銀的同位素

銀（原子量：107.8682(2)）共有74個同位素，其中有2個同位素是穩定的。

 圖表 

|-
| 93Ag
| style="text-align:right" | 47
| style="text-align:right" | 46
| 92.94978(64)#
| 5# ms[>1.5 µs]
|
|
| 9/2+#
|
|
|-
| 94Ag
| style="text-align:right" | 47
| style="text-align:right" | 47
| 93.94278(54)#
| 37(18) ms[26(+26-9) ms]
| 
| 94Pd
| 0+#
|
|
|-
| rowspan=2 style="text-indent:1em" | 94m1Ag
| rowspan=2 colspan="3" style="text-indent:2em" | 1350(400)# keV
| rowspan=2|422(16) ms
|  (>99.9%)
| 94Pd
| rowspan=2|(7+)
| rowspan=2|
| rowspan=2| 
|-
| ,  (<.1%)
| 93Rh
|-
| style="text-indent:1em" | 94m2Ag
| colspan="3" style="text-indent:2em" | 6500(2000)# keV
| 300(200) ms
|
|
| (21+)
|
|
|-
| rowspan=2|95Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 48
| rowspan=2|94.93548(43)#
| rowspan=2|1.74(13) s
|  (>99.9%)
| 95Pd
| rowspan=2|(9/2+)
| rowspan=2|
| rowspan=2|
|-
| , p (<.1%)
| 94Rh
|-
| style="text-indent:1em" | 95m1Ag
| colspan="3" style="text-indent:2em" | 344.2(3) keV
| <0.5 s
|
|
| (1/2-)
|
|
|-
| style="text-indent:1em" | 95m2Ag
| colspan="3" style="text-indent:2em" | 2531(1) keV
| <16 ms
|
|
| (23/2+)
|
|
|-
| style="text-indent:1em" | 95m3Ag
| colspan="3" style="text-indent:2em" | 4859(1) keV
| <40 ms
|
|
| (37/2+)
|
|
|-
| rowspan=2|96Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 49
| rowspan=2|95.93068(43)#
| rowspan=2|4.45(4) s
|  (96.3%)
| 96Pd
| rowspan=2|(8+)
| rowspan=2|
| rowspan=2|
|-
| , p (3.7%)
| 95Rh
|-
| style="text-indent:1em" | 96m1Ag
| colspan="3" style="text-indent:2em" | 0(50)# keV
| 6.9(6) s
|
|
| (2+)
|
|
|-
| style="text-indent:1em" | 96m2Ag
| colspan="3" style="text-indent:2em" |
| 700(200) ns
|
|
|
|
|
|-
| 97Ag
| style="text-align:right" | 47
| style="text-align:right" | 50
| 96.92397(35)
| 25.3(3) s
| 
| 97Pd
| (9/2+)
|
|
|-
| style="text-indent:1em" | 97mAg
| colspan="3" style="text-indent:2em" | 2343(49) keV
| 5 ns
|
|
| (21/2+)
|
|
|-
| rowspan=2|98Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 51
| rowspan=2|97.92157(7)
| rowspan=2|47.5(3) s
|  (99.99%)
| 98Pd
| rowspan=2|(5+)
| rowspan=2|
| rowspan=2|
|-
| , p (.0012%)
| 97Rh
|-
| style="text-indent:1em" | 98mAg
| colspan="3" style="text-indent:2em" | 167.83(15) keV
| 220(20) ns
|
|
| (3+)
|
|
|-
| 99Ag
| style="text-align:right" | 47
| style="text-align:right" | 52
| 98.91760(16)
| 124(3) s
| 
| 99Pd
| (9/2)+
|
|
|-
| style="text-indent:1em" | 99mAg
| colspan="3" style="text-indent:2em" | 506.1(4) keV
| 10.5(5) s
| IT
| 99Ag
| (1/2-)
|
|
|-
| 100Ag
| style="text-align:right" | 47
| style="text-align:right" | 53
| 99.91610(8)
| 2.01(9) min
| 
| 100Pd
| (5)+
| 
| 
|-
| rowspan=2 style="text-indent:1em" | 100mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 15.52(16) keV
| rowspan=2|2.24(13) min
| IT
| 100Ag
| rowspan=2|(2)+
| rowspan=2|
| rowspan=2|
|-
| 
| 100Pd
|-
| 101Ag
| style="text-align:right" | 47
| style="text-align:right" | 54
| 100.91280(11)
| 11.1(3) min
| 
| 101Pd
| 9/2+
|
|
|-
| style="text-indent:1em" | 101mAg
| colspan="3" style="text-indent:2em" | 274.1(3) keV
| 3.10(10) s
| IT
| 101Ag
| 1/2-
|
|
|-
