Isotopes of barium

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Template:Short description Template:Infobox barium isotopes Naturally occurring barium (56Ba) is a mix of six stable isotopes and one very long-lived radioactive primordial isotope, barium-130, identified as being unstable by geochemical means (from analysis of the presence of its daughter xenon-130 in rocks) in 2001.[1] This nuclide decays by double electron capture (absorbing two electrons and emitting two neutrinos), with a half-life of (0.5–2.7)×1021 years (about 1011 times the age of the universe).

There are a total of thirty-three known radioisotopes in addition to 130Ba. The longest-lived of these is 133Ba, which has a half-life of 10.51 years. All other radioisotopes have half-lives shorter than two weeks. The longest-lived isomer is 133mBa, which has a half-life of 38.9 hours. The shorter-lived 137mBa (half-life 2.55 minutes) arises as the decay product of the common fission product caesium-137.

Barium-114 is predicted to undergo cluster decay, emitting a nucleus of stable 12C to produce 102Sn. However this decay is not yet observed; the upper limit on the branching ratio of such decay is 0.0034%.

List of isotopes

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Template:Isotopes table |-id=Barium-114 | rowspan=4|114Ba | rowspan=4 style="text-align:right" | 56 | rowspan=4 style="text-align:right" | 58 | rowspan=4|113.95072(11) | rowspan=4|460(125) ms | β+ (79%) | 114Cs | rowspan=4|0+ | rowspan=4| | rowspan=4| |- | α (0.9%) | 110Xe |- | β+, p (20%) | 113Xe |- | CD (<.0034%) | 102Sn, 12C |-id=Barium-115 | rowspan=2|115Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 59 | rowspan=2|114.94748(22)# | rowspan=2|0.45(5) s | β+ | 115Cs | rowspan=2|5/2+# | rowspan=2| | rowspan=2| |- | β+, p (>15%) | 114Xe |-id=Barium-116 | rowspan=2|116Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 60 | rowspan=2|115.94162(22)# | rowspan=2|1.3(2) s | β+ (97%) | 116Cs | rowspan=2|0+ | rowspan=2| | rowspan=2| |- | β+, p (3%) | 115Xe |-id=Barium-117 | rowspan=3|117Ba | rowspan=3 style="text-align:right" | 56 | rowspan=3 style="text-align:right" | 61 | rowspan=3|116.93832(27) | rowspan=3|1.75(7) s | β+ (87%) | 117Cs | rowspan=3|(3/2+) | rowspan=3| | rowspan=3| |- | β+, p (13%) | 116Xe |- | β+, α (0.024%) | 113I |-id=Barium-118 | 118Ba | style="text-align:right" | 56 | style="text-align:right" | 62 | 117.93323(22)# | 5.2(2) s | β+ | 118Cs | 0+ | | |-id=Barium-119 | rowspan=2|119Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 63 | rowspan=2|118.93066(21) | rowspan=2|5.4(3) s | β+ (75%) | 119Cs | rowspan=2|(3/2+)[2] | rowspan=2| | rowspan=2| |- | β+, p (25%) | 118Xe |-id=Barium-119m | style="text-indent:1em" | 119mBa[2] | colspan="3" style="text-indent:2em" | 66.0 keV | 360(20) ns | IT | 119Ba | (5/2−) | | |-id=Barium-120 | 120Ba | style="text-align:right" | 56 | style="text-align:right" | 64 | 119.92604(32) | 24(2) s | β+ | 120Cs | 0+ | | |-id=Barium-121 | rowspan=2|121Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 65 | rowspan=2|120.92405(15) | rowspan=2|29.7(15) s | β+ (99.98%) | 121Cs | rowspan=2|5/2+ | rowspan=2| | rowspan=2| |- | β+, p (0.02%) | 120Xe |-id=Barium-122 | 122Ba | style="text-align:right" | 56 | style="text-align:right" | 66 | 121.91990(3) | 1.95(15) min | β+ | 122Cs | 0+ | | |-id=Barium-123 | 123Ba | style="text-align:right" | 56 | style="text-align:right" | 67 | 122.918781(13) | 2.7(4) min | β+ | 123Cs | 5/2+ | | |-id=Barium-123m | style="text-indent:1em" | 123mBa | colspan="3" style="text-indent:2em" | 120.95(8) keV | 830(60) ns | IT | 123Ba | 1/2+# | | |-id=Barium-124 | 124Ba | style="text-align:right" | 56 | style="text-align:right" | 68 | 