Naturally occurring silver (47Ag) is composed of the two stable isotopes 107Ag and 109Ag in almost equal proportions, with 107Ag being slightly more abundant (51.839% natural abundance). Notably, silver is the only element with multiple NMR-active isotopes all having spin 1/2. Thus both 107Ag and 109Ag nuclei produce narrow lines in nuclear magnetic resonance spectra.[1]

40 radioisotopes have been characterized with the most stable being 105Ag with a half-life of 41.29 days, 111Ag with a half-life of 7.43 days, and 112Ag with a half-life of 3.13 hours.

All of the remaining radioactive isotopes have half-lives that are less than an hour, and the majority of these have half-lives that are less than 3 minutes. This element has numerous meta states, with the most stable being 108mAg (half-life 439 years), 110mAg (half-life 249.86 days) and 106mAg (half-life 8.28 days).

Known isotopes of silver range in atomic weight from 92Ag to 132Ag. The primary decay mode before the most abundant stable isotope, 107Ag, is electron capture and the primary mode after is beta decay. The primary decay products before 107Ag are palladium (element 46) isotopes and the primary products after are cadmium (element 48) isotopes.

The palladium isotope 107Pd decays by beta emission to 107Ag with a half-life of 6.5 million years. Iron meteorites are the only objects with a high enough palladium/silver ratio to yield measurable variations in 107Ag abundance. Radiogenic 107Ag was first discovered in the Santa Clara meteorite in 1978.

The discoverers[who?] suggest that the coalescence and differentiation of iron-cored small planets may have occurred 10 million years after a nucleosynthetic event. 107Pd versus 107Ag correlations observed in bodies, which have clearly been melted since the accretion of the Solar System, must reflect the presence of live short-lived nuclides in the early Solar System.

List of isotopes

|-id=Silver-92 | rowspan=2 | 92Ag | rowspan=2 | 47 | rowspan=2 | 45 | rowspan=2 | 91.95971(43)# | rowspan=2 style="text-align:center" | 2016 | rowspan=2|1# ms
[>400 ns] | β+? | 92Pd | rowspan=2| | rowspan=2| | rowspan=2| |- | p? | 91Pd |-id=Silver-93 | rowspan=3 | 93Ag | rowspan=3 | 47 | rowspan=3 | 46 | rowspan=3 | 92.95019(43)# | rowspan=3 style="text-align:center" | 1995 | rowspan=3| 228(16) ns | β+? | 93Pd | rowspan=3|9/2+# | rowspan=3| | rowspan=3| |- | p? | 92Pd |- | β+, p? | 92Rh |-id=Silver-94 | rowspan=2| 94Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 47 | rowspan=2| 93.94374(43)# | rowspan=2 style="text-align:center" | 1994 | rowspan=2| 27(2) ms | β+ (>99.8%) | 94Pd | rowspan=2| 0+# | rowspan=2| | rowspan=2| |- | β+, p (<0.2%) | 93Rh |-id=Silver-94m1 | rowspan=2 style="text-indent:1em" | 94m1Ag | rowspan=2 colspan="3" style="text-indent:2em" | 1350(400)# keV | rowspan=2 style="text-align:center" | 2002 | rowspan=2|470(10) ms | β+ (83%) | 94Pd | rowspan=2|(7+) | rowspan=2| | rowspan=2| |- | β+, p (17%) | 93Rh |-id=Silver-94m2 | rowspan=4 style="text-indent:1em" | 94m2Ag | rowspan=4 colspan="3" style="text-indent:2em" | 6500(550)# keV | rowspan=4 style="text-align:center" | 2002 | rowspan=4| 400(40) ms | β+ (~68.4%) | 94Pd | rowspan=4| (21+) | rowspan=4| | rowspan=4| |- | β+, p (~27%) | 93Rh |- | p (4.1%) | 93Pd |- | 2p (0.5%) | 92Rh |-id=Silver-95 | rowspan=2|95Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 48 | rowspan=2|94.93569(43)# | rowspan=2 style="text-align:center" | 1994 | rowspan=2|1.78(6) s | β+ (97.7%) | 95Pd | rowspan=2|(9/2+) | rowspan=2| | rowspan=2| |- | β+, p (2.3%) | 94Rh |-id=Silver-95m1 | style="text-indent:1em" | 95m1Ag | colspan="3" style="text-indent:2em" | 344.2(3) keV | style="text-align:center" | 2003 | <0.5 s | IT | 95Ag | (1/2−) | | |-id=Silver-95m2 | style="text-indent:1em" | 95m2Ag | colspan="3" style="text-indent:2em" | 2531.3(15) keV | style="text-align:center" | 2003 | <16 ms | IT | 95Ag | (23/2+) | | |-id=Silver-95m3 | style="text-indent:1em" | 95m3Ag | colspan="3" style="text-indent:2em" | 4860.0(15) keV | style="text-align:center" | 2003 | <40 ms | IT | 95Ag | (37/2+) | | |-id=Silver-96 | rowspan=2|96Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 49 | rowspan=2|95.93074(10) | rowspan=2 style="text-align:center" | 1982 | rowspan=2|4.45(3) s | β+ (95.8%) | 96Pd | rowspan=2|(8)+ | rowspan=2| | rowspan=2| |- | β+, p (4.2%) | 95Rh |-id=Silver-96m1 | rowspan=2 style="text-indent:1em" | 96m1Ag[n 1] | rowspan=2 colspan="3" style="text-indent:2em" | 0(50)# keV | rowspan=2 style="text-align:center" | 2003 | rowspan=2| 6.9(5) s | β+ (85.1%) | 96Pd | rowspan=2| (2+) | rowspan=2| | rowspan=2| |- | β+, p (14.9%) | 95Rh |-id=Silver-96m2 | style="text-indent:1em" | 96m2Ag | colspan="3" style="text-indent:2em" | 2461.4(3) keV | style="text-align:center" | 2011 | 103.2(45) μs | IT | 96Ag | (13−) | | |-id=Silver-96m3 | style="text-indent:1em" | 96m3Ag | colspan="3" style="text-indent:2em" | 2686.7(4) keV | style="text-align:center" | 2011 | 1.561(16) μs | IT | 96Ag | (15+) | | |-id=Silver-96m4 | style="text-indent:1em" | 96m4Ag | colspan="3" style="text-indent:2em" | 6951.8(14) keV | style="text-align:center" | 2011 | 132(17) ns | IT | 96Ag | (19+) | | |-id=Silver-97 | 97Ag | style="text-align:right" | 47 | style="text-align:right" | 50 | 96.923881(13) | style="text-align:center" | 1978 | 25.5(3) s | β+ | 97Pd | (9/2)+ | | |-id=Silver-97m | style="text-indent:1em" | 97mAg | colspan="3" style="text-indent:2em" | 620(40) keV | style="text-align:center" | 2020 | 100# ms | IT? | 97Ag | 1/2−# | | |-id=Silver-98 | rowspan=2|98Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 51 | rowspan=2|97.92156(4) | rowspan=2 style="text-align:center" | 1978 | rowspan=2|47.5(3) s | β+ | 98Pd | rowspan=2|(6)+ | rowspan=2| | rowspan=2| |- | β+, p (.0012%) | 97Rh |-id=Silver-98m | style="text-indent:1em" | 98mAg | colspan="3" style="text-indent:2em" | 107.28(10) keV | style="text-align:center" | 2017 | 161(7) ns | IT | 98Ag | (4+) | | |-id=Silver-99 | 99Ag | style="text-align:right" | 47 | style="text-align:right" | 52 | 98.917646(7) | style="text-align:center" | 1967 | 2.07(5) min | β+ | 99Pd | (9/2)+ | | |-id=Silver-99m | style="text-indent:1em" | 99mAg | colspan="3" style="text-indent:2em" | 506.2(4) keV | style="text-align:center" | 1978 | 10.5(5) s | IT | 99Ag | (1/2−) | | |-id=Silver-100 | 100Ag | style="text-align:right" | 47 | style="text-align:right" | 53 | 99.916115(5) | style="text-align:center" | 1970 | 2.01(9) min | β+ | 100Pd | (5)+ | | |-id=Silver-100m | rowspan=2 style="text-indent:1em" | 100mAg | rowspan=2 colspan="3" style="text-indent:2em" | 15.52(16) keV | rowspan=2 style="text-align:center" | 1980 | rowspan=2|2.24(13) min | IT? | 100Ag | rowspan=2|(2)+ | rowspan=2| | rowspan=2| |- | β+? | 100Pd |-id=Silver-101 | 101Ag | style="text-align:right" | 47 | style="text-align:right" | 54 | 100.912684(5) | style="text-align:center" | 1966 | 11.1(3) min | β+ | 101Pd | 9/2+ | | |-id=Silver-101m | style="text-indent:1em" | 101mAg | colspan="3" style="text-indent:2em" | 274.1(3) keV | style="text-align:center" | 1975 | 3.10(10) s | IT | 101Ag | (1/2)− | | |-id=Silver-102 | 102Ag | style="text-align:right" | 47 | style="text-align:right" | 55 | 101.911705(9) | style="text-align:center" | 1960 | 12.9(3) min | β+ | 102Pd | 5+ | | |-id=Silver-102m | rowspan=2 style="text-indent:1em" | 102mAg | rowspan=2 colspan="3" style="text-indent:2em" | 9.40(7) keV | rowspan=2 style="text-align:center" | 1967 | rowspan=2|7.7(5) min | β+ (51%) | 102Pd | rowspan=2|2+ | rowspan=2| | rowspan=2| |- | IT (49%) | 102Ag |-id=Silver-103 | 103Ag | style="text-align:right" | 47 | style="text-align:right" | 56 | 102.908961(4) | style="text-align:center" | 1954 | 65.7(7) min | β+ | 103Pd | 7/2+ | | |-id=Silver-103m | style="text-indent:1em" | 103mAg | colspan="3" style="text-indent:2em" | 134.45(4) keV | style="text-align:center" | 1962 | 5.7(3) s | IT | 103Ag | 1/2− | | |-id=Silver-104 | 104Ag | style="text-align:right" | 47 | style="text-align:right" | 57 | 103.908624(5) | style="text-align:center" | 1955 | 69.2(10) min | β+ | 104Pd | 5+ | | |-id=Silver-104m | rowspan=2 style="text-indent:1em" | 104mAg | rowspan=2 colspan="3" style="text-indent:2em" | 6.90(22) keV | rowspan=2 style="text-align:center" | 1959 | rowspan=2|33.5(20) min | β+ (>99.93%) | 104Pd | rowspan=2|2+ | rowspan=2| | rowspan=2| |- | IT (<0.07%) | 104Ag |-id=Silver-105 | 105Ag | style="text-align:right" | 47 | style="text-align:right" | 58 | 104.906526(5) | style="text-align:center" | 1939 | 41.29(7) d | β+ | 105Pd | 1/2− | | |-id=Silver-105m | rowspan=2 style="text-indent:1em" | 105mAg | rowspan=2 colspan="3" style="text-indent:2em" | 25.468(16) keV | rowspan=2 style="text-align:center" | 1969 | rowspan=2|7.23(16) min | IT (99.66%) | 105Ag | rowspan=2|7/2+ | rowspan=2| | rowspan=2| |- | β+ (.34%) | 105Pd |-id=Silver-106 | rowspan=2|106Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 59 | rowspan=2|105.906663(3) | rowspan=2 style="text-align:center" | 1937 | rowspan=2|23.96(4) min | β+ | 106Pd | rowspan=2|1+ | rowspan=2| | rowspan=2| |- | β−? | 106Cd |-id=Silver-106m | rowspan=2 style="text-indent:1em" | 106mAg | rowspan=2 colspan="3" style="text-indent:2em" | 89.66(7) keV | rowspan=2 style="text-align:center" | 1938 | rowspan=2|8.28(2) d | β+ | 106Pd | rowspan=2|6+ | rowspan=2| | rowspan=2| |- | IT? | 106Ag |-id=Silver-107 | 107Ag[n 2] | style="text-align:right" | 47 | style="text-align:right" | 60 | 106.9050915(26) | style="text-align:center" | 1923 | colspan=3 align=center|Stable | 1/2− | 0.51839(8) | |-id=Silver-107m | style="text-indent:1em" | 107mAg | colspan="3" style="text-indent:2em" | 93.125(19) keV | style="text-align:center" | 1946 | 44.3(2) s | IT | 107Ag | 7/2+ | | |-id=Silver-108 | rowspan=3|108Ag[2] | rowspan=3 style="text-align:right" | 47 | rowspan=3 style="text-align:right" | 61 | rowspan=3|107.9059502(26) | rowspan=3 style="text-align:center" | 1937 | rowspan=3|2.382(11) min | β− (97.15%) | 108Cd | rowspan=3|1+ | rowspan=3| | rowspan=3| |- | EC (2.57%) | rowspan=2|108Pd |- | β+ (0.283%) |-id=Silver-108m | rowspan=2 style="text-indent:1em" | 108mAg[2] | rowspan=2 colspan="3" style="text-indent:2em" | 109.466(7) keV | rowspan=2 style="text-align:center" | 1960 | rowspan=2|439(9) y | EC (91.3%) | 108Pd | rowspan=2|6+ | rowspan=2| | rowspan=2| |- | IT (8.7%) | 108Ag |-id=Silver-109 | 109Ag[n 3] | style="text-align:right" | 47 | style="text-align:right" | 62 | 108.9047558(14) | style="text-align:center" | 1923 | colspan=3 align=center|Stable | 1/2− | 0.48161(8) | |-id=Silver-109m | style="text-indent:1em" | 109mAg[n 3] | colspan="3" style="text-indent:2em" | 88.0337(10) keV | style="text-align:center" | 1946 | 39.79(21) s | IT | 109Ag | 7/2+ | | |-id=Silver-110 | rowspan=2|110Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 63 | rowspan=2|109.9061107(14) | rowspan=2 style="text-align:center" | 1937 | rowspan=2|24.56(11) s | β− (99.70%) | 110Cd | rowspan=2|1+ | rowspan=2| | rowspan=2| |- | EC (0.30%) | 110Pd |-id=Silver-110m1 | style="text-indent:1em" | 110m1Ag | colspan="3" style="text-indent:2em" | 1.112(16) keV | style="text-align:center" | 1975 | 660(40) ns | IT | 110Ag | 2− | | |-id=Silver-110m2 | rowspan=2 style="text-indent:1em" | 110m2Ag | rowspan=2 colspan="3" style="text-indent:2em" | 117.59(5) keV | rowspan=2 style="text-align:center" | 1950 | rowspan=2|249.863(24) d | β− (98.67%) | 110Cd | rowspan=2|6+ | rowspan=2| | rowspan=2| |- | IT (1.33%) | 110Ag |-id=Silver-111 | 111Ag[n 3] | style="text-align:right" | 47 | style="text-align:right" | 64 | 110.9052968(16) | style="text-align:center" | 1937 | 7.433(10) d | β− | 111Cd | 1/2− | | |-id=Silver-111m | rowspan=2 style="text-indent:1em" | 111mAg | rowspan=2 colspan="3" style="text-indent:2em" | 59.82(4) keV | rowspan=2 style="text-align:center" | 1957 | rowspan=2|64.8(8) s | IT (99.3%) | 111Ag | rowspan=2|7/2+ | rowspan=2| | rowspan=2| |- | β− (0.7%) | 111Cd |-id=Silver-112 | 112Ag | style="text-align:right" | 47 | style="text-align:right" | 65 | 111.9070485(26) | style="text-align:center" | 1938 | 3.130(8) h | β− | 112Cd | 2(−) | | |-id=Silver-113 | 113Ag | style="text-align:right" | 47 | style="text-align:right" | 66 | 112.906573(18) | style="text-align:center" | 1949 | 5.37(5) h | β− | 113mCd | 1/2− | | |-id=Silver-113m | rowspan=2 style="text-indent:1em" | 113mAg | rowspan=2 colspan="3" style="text-indent:2em" | 43.50(10) keV | rowspan=2 style="text-align:center" | 1958 | rowspan=2|68.7(16) s | IT (64%) | 113Ag | rowspan=2|7/2+ | rowspan=2| | rowspan=2| |- | β− (36%) | 113Cd |-id=Silver-114 | 114Ag | style="text-align:right" | 47 | style="text-align:right" | 67 | 113.908823(5) | style="text-align:center" | 1958 | 4.6(1) s | β− | 114Cd | 1+ | | |-id=Silver-114m | style="text-indent:1em" | 114mAg | colspan="3" style="text-indent:2em" | 198.9(10) keV | style="text-align:center" | (1990)[n 4] | 1.50(5) ms | IT | 114Ag | (6+) | | |-id=Silver-115 | 115Ag | style="text-align:right" | 47 | style="text-align:right" | 68 | 114.908767(20) | style="text-align:center" | 1949 | 20.0(5) min | β− | 115mCd | 1/2− | | |-id=Silver-115m | rowspan=2 style="text-indent:1em" | 115mAg | rowspan=2 colspan="3" style="text-indent:2em" | 41.16(10) keV | rowspan=2 style="text-align:center" | 1958 | rowspan=2|18.0(7) s | β− (79.0%) | 115Cd | rowspan=2|7/2+ | rowspan=2| | rowspan=2| |- | IT (21.0%) | 115Ag |-id=Silver-116 | 116Ag | style="text-align:right" | 47 | style="text-align:right" | 69 | 115.911387(4) | style="text-align:center" | 1958 | 3.83(8) min | β− | 116Cd | (0−) | | |-id=Silver-116m1 | rowspan=2 style="text-indent:1em" | 116m1Ag | rowspan=2 colspan="3" style="text-indent:2em" | 47.90(10) keV | rowspan=2 style="text-align:center" | 2005 | rowspan=2|20(1) s | β− (93%) | 116Cd | rowspan=2|(3+) | rowspan=2| | rowspan=2| |- | IT (7%) | 116Ag |-id=Silver-116m2 | rowspan=2 style="text-indent:1em" | 116m2Ag | rowspan=2 colspan="3" style="text-indent:2em" | 129.80(22) keV | rowspan=2 style="text-align:center" | 1971 | rowspan=2|9.3(3) s | β− (92%) | 116Cd | rowspan=2|(6−) | rowspan=2| | rowspan=2| |- | IT (8%) | 116Ag |-id=Silver-117 | 117Ag | style="text-align:right" | 47 | style="text-align:right" | 70 | 116.911774(15) | style="text-align:center" | 1958 | 73.6(14) s | β− | 117mCd | 1/2−# | | |-id=Silver-117m | rowspan=2 style="text-indent:1em" | 117mAg | rowspan=2 colspan="3" style="text-indent:2em" | 28.6(2) keV | rowspan=2 style="text-align:center" | 1990 | rowspan=2|5.34(5) s | β− (94.0%) | 117mCd | rowspan=2|7/2+# | rowspan=2| | rowspan=2| |- | IT (6.0%) | 117Ag |-id=Silver-118 | 118Ag | style="text-align:right" | 47 | style="text-align:right" | 71 | 117.9145955(27) | style="text-align:center" | 1968 | 3.76(15) s | β− | 118Cd | (2−) | | |-id=Silver-118m1 | style="text-indent:1em" | 118m1Ag | colspan="3" style="text-indent:2em" | 45.79(9) keV | style="text-align:center" | 1989 | ~0.1 μs[n 5] | IT | 118Ag | (1,2)− | |-id=Silver-118m2 | style="text-indent:1em" | 118m2Ag | colspan="3" style="text-indent:2em" | 123.5(12) keV | style="text-align:center" | 2025 | 1.92(7) s | β− | 118Cd | (7-) | |-id=Silver-118m3 | rowspan=2 style="text-indent:1em" | 118m3Ag | rowspan=2 colspan="3" style="text-indent:2em" | 127.63(10) keV | rowspan=2 style="text-align:center" | 1971 | rowspan=2|2.0(2) s | β− (59%) | 118Cd | rowspan=2|(5+) | rowspan=2| | rowspan=2| |- | IT (41%) | 118Ag |-id=Silver-118m4 | style="text-indent:1em" | 118m4Ag | colspan="3" style="text-indent:2em" | 279.37(20) keV | style="text-align:center" | 1993 | ~0.1 μs[n 5] | IT | 118Ag | (3+) | | |-id=Silver-119 | 119Ag | style="text-align:right" | 47 | style="text-align:right" | 72 | 118.915570(16) | style="text-align:center" | 1975 | 2.1(1) s | β− | 119Cd | (7/2+) | | |-id=Silver-119m | style="text-indent:1em" | 119mAg | colspan="3" style="text-indent:2em" |33.5(3) keV[3] | style="text-align:center" | 1991 | 6.0(5) s | β− | 119Cd | (1/2−) | | |-id=Silver-120 | rowspan=2|120Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 73 | rowspan=2|119.918785(5) | rowspan=2 style="text-align:center" | 1971 | rowspan=2|1.52(7) s | β− | 120Cd | rowspan=2|4(+) | rowspan=2| | rowspan=2| |- | β−, n (<.003%) | 119Cd |-id=Silver-120m1 | rowspan=3 style="text-indent:1em" | 120m1Ag[n 1] | rowspan=3 colspan="3" style="text-indent:2em" | 0(50)# keV | rowspan=3 style="text-align:center" | 2012 | rowspan=3|940(100) ms | β−? | 120Cd | rowspan=3|(0−, 1−) | rowspan=3| | rowspan=3| |- | IT? | 120Ag |- | β−, n? | 119Cd |-id=Silver-120m2 | rowspan=3 style="text-indent:1em" | 120m2Ag | rowspan=3 colspan="3" style="text-indent:2em" | 203.2(2) keV | rowspan=3 style="text-align:center" | 1971 | rowspan=3|384(22) ms | IT (68%) | 120Sn | rowspan=3|7(−) | rowspan=3| | rowspan=3| |- | β− (32%) | 120Cd |- | β−, n? | 119Cd |-id=Silver-121 | rowspan=2|121Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 74 | rowspan=2|120.920125(13) | rowspan=2 style="text-align:center" | 1982 | rowspan=2|777(10) ms | β− (99.92%) | 121Cd | rowspan=2|7/2+# | rowspan=2| | rowspan=2| |- | β−, n (0.080%) | 120Cd |-id=Silver-122 | rowspan=2|122Ag[4] | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 75 | rowspan=2|121.9235420(56) | rowspan=2 style="text-align:center" | 1978 | rowspan=2|550(50) ms | β− | 122Cd | rowspan=2|(1−) | rowspan=2| | rowspan=2| |- | β−, n? | 121Cd |-id=Silver-122m1 | rowspan=3 style="text-indent:1em" | 122m1Ag[4] | rowspan=3 colspan="3" style="text-indent:2em" | 303.7(50) keV | rowspan=3 style="text-align:center" | 2000 | rowspan=3|200(50) ms | β− | 122Cd | rowspan=3|(9−) | rowspan=3| | rowspan=3| |- | β−, n? | 121Cd |- | IT? | 122Ag |-id=Silver-122m2 | style="text-indent:1em" | 122m2Ag | colspan="3" style="text-indent:2em" | 171(50)# keV | style="text-align:center" | 2013 | 6.3(1) μs | IT | 122Ag | (1+) | | |-id=Silver-123 | rowspan=2|123Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 76 | rowspan=2|122.92532(4) | rowspan=2 style="text-align:center" | 1976 | rowspan=2|294(5) ms | β− (99.44%) | 123Cd | rowspan=2|(7/2+) | rowspan=2| | rowspan=2| |- | β−, n (0.56%) | 122Cd |-id=Silver-123m1 | rowspan=2 style="text-indent:1em" | 123m1Ag | rowspan=2 colspan="3" style="text-indent:2em" | 59.5(5) keV | rowspan=2 style="text-align:center" | 2019 | rowspan=2|100# ms | β− | 123Cd | rowspan=2|(1/2−) | rowspan=2| | rowspan=2| |- | β−, n? | 122Cd |-id=Silver-123m2 | style="text-indent:1em" | 123m2Ag | colspan="3" style="text-indent:2em" | 1450(14)# keV | style="text-align:center" | 2013 | 202(20) ns | IT | 123Ag | | | |-id=Silver-123m3 | style="text-indent:1em" | 123m3Ag | colspan="3" style="text-indent:2em" | 1472.8(8) keV | style="text-align:center" | 2009 | 393(16) ns | IT | 123Ag | (17/2−) | | |-id=Silver-124 | rowspan=2|124Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 77 | rowspan=2|123.9289318(74)[5] | rowspan=2 style="text-align:center" | 1984 | rowspan=2|177.9(26) ms | β− (98.7%) | 124Cd | rowspan=2|(2−) | rowspan=2| | rowspan=2| |- | β−, n (1.3%) | 123Cd |-id=Silver-124m1 | rowspan=2 style="text-indent:1em" | 124m1Ag | rowspan=2 colspan="3" style="text-indent:2em" | 188.2(25) keV[5] | rowspan=2 style="text-align:center" | 2014 | rowspan=2|144(20) ms | β− | 124Cd | rowspan=2|(8−)[5] | rowspan=2| | rowspan=2| |- | β−, n? | 123Cd |-id=Silver-124m2 | style="text-indent:1em" | 124m2Ag | colspan="3" style="text-indent:2em" | 155.6(5) keV | style="text-align:center" | 2013 | 140(50) ns | IT | 124Ag | (1+) | | |-id=Silver-124m3 | style="text-indent:1em" | 124m3Ag | colspan="3" style="text-indent:2em" | 231.1(7) keV | style="text-align:center" | 2012 | 1.48(15) μs | IT | 124Ag | (1−) | | |-id=Silver-125 | rowspan=2|125Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 78 | rowspan=2|124.9310029(43)[5] | rowspan=2 style="text-align:center" | 1994 | rowspan=2|160(5) ms | β− (88.2%) | 125Cd | rowspan=2|(9/2+) | rowspan=2| | rowspan=2| |- | β−, n (11.8%) | 124Cd |-id=Silver-125m1 | rowspan=3 style="text-indent:1em" | 125m1Ag | rowspan=3 