| 102Ag
| style="text-align:right" | 47
| style="text-align:right" | 55
| 101.91169(3)
| 12.9(3) min
| 
| 102Pd
| 5+
|
|
|-
| rowspan=2 style="text-indent:1em" | 102mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 9.3(4) keV
| rowspan=2|7.7(5) min
|  (51%)
| 102Pd
| rowspan=2|2+
| rowspan=2|
| rowspan=2|
|-
| IT (49%)
| 102Ag
|-
| 103Ag
| style="text-align:right" | 47
| style="text-align:right" | 56
| 102.908973(18)
| 65.7(7) min
| 
| 103Pd
| 7/2+
|
|
|-
| style="text-indent:1em" | 103mAg
| colspan="3" style="text-indent:2em" | 134.45(4) keV
| 5.7(3) s
| IT
| 103Ag
| 1/2-
|
|
|-
| 104Ag
| style="text-align:right" | 47
| style="text-align:right" | 57
| 103.908629(6)
| 69.2(10) min
| 
| 104Pd
| 5+
|
|
|-
| rowspan=2 style="text-indent:1em" | 104mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 6.9(4) keV
| rowspan=2|33.5(20) min
|  (99.93%)
| 104Pd
| rowspan=2|2+
| rowspan=2|
| rowspan=2|
|-
| IT (.07%)
| 104Ag
|-
| 105Ag
| style="text-align:right" | 47
| style="text-align:right" | 58
| 104.906529(12)
| 41.29(7) d
| 
| 105Pd
| 1/2-
|
|
|-
| rowspan=2 style="text-indent:1em" | 105mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 25.465(12) keV
| rowspan=2|7.23(16) min
| IT (99.66%)
| 105Ag
| rowspan=2|7/2+
| rowspan=2|
| rowspan=2|
|-
|  (.34%)
| 105Pd
|-
| rowspan=2|106Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 59
| rowspan=2|105.906669(5)
| rowspan=2|23.96(4) min
|  (99.5%)
| 106Pd
| rowspan=2|1+
| rowspan=2|
| rowspan=2|
|-
|  (0.5%)
| 106Cd
|-
| rowspan=2 style="text-indent:1em" | 106mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 89.66(7) keV
| rowspan=2|8.28(2) d
| 
| 106Pd
| rowspan=2|6+
| rowspan=2|
| rowspan=2|
|-
| IT (4.16×10−6%)
| 106Ag
|-
| Used to date certain events in the early history of the Solar System
| style="text-align:right" | 47
| style="text-align:right" | 60
| 106.905097(5)
| colspan=3 align=center|
| 1/2-
| 0.51839(8)
|
|-
| style="text-indent:1em" | 107mAg
| colspan="3" style="text-indent:2em" | 93.125(19) keV
| 44.3(2) s
| IT
| 107Ag
| 7/2+
|
|
|-
| rowspan=2|108Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 61
| rowspan=2|107.905956(5)
| rowspan=2|2.37(1) min
|  (97.15%)
| 108Cd
| rowspan=2|1+
| rowspan=2|
| rowspan=2|
|-
|  (2.85%)
| 108Pd
|-
| rowspan=2 style="text-indent:1em" | 108mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 109.440(7) keV
| rowspan=2|418(21) y
|  (91.3%)
| 108Pd
| rowspan=2|6+
| rowspan=2|
| rowspan=2|
|-
| IT (8.96%)
| 108Ag
|-
| 109AgFission product
| style="text-align:right" | 47
| style="text-align:right" | 62
| 108.904752(3)
| colspan=3 align=center|
| 1/2-
| 0.48161(8)
|
|-
| style="text-indent:1em" | 109mAg
| colspan="3" style="text-indent:2em" | 88.0341(11) keV
| 39.6(2) s
| IT
| 109Ag
| 7/2+
|
|
|-
| rowspan=2|110Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 63
| rowspan=2|109.906107(3)
| rowspan=2|24.6(2) s
|  (99.7%)
| 110Cd
| rowspan=2|1+
| rowspan=2|
| rowspan=2|
|-
| (.3%)
| 110Pd
|-
| style="text-indent:1em" | 110m1Ag
| colspan="3" style="text-indent:2em" | 1.113 keV
| 660(40) ns