123.915094(13) | 11.0(5) min | β+ | 124Cs | 0+ | | |-id=Barium-125 | 125Ba | style="text-align:right" | 56 | style="text-align:right" | 69 | 124.914472(12) | 3.3(3) min | β+ | 125Cs | 1/2+ | | |-id=Barium-125m | style="text-indent:1em" | 125mBa | colspan="3" style="text-indent:2em" | 120(20)# keV | 2.76(14) μs | IT | 125Ba | (7/2−) | | |-id=Barium-126 | 126Ba | style="text-align:right" | 56 | style="text-align:right" | 70 | 125.911250(13) | 100(2) min | β+ | 126Cs | 0+ | | |-id=Barium-127 | 127Ba | style="text-align:right" | 56 | style="text-align:right" | 71 | 126.911091(12) | 12.7(4) min | β+ | 127Cs | 1/2+ | | |-id=Barium-127m | style="text-indent:1em" | 127mBa | colspan="3" style="text-indent:2em" | 80.32(11) keV | 1.93(7) s | IT | 127Ba | 7/2− | | |-id=Barium-128 | 128Ba | style="text-align:right" | 56 | style="text-align:right" | 72 | 127.9083524(17) | 2.43(5) d | EC | 128Cs | 0+ | | |-id=Barium-129 | 129Ba | style="text-align:right" | 56 | style="text-align:right" | 73 | 128.908683(11) | 2.23(11) h | β+ | 129Cs | 1/2+ | | |-id=Barium-129m | rowspan=2 style="text-indent:1em" | 129mBa | rowspan=2 colspan="3" style="text-indent:2em" | 8.42(6) keV | rowspan=2|2.135(10) h | β+ | 129Cs | rowspan=2|7/2+ | rowspan=2| | rowspan=2| |- | IT? | 129Ba |-id=Barium-130 | 130Ba[n 1] | style="text-align:right" | 56 | style="text-align:right" | 74 | 129.9063260(3) | ≈ 1×1021 y | β+β+ | 130Xe | 0+ | 0.0011(1) | |-id=Barium-130m | style="text-indent:1em" | 130mBa | colspan="3" style="text-indent:2em" | 2475.12(18) keV | 9.54(14) ms | IT | 130Ba | 8− | | |-id=Barium-131 | 131Ba | style="text-align:right" | 56 | style="text-align:right" | 75 | 130.9069463(4) | 11.52(1) d | β+ | 131Cs | 1/2+ | | |-id=Barium-131m | style="text-indent:1em" | 131mBa | colspan="3" style="text-indent:2em" | 187.995(9) keV | 14.26(9) min | IT | 131Ba | 9/2− | | |-id=Barium-132 | 132Ba | style="text-align:right" | 56 | style="text-align:right" | 76 | 131.9050612(11) | colspan=3 align=center|Observationally Stable[n 2] | 0+ | 0.0010(1) | |-id=Barium-133 | 133Ba | style="text-align:right" | 56 | style="text-align:right" | 77 |132.9060074(11) | 10.5379(16) y | EC | 133Cs | 1/2+ | | |-id=Barium-133m | rowspan=2 style="text-indent:1em" | 133mBa | rowspan=2 colspan="3" style="text-indent:2em" | 288.252(9) keV | rowspan=2|38.90(6) h | IT (99.99%) | 133Ba | rowspan=2|11/2− | rowspan=2| | rowspan=2| |- | EC (0.0104%) | 133Cs |-id=Barium-134 | 134Ba[n 3] | style="text-align:right" | 56 | style="text-align:right" | 78 | 133.90450825(27) | colspan=3 align=center|Stable | 0+ | 0.0242(15) | |-id=Barium-134m | style="text-indent:1em" | 134mBa | colspan="3" style="text-indent:2em" | 2957.2(5) keV | 2.61(13) μs | IT | 134Ba | 10+ | | |-id=Barium-135 | 135Ba | style="text-align:right" | 56 | style="text-align:right" | 79 | 134.90568845(26) | colspan=3 align=center|Stable | 3/2+ | 0.0659(10) | |-id=Barium-135m1 | style="text-indent:1em" | 135m1Ba | colspan="3" style="text-indent:2em" | 268.218(20) keV | 28.11(2) h | IT | 135Ba | 11/2− | | |-id=Barium-135m2 | style="text-indent:1em" | 135m2Ba | colspan="3" style="text-indent:2em" | 2388.0(5) keV | 1.06(4) ms | IT | 135Ba | (23/2+) | | |-id=Barium-136 | 136Ba | style="text-align:right" | 56 | style="text-align:right" | 80 |135.90457580(26) | colspan=3 align=center|Stable | 0+ | 0.0785(24) | |-id=Barium-136m1 | style="text-indent:1em" | 136m1Ba | colspan="3" style="text-indent:2em" | 2030.535(18) keV | 308.4(19) ms | IT | 136Ba | 7− | | |-id=Barium-136m2 | style="text-indent:1em" | 136m2Ba | colspan="3" style="text-indent:2em" | 3357.19(25) keV | 91(2) ns | IT | 136Ba | 10+ | | |-id=Barium-137 | 137Ba[n 3] | style="text-align:right" | 56 | style="text-align:right" | 