colspan="3" style="text-indent:2em" | 97.1(5) keV | rowspan=3 style="text-align:center" | 2019 | rowspan=3|50# ms | β−? | 125Cd | rowspan=3|(1/2−) | rowspan=3| | rowspan=3| |- | IT? | 125Ag |- | β−, n? | 124Cd |-id=Silver-125m2 | style="text-indent:1em" | 125m2Ag | colspan="3" style="text-indent:2em" | 1501.2(6) keV | style="text-align:center" | 2009 | 491(20) ns | IT | 125Ag | (17/2−) | | |-id=Silver-126 | rowspan=2|126Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 79 | rowspan=2|125.93481(22)# | rowspan=2 style="text-align:center" | 1994 | rowspan=2|52(10) ms | β− (86.3%) | 126Cd | rowspan=2|3+# | rowspan=2| | rowspan=2|

|- | β−, n (13.7%) | 125Cd |-id=Silver-126m1 | rowspan=3 style="text-indent:1em" | 126m1Ag | rowspan=3 colspan="3" style="text-indent:2em" | 100(100)# keV | rowspan=3 style="text-align:center" | 1995 | rowspan=3|108.4(24) ms | β− | 126Cd | rowspan=3|9−# | rowspan=3| | rowspan=3| |- | IT? | 126Ag |- | β−, n? | 125Cd |-id=Silver-126m2 | style="text-indent:1em" | 126m2Ag | colspan="3" style="text-indent:2em" | 254.8(5) keV | style="text-align:center" | 2012 | 27(6) μs | IT | 126Ag | 1−# | | |-id=Silver-127 | rowspan=2|127Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 80 | rowspan=2|126.93704(22)# | rowspan=2 style="text-align:center" | 1995 | rowspan=2|89(2) ms | β− (85.4%) | 127Cd | rowspan=2|(9/2+) | rowspan=2| | rowspan=2| |- | β−, n (14.6%) | 126Cd |-id=Silver-127m | rowspan=2 style="text-indent:1em" | 127mAg | rowspan=2 colspan="3" style="text-indent:2em" | 1938(17) keV | rowspan=2 style="text-align:center" | 2021 | rowspan=2| 67.5(9) ms | β− (91.2%) | 127Cd | rowspan=2| (27/2+) | rowspan=2| | rowspan=2| |- | IT (8.8%) | 127Ag |-id=Silver-128 | rowspan=3| 128Ag | rowspan=3 style="text-align:right" | 47 | rowspan=3 style="text-align:right" | 81 | rowspan=3| 127.94127(32)# | rowspan=3 style="text-align:center" | 2000 | rowspan=3| 54(4) ms[6] | β− (80%) | 128Cd | rowspan=3| (9−)[6] | rowspan=3| | rowspan=3| |- | β−, n (20%) | 127Cd |- | β−, 2n? | 126Cd |-id=Silver-128m | style="text-indent:1em" | 128mAg[6] | colspan="3" style="text-indent:2em" | 2053.9+Z keV | style="text-align:center" | 2025 | 1.60(7) μs | IT | 128Ag | (16−) | | |-id=Silver-129 | rowspan=2| 129Ag | rowspan=2 style="text-align:right" | 47 | rowspan=2 style="text-align:right" | 82 | rowspan=2| 128.94432(43)# | rowspan=2 style="text-align:center" | 2000 | rowspan=2| 49.9(35) ms | β− (>80%) | 129Cd | rowspan=2| 9/2+# | rowspan=2| | rowspan=2| |- | β−, n (<20%) | 128Cd |-id=Silver-130 | rowspan=3|130Ag | rowspan=3 style="text-align:right" | 47 | rowspan=3 style="text-align:right" | 83 | rowspan=3|129.95073(46)# | rowspan=3 style="text-align:center" | 2000 | rowspan=3|40.6(45) ms | β− | 130Cd | rowspan=3|1−# | rowspan=3| | rowspan=3| |- | β−, n? | 129Cd |- | β−, 2n? | 128Cd |-id=Silver-131 | rowspan=3| 131Ag | rowspan=3 style="text-align:right" | 47 | rowspan=3 style="text-align:right" | 84 | rowspan=3| 130.95625(54)# | rowspan=3 style="text-align:center" | 2013 | rowspan=3| 35(8) ms | β− (90%) | 131Cd | rowspan=3| 9/2+# | rowspan=3| | rowspan=3| |- | β−, 2n (10%) | 129Cd |- | β−, n? | 130Cd |-id=Silver-132 | rowspan=3|132Ag | rowspan=3 style="text-align:right" | 47 | rowspan=3 style="text-align:right" | 85 | rowspan=3|131.96307(54)# | rowspan=3 style="text-align:center" | 2015 | rowspan=3|30(14) ms | β− | 132Cd | rowspan=3|6−# | rowspan=3| | rowspan=3| |- | β−, n? | 131Cd |- | β−, 2n? | 130Cd