|
|
| 2-
| 
| 
|-
| rowspan=2 style="text-indent:1em" | 110m2Ag
| rowspan=2 colspan="3" style="text-indent:2em" | 117.59(5) keV
| rowspan=2|249.950(24) d
|  (98.64%)
| 110Cd
| rowspan=2|6+
| rowspan=2|
| rowspan=2|
|-
| IT (1.36%)
| 110Ag
|-
| 111Ag
| style="text-align:right" | 47
| style="text-align:right" | 64
| 110.905291(3)
| 7.45(1) d
| 
| 111Cd
| 1/2-
|
|
|-
| rowspan=2 style="text-indent:1em" | 111mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 59.82(4) keV
| rowspan=2|64.8(8) s
| IT (99.3%)
| 111Ag
| rowspan=2|7/2+
| rowspan=2|
| rowspan=2|
|-
|  (.7%)
| 111Cd
|-
| 112Ag
| style="text-align:right" | 47
| style="text-align:right" | 65
| 111.907005(18)
| 3.130(9) h
| 
| 112Cd
| 2(-)
|
|
|-
| 113Ag
| style="text-align:right" | 47
| style="text-align:right" | 66
| 112.906567(18)
| 5.37(5) h
| 
| 113mCd
| 1/2-
|
|
|-
| rowspan=2 style="text-indent:1em" | 113mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 43.50(10) keV
| rowspan=2|68.7(16) s
| IT (64%)
| 113Ag
| rowspan=2|7/2+
| rowspan=2|
| rowspan=2|
|-
|  (36%)
| 113Cd
|-
| 114Ag
| style="text-align:right" | 47
| style="text-align:right" | 67
| 113.908804(27)
| 4.6(1) s
| 
| 114Cd
| 1+
|
|
|-
| style="text-indent:1em" | 114mAg
| colspan="3" style="text-indent:2em" | 199(5) keV
| 1.50(5) ms
| IT
| 114Ag
| (<7+)
|
|
|-
| 115Ag
| style="text-align:right" | 47
| style="text-align:right" | 68
| 114.90876(4)
| 20.0(5) min
| 
| 115mCd
| 1/2-
|
|
|-
| rowspan=2 style="text-indent:1em" | 115mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 41.16(10) keV
| rowspan=2|18.0(7) s
|  (79%)
| 115Cd
| rowspan=2|7/2+
| rowspan=2|
| rowspan=2|
|-
| IT (21%)
| 115Ag
|-
| 116Ag
| style="text-align:right" | 47
| style="text-align:right" | 69
| 115.91136(5)
| 2.68(10) min
| 
| 116Cd
| (2)-
|
|
|-
| rowspan=2 style="text-indent:1em" | 116mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 81.90(20) keV
| rowspan=2|8.6(3) s
|  (94%)
| 116Cd
| rowspan=2|(5+)
| rowspan=2|
| rowspan=2|
|-
| IT (6%)
| 116Ag
|-
| 117Ag
| style="text-align:right" | 47
| style="text-align:right" | 70
| 116.91168(5)
| 73.6(14) s[72.8(+20-7) s]
| 
| 117mCd
| 1/2-#
|
|
|-
| rowspan=2 style="text-indent:1em" | 117mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 28.6(2) keV
| rowspan=2|5.34(5) s
|  (94%)
| 117mCd
| rowspan=2|(7/2+)
| rowspan=2|
| rowspan=2|
|-
| IT (6%)
| 117Ag
|-
| 118Ag
| style="text-align:right" | 47
| style="text-align:right" | 71
| 117.91458(7)
| 3.76(15) s
| 
| 118Cd
| 1-
|
|
|-
| style="text-indent:1em" | 118m1Ag
| colspan="3" style="text-indent:2em" | 45.79(9) keV
| ~0.1 µs
|
|
| 0(-) to 2(-)
|
|
|-
| rowspan=2 style="text-indent:1em" | 118m2Ag
| rowspan=2 colspan="3" style="text-indent:2em" | 127.49(5) keV
| rowspan=2|2.0(2) s
|  (59%)
| 118Cd
| rowspan=2|4(+)
| rowspan=2|
| rowspan=2|
|-
| IT (41%)
| 118Ag
|-
| style="text-indent:1em" | 118m3Ag
| colspan="3" style="text-indent:2em" | 279.37(20) keV
| ~0.1 µs
|
|
| (2+,3+)
|
|
|-
| 119Ag
| style="text-align:right" | 47
| style="text-align:right" | 72
| 118.91567(10)
| 6.0(5) s
| 
| 119mCd