81 |136.90582721(27) | colspan=3 align=center|Stable | 3/2+ | 0.1123(23) | |-id=Barium-137m1 | style="text-indent:1em" | 137m1Ba[n 3] | colspan="3" style="text-indent:2em" | 661.659(3) keV | 2.552(1) min | IT | 137Ba | 11/2− | | |-id=Barium-137m2 | style="text-indent:1em" | 137m2Ba | colspan="3" style="text-indent:2em" | 2349.1(5) keV | 589(20) ns | IT | 137Ba | (19/2−) | | |-id=Barium-138 | 138Ba[n 3] | style="text-align:right" | 56 | style="text-align:right" | 82 | 137.90524706(27) | colspan=3 align=center|Stable | 0+ | 0.7170(29) | |-id=Barium-138m | style="text-indent:1em" | 138mBa | colspan="3" style="text-indent:2em" | 2090.536(21) keV | 850(100) ns | IT | 138Ba | 6+ | | |-id=Barium-139 | 139Ba[n 3] | style="text-align:right" | 56 | style="text-align:right" | 83 | 138.90884116(27) | 82.93(9) min | β | 139La | 7/2− | | |-id=Barium-140 | 140Ba[n 3] | style="text-align:right" | 56 | style="text-align:right" | 84 | 139.910608(8) | 12.7534(21) d | β | 140La | 0+ | | |-id=Barium-141 | 141Ba | style="text-align:right" | 56 | style="text-align:right" | 85 | 140.914404(6) | 18.27(7) min | β | 141La | 3/2− | | |-id=Barium-142 | 142Ba | style="text-align:right" | 56 | style="text-align:right" | 86 | 141.916433(6) | 10.6(2) min | β | 142La | 0+ | | |-id=Barium-143 | 143Ba | style="text-align:right" | 56 | style="text-align:right" | 87 | 142.920625(7) | 14.5(3) s | β | 143La | 5/2− | | |-id=Barium-144 | 144Ba | style="text-align:right" | 56 | style="text-align:right" | 88 |143.922955(8) | 11.73(8) s | β | 144La | 0+ | | |-id=Barium-145 | 145Ba | style="text-align:right" | 56 | style="text-align:right" | 89 | 144.927518(9) | 4.31(16) s | β | 145La | 5/2− | | |-id=Barium-146 | 146Ba | style="text-align:right" | 56 | style="text-align:right" | 90 | 145.9303632(19) | 2.15(4) s | β | 146La | 0+ | | |-id=Barium-147 | rowspan=2|147Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 91 | rowspan=2|146.935304(21) | rowspan=2|893(1) ms | β (99.93%) | 147La | rowspan=2|5/2− | rowspan=2| | rowspan=2| |- | β, n (0.07%) | 146La |-id=Barium-148 | rowspan=2|148Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 92 | rowspan=2| 147.9382230(16) | rowspan=2|620(5) ms | β (99.6%) | 148La | rowspan=2|0+ | rowspan=2| | rowspan=2| |- | β, n (0.4%) | 147La |-id=Barium-149 | rowspan=2|149Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 93 | rowspan=2|148.9432840(27) | rowspan=2|349(4) ms | β (96.1%) | 149La | rowspan=2|3/2−# | rowspan=2| | rowspan=2| |- | β, n (3.9%) | 148La |-id=Barium-150 | rowspan=2|150Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 94 | rowspan=2| 149.946441(6) | rowspan=2|258(5) ms | β (99.0%) | 150La | rowspan=2|0+ | rowspan=2| | rowspan=2| |- | β, n (1.0%) | 149La |-id=Barium-151 | rowspan=2|151Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 95 | rowspan=2|150.95176(43)# | rowspan=2|167(5) ms | β | 151La | rowspan=2|3/2−# | rowspan=2| | rowspan=2| |- | β, n? | 150La |-id=Barium-152 | rowspan=2|152Ba | rowspan=2 style="text-align:right" | 56 | rowspan=2 style="text-align:right" | 96 | rowspan=2|151.95533(43)# | rowspan=2|139(8) ms | β | 152La | rowspan=2|0+ | rowspan=2| | rowspan=2| |- | β, n? | 151La |-id=Barium-153 | rowspan=3|153Ba | rowspan=3 style="text-align:right" | 56 | rowspan=3 style="text-align:right" | 97 | rowspan=3|152.96085(43)# | rowspan=3|113(39) ms | β | 153La | rowspan=3|5/2−# | rowspan=3| | rowspan=3| |- | β, n? | 152La |- | β, 2n? | 151La |-id=Barium-154 | 154Ba | style="text-align:right" | 56 | style="text-align:right" | 98 |153.96466(54)# | 53(48) ms | β | 154La | 0+ | | Template:Isotopes table/footer

See also

Daughter products other than barium

References

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