See also

Daughter products other than silver

References

  1. ^ "(Ag) Silver NMR"
  2. ^ Blachot, Jean (October 2000). "Nuclear Data Sheets for A = 108". Nuclear Data Sheets. 91 (2): 135–296. Bibcode:2000NDS....91..135B. doi:10.1006/ndsh.2000.0017
  3. ^ Kurpeta, J.; Abramuk, A.; Rząca-Urban, T.; Urban, W.; Canete, L.; Eronen, T.; Geldhof, S.; Gierlik, M.; Greene, J. P.; Jokinen, A.; Kankainen, A.; Moore, I. D.; Nesterenko, D. A.; Penttilä, H.; Pohjalainen, I.; Reponen, M.; Rinta-Antila, S.; de Roubin, A.; Simpson, G. S.; Smith, A. G.; Vilén, M. (14 March 2022). "β - and γ -spectroscopy study of Pd 119 and Ag 119". Physical Review C. 105 (3). doi:10.1103/PhysRevC.105.034316
  4. ^ Jaries, A.; Stryjczyk, M.; Kankainen, A.; Ayoubi, L. Al; Beliuskina, O.; Canete, L.; de Groote, R. P.; Delafosse, C.; Delahaye, P.; Eronen, T.; Flayol, M.; Ge, Z.; Geldhof, S.; Gins, W.; Hukkanen, M.; Imgram, P.; Kahl, D.; Kostensalo, J.; Kujanpää, S.; Kumar, D.; Moore, I. D.; Mougeot, M.; Nesterenko, D. A.; Nikas, S.; Patel, D.; Penttilä, H.; Pitman-Weymouth, D.; Pohjalainen, I.; Raggio, A.; Ramalho, M.; Reponen, M.; Rinta-Antila, S.; de Roubin, A.; Ruotsalainen, J.; Srivastava, P. C.; Suhonen, J.; Vilen, M.; Virtanen, V.; Zadvornaya, A. (2024). "Isomeric states of fission fragments explored via Penning trap mass spectrometry at IGISOL". Physical Review C. 110 (3). arXiv:2403.04710. Bibcode:2024PhRvC.110c4326J. doi:10.1103/PhysRevC.110.034326
  5. ^ Ruotsalainen, J.; Nesterenko, D. A.; Stryjczyk, M.; Kankainen, A.; Al Ayoubi, L.; Beliuskina, O.; Canete, L.; Chauveau, P.; de Groote, R. P.; Delahaye, P.; Eronen, T.; Flayol, M.; Ge, Z.; Geldhof, S.; Gins, W.; Hukkanen, M.; Jaries, A.; Kahl, D.; Kumar, D.; Moore, I. D.; Nikas, S.; Penttilä, H.; Pitman-Weymouth, D.; Raggio, A.; Rinta-Antila, S.; de Roubin, A.; Vilen, M.; Virtanen, V. A.; Winter, M. (16 April 2025). "High-precision mass measurements of the ground and isomeric states in Ag 124, 125". Physical Review C. 111 (4). arXiv:2408.14181. doi:10.1103/PhysRevC.111.044314
  6. ^ Luo, D. W.; Zhang, J. Z.; Li, Z. H.; Cheng, Y. Y.; Hua, H.; Watanabe, H.; Lorusso, G.; Yuan, C. X.; Nishimura, S.; Baba, H.; Benzoni, G.; Browne, F.; Chae, K. Y.; Chen, Z. Q.; Crespi, F. C. L.; Doornenbal, P.; Fukuda, N.; Gernhäuser, R.; Gey, G.; Guo, C. Y.; Inabe, N.; Isobe, T.; Jiang, D. X.; Jin, Y.; Jung, H. S.; Jungclaus, A.; Kameda, D.; Kim, G. D.; Kim, Y. K.; Kojouharov, I.; Kondev, F. G.; Kubo, T.; Kurz, N.; Kwon, Y. K.; Lane, G. J.; Li, X. Q.; Lou, J. L.; Montaner-Pizá, A.; Moschner, K.; Naqvi, F. (12 June 2025). "Seniority Structure in Neutron-Rich Nucleus Ag 128 : Evidence for Robustness of N = 82 Shell Closure in Silver Isotopes". Physical Review Letters. 134 (23). Bibcode:2025PhRvL.134w2502L. doi:10.1103/wq9m-trj8. hdl:10261/397406. PMID 40577732
  • Isotope masses from:
  • Isotopic compositions and standard atomic masses from:
  • Half-life, spin, and isomer data selected from the following sources.
  1. ^ Order of ground state and isomer is uncertain.
  2. ^ Used to date certain events in the early history of the Solar System
  3. ^ Fission product
  4. ^ Only published in a conference proceeding and not a refereed journal.
  5. ^ Half-life only estimated