 style="text-indent:1em" | 93mMo
| rowspan=2 colspan="3" style="text-indent:2em" | 2424.89(3) keV
| rowspan=2|6.85(7) h
| IT (99.88%)
| 93Mo
| rowspan=2|21/2+
| rowspan=2|
| rowspan=2|
|-
|  (.12%)
| 93Nb
|-
| 94Mo
| style="text-align:right" | 42
| style="text-align:right" | 52
| 93.9050883(21)
| colspan=3 align=center|
| 0+
|  0.09187(33)
|
|-
| 95MoFission product
| style="text-align:right" | 42
| style="text-align:right" | 53
| 94.9058421(21)
| colspan=3 align=center|
| 5/2+
| 0.15873(30)
|
|-
| 96Mo
| style="text-align:right" | 42
| style="text-align:right" | 54
| 95.9046795(21)
| colspan=3 align=center|
| 0+
| 0.16673(30)
|
|-
| 97Mo
| style="text-align:right" | 42
| style="text-align:right" | 55
| 96.9060215(21)
| colspan=3 align=center|
| 5/2+
| 0.09582(15)
|
|-
|
| style="text-align:right" | 42
| style="text-align:right" | 56
| 97.9054082(21)
| colspan=3 align=center|觀測上穩定Believed to decay by  to 98Ru with a half-life of over 1×1014 years
| 0+
| 0.24292(80)
|
|-
| 99MoUsed to produce the medically useful radioisotope technetium-99m
| style="text-align:right" | 42
| style="text-align:right" | 57
| 98.9077119(21)
| 2.7489(6) d
| 
| 99mTc
| 1/2+
|
|
|-
| style="text-indent:1em" | 99m1Mo
| colspan="3" style="text-indent:2em" | 97.785(3) keV
| 15.5(2) µs
|
|
| 5/2+
|
|
|-
| style="text-indent:1em" | 99m2Mo
| colspan="3" style="text-indent:2em" | 684.5(4) keV
| 0.76(6) µs
|
|
| 11/2-
|
|
|-
| 100MoPrimordial radionuclide
| style="text-align:right" | 42
| style="text-align:right" | 58
| 99.907477(6)
| 8.5(5)×1018 a
| 
| 100Ru
| 0+
| 0.09744(65)
|
|-
| 101Mo
| style="text-align:right" | 42
| style="text-align:right" | 59
| 100.910347(6)
| 14.61(3) min
| 
| 101Tc
| 1/2+
|
|
|-
| 102Mo
| style="text-align:right" | 42
| style="text-align:right" | 60
| 101.910297(22)
| 11.3(2) min
| 
| 102Tc
| 0+
|
|
|-
| 103Mo
| style="text-align:right" | 42
| style="text-align:right" | 61
| 102.91321(7)
| 67.5(15) s
| 
| 103Tc
| (3/2+)
|
|
|-
| 104Mo
| style="text-align:right" | 42
| style="text-align:right" | 62
| 103.91376(6)
| 60(2) s
| 
| 104Tc
| 0+
|
|
|-
| 105Mo
| style="text-align:right" | 42
| style="text-align:right" | 63
| 104.91697(8)
| 35.6(16) s
| 
| 105Tc
| (5/2-)
|
|
|-
| 106Mo
| style="text-align:right" | 42
| style="text-align:right" | 64
| 105.918137(19)
| 8.73(12) s
| 
| 106Tc
| 0+
|
|
|-
| 107Mo
| style="text-align:right" | 42
| style="text-align:right" | 65
| 106.92169(17)
| 3.5(5) s
| 
| 107Tc
| (7/2-)
|
|
|-
| style="text-indent:1em" | 107mMo
| colspan="3" style="text-indent:2em" | 66.3(2) keV
| 470(30) ns
|
|
| (5/2-)
|
|
|-
| 108Mo
| style="text-align:right" | 42
| style="text-align:right" | 66
| 107.92345(21)#
| 1.09(2) s
| 
| 108Tc
| 0+
|
|
|-
| 109Mo
| style="text-align:right" | 42
| style="text-align:right" | 67
| 108.92781(32)#
| 0.53(6) s
| 
| 109Tc
| (7/2-)#
|
|
|-
| rowspan=2|110Mo
| rowspan=2 style="text-align:right" | 42
| rowspan=2 style="text-align:right" | 68
| rowspan=2|109.92973(43)#
| rowspan=2|0.27(1) s
|  (>99.9%)
| 110Tc
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| ,  (<.1%)
| 109Tc
|-
| 111Mo
| style="text-align:right" | 42
| style="text-align:right" | 69
| 110.93441(43)#
| 200# ms[>300 ns]
| 
| 111Tc
|
|
|
|-
| 112Mo
| style="text-align:right" | 42
| style="text-align:right" | 70
| 111.93684(64)#
| 150# ms[>300 ns]
| 
| 112Tc
| 0+
|
|
|-
| 113Mo
| style="text-align:right" | 42
| style="text-align:right" | 71
| 112.94188(64)#
| 100# ms[>300 ns]
| 
| 113Tc
|
|
|
|-
| 114Mo
| style="text-align:right" | 42
| style="text-align:right" | 72
| 113.94492(75)#
| 80# ms[>300 ns]
|
|
| 0+
|
|
|-
| 115Mo
| style="text-align:right" | 42
| style="text-align:right" | 73
| 114.95029(86)#
| 60# ms[>300 ns]
|
|
|
|
|
|-
| rowspan=2|116Mo
| rowspan=2 style="text-align:right" | 42
| rowspan=2 style="text-align:right" | 74
| rowspan=2|(116)#
| rowspan=2|> 391 ns
| 
| 116Tc
| rowspan=2|0+molybdenum-116 :Table of Nuclides  Brookhaven National Laboratory Interactive, nndc.bnl.gov [2015-9-14]
| rowspan=2|
| rowspan=2|
|-
| , 
| 115Tc
|-
| rowspan=3|117Mo
| rowspan=3 style="text-align:right" | 42
| rowspan=3 style="text-align:right" | 75
| rowspan=3|(117)#
| rowspan=3|(> 393) nsmolybdenum-117 :Table of Nuclides  Brookhaven National Laboratory Interactive, nndc.bnl.gov [2015-9-14]
| , 2
| 
| rowspan=3|
| rowspan=3|
| rowspan=3|
|-
| , 
| 
|-
| 
| 
|-
| 118Mo
| style="text-align:right" | 42
| style="text-align:right" | 76
| (118)#
| 
|
|
|
|
|
|}

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).
 Isotopic compositions and standard atomic masses from Atomic weights of the elements. Review 2000 (IUPAC Technical Report) . Pure Appl. Chem. Vol. 75, No. 6, pp. 683-800, (2003) and Atomic Weights Revised (2005) .
 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.

Mo
Category:钼