| 1/2-#
|
|
|-
| style="text-indent:1em" | 119mAg
| colspan="3" style="text-indent:2em" | 20(20)# keV
| 2.1(1) s
| 
| 119Cd
| 7/2+#
|
|
|-
| rowspan=2|120Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 73
| rowspan=2|119.91879(8)
| rowspan=2|1.23(4) s
|  (99.99%)
| 120Cd
| rowspan=2|3(+#)
| rowspan=2|
| rowspan=2|
|-
| , n (.003%)
| 119Cd
|-
| rowspan=2 style="text-indent:1em" | 120mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 203.0(10) keV
| rowspan=2|371(24) ms
|  (63%)
| 120Cd
| rowspan=2|6(-)
| rowspan=2|
| rowspan=2|
|-
| IT (37%)
| 120Ag
|-
| rowspan=2|121Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 74
| rowspan=2|120.91985(16)
| rowspan=2|0.79(2) s
|  (99.92%)
| 121Cd
| rowspan=2|(7/2+)#
| rowspan=2| 
| rowspan=2|
|-
| , n (.076%)
| 120Cd
|-
| rowspan=2|122Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 75
| rowspan=2|121.92353(22)#
| rowspan=2|0.529(13) s
|  (>99.9%)
| 122Cd
| rowspan=2|(3+)
| rowspan=2|
| rowspan=2|
|-
| , n (<.1%)
| 121Cd
|-
| rowspan=2 style="text-indent:1em" | 122mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 80(50)# keV
| rowspan=2|1.5(5) s
|  (>99.9%)
| 122Cd
| rowspan=2|8-#
| rowspan=2|
| rowspan=2|
|-
| , n (<.1%)
| 121Cd
|-
| rowspan=2|123Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 76
| rowspan=2|122.92490(22)#
| rowspan=2|0.300(5) s
|  (99.45%)
| 123Cd
| rowspan=2|(7/2+)
| rowspan=2|
| rowspan=2|
|-
| , n (.549%)
| 122Cd
|-
| rowspan=2|124Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 77
| rowspan=2|123.92864(21)#
| rowspan=2|172(5) ms
|  (99.9%)
| 124Cd
| rowspan=2|3+#
| rowspan=2| 
| rowspan=2|
|-
| , n (.1%)
| 123Cd
|-
| rowspan=2 style="text-indent:1em" | 124mAg
| rowspan=2 colspan="3" style="text-indent:2em" | 0(100)# keV
| rowspan=2|200# ms
| 
| 124Cd
| rowspan=2|8-#
| rowspan=2|
| rowspan=2|
|-
| IT
| 124Ag
|-
| rowspan=2|125Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 78
| rowspan=2|124.93043(32)#
| rowspan=2|166(7) ms
|  (>99.9%)
| 125Cd
| rowspan=2|(7/2+)#
| rowspan=2|
| rowspan=2|
|-
| , n (<.1%)
| 124Cd
|-
| rowspan=2|126Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 79
| rowspan=2|125.93450(32)#
| rowspan=2|107(12) ms
|  (>99.9%)
| 126Cd
| rowspan=2|3+#
| rowspan=2|
| rowspan=2|
|-
| , n (<.1%)
| 125Cd
|-
| rowspan=2|127Ag
| rowspan=2 style="text-align:right" | 47
| rowspan=2 style="text-align:right" | 80
| rowspan=2|126.93677(32)#
| rowspan=2|79(3) ms
|  (>99.9%)
| 127Cd
| rowspan=2|7/2+#
| rowspan=2|
| rowspan=2|
|-
| , n (<.1%)
| 126Cd
|-
| 128Ag
| style="text-align:right" | 47
| style="text-align:right" | 81
| 127.94117(32)#
| 58(5) ms
|
|
|
|
|
|-
| 129Ag
| style="text-align:right" | 47
| style="text-align:right" | 82
| 128.94369(43)#
| 44(7) ms[46(+5-9) ms]
|
|
| 7/2+#
|
|
|-
| style="text-indent:1em" | 129mAg
| colspan="3" style="text-indent:2em" | 0(200)# keV
| ~160 ms
|
|
| 1/2-#
|
|
|-
| 130Ag
| style="text-align:right" | 47
| style="text-align:right" | 83
| 129.95045(36)#
| ~50 ms
|
|
| 0+
|
|
|}

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.

Ag
Category:银
*