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Isotopes of barium

From Wikipedia, the free encyclopedia

Isotopes ofbarium (56Ba)
Main isotopes[1]Decay
Isotopeabun­dancehalf-life(t1/2)modepro­duct
130Ba0.11%(0.5–2.7)×1021 yεε130Xe
131Basynth11.52 dβ+131Cs
132Ba0.1%stable
133Basynth10.538 yε133Cs
134Ba2.42%stable
135Ba6.59%stable
136Ba7.85%stable
137Ba11.2%stable
138Ba71.7%stable
140Basynth12.753 dβ140La
Standard atomic weightAr°(Ba)

Naturally occurringbarium (56Ba) is a mix of six stableisotopes 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,[4][5] presumably decaying bydouble electron capture with a half-life of (0.5–2.7)×1021 years (about 1011 times the age of the universe). The two measurements are discordant; the above reflects the total range, the value in the table below is a crude average.

With the total range of mass numbers known 114 to 154, there are thirty-three knownradioisotopes in addition to130Ba. The longest-lived of these is133Ba, which has a half-life of 10.538 years; all others have half-lives shorter than two weeks. The longest-livedisomers are133mBa at 38.90 hours and135m1Ba at 28.11 hours. The analogous137m1Ba (half-life 2.552 minutes) occurs in the decay of the common fission productcaesium-137.

Barium-114 is theorized to undergocluster decay, emitting a nucleus of stable12C to produce102Sn. This decay has not been observed, with only an upper limit on the branching ratio of such decay (0.0034%).

List of isotopes

[edit]

Nuclide
[n 1]
ZNIsotopic mass(Da)[6]
[n 2][n 3]
Half-life[1]
Decay
mode
[1]
[n 4]
Daughter
isotope

[n 5][n 6]
Spin and
parity[1]
[n 7][n 8]
Natural abundance(mole fraction)
Excitation energyNormal proportion[1]Range of variation
114Ba5658113.95072(11)460(125) msβ+ (79%)114Cs0+
α (0.9%)110Xe
β+,p (20%)113Xe
CD (<.0034%)102Sn,12C
115Ba5659114.94748(22)#0.45(5) sβ+115Cs5/2+#
β+, p (>15%)114Xe
116Ba5660115.94162(22)#1.3(2) sβ+ (97%)116Cs0+
β+, p (3%)115Xe
117Ba5661116.93832(27)1.75(7) sβ+ (87%)117Cs(3/2+)
β+, p (13%)116Xe
β+, α (0.024%)113I
118Ba5662117.93323(22)#5.2(2) sβ+118Cs0+
119Ba5663118.93066(21)5.4(3) sβ+ (75%)119Cs(3/2+)[7]
β+, p (25%)118Xe
119mBa[7]66.0 keV360(20) nsIT119Ba(5/2−)
120Ba5664119.92604(32)24(2) sβ+120Cs0+
121Ba5665120.92405(15)29.7(15) sβ+ (99.98%)121Cs5/2+
β+, p (0.02%)120Xe
122Ba5666121.91990(3)1.95(15) minβ+122Cs0+
123Ba5667122.918781(13)2.7(4) minβ+123Cs5/2+
123mBa120.95(8) keV830(60) nsIT123Ba1/2+#
124Ba5668123.915094(13)11.0(5) minβ+124Cs0+
125Ba5669124.914472(12)3.3(3) minβ+125Cs1/2+
125mBa120(20)# keV2.76(14) μsIT125Ba(7/2−)
126Ba5670125.911250(13)100(2) minβ+126Cs0+
127Ba5671126.911091(12)12.7(4) minβ+127Cs1/2+
127mBa80.32(11) keV1.93(7) sIT127Ba7/2−
128Ba5672127.9083524(17)2.43(5) dEC128Cs0+
129Ba5673128.908683(11)2.23(11) hβ+129Cs1/2+
129mBa8.42(6) keV2.135(10) hβ+129Cs7/2+
IT?129Ba
130Ba[n 9]5674129.9063260(3)≈ 1×1021 yεε130Xe0+0.0011(1)
130mBa2475.12(18) keV9.54(14) msIT130Ba8−
131Ba5675130.9069463(4)11.52(1) dβ+131Cs1/2+
131mBa187.995(9) keV14.26(9) minIT131Ba9/2−
132Ba5676131.9050612(11)Observationally Stable[n 10]0+0.0010(1)
133Ba5677132.9060074(11)10.5379(16) yEC133Cs1/2+
133mBa288.252(9) keV38.90(6) hIT (99.99%)133Ba11/2−
EC (0.0104%)133Cs
134Ba[n 11]5678133.90450825(27)Stable0+0.0242(15)
134mBa2957.2(5) keV2.61(13) μsIT134Ba10+
135Ba5679134.90568845(26)Stable3/2+0.0659(10)
135m1Ba268.218(20) keV28.11(2) hIT135Ba11/2−
135m2Ba2388.0(5) keV1.06(4) msIT135Ba(23/2+)
136Ba5680135.90457580(26)Stable0+0.0785(24)
136m1Ba2030.535(18) keV308.4(19) msIT136Ba7−
136m2Ba3357.19(25) keV91(2) nsIT136Ba10+
137Ba[n 11]5681136.90582721(27)Stable3/2+0.1123(23)
137m1Ba[n 11]661.659(3) keV2.552(1) minIT137Ba11/2−
137m2Ba2349.1(5) keV589(20) nsIT137Ba(19/2−)
138Ba[n 11]5682137.90524706(27)Stable0+0.7170(29)
138mBa2090.536(21) keV850(100) nsIT138Ba6+
139Ba[n 11]5683138.90884116(27)82.93(9) minβ139La7/2−
140Ba[n 11]5684139.910608(8)12.7534(21) dβ140La0+
141Ba5685140.914404(6)18.27(7) minβ141La3/2−
142Ba5686141.916433(6)10.6(2) minβ142La0+
143Ba5687142.920625(7)14.5(3) sβ143La5/2−
144Ba5688143.922955(8)11.73(8) sβ144La0+
145Ba5689144.927518(9)4.31(16) sβ145La5/2−
146Ba5690145.9303632(19)2.15(4) sβ146La0+
147Ba5691146.935304(21)893(1) msβ (99.93%)147La5/2−
β, n (0.07%)146La
148Ba5692147.9382230(16)620(5) msβ (99.6%)148La0+
β, n (0.4%)147La
149Ba5693148.9432840(27)349(4) msβ (96.1%)149La3/2−#
β, n (3.9%)148La
150Ba5694149.946441(6)258(5) msβ (99.0%)150La0+
β, n (1.0%)149La
151Ba5695150.95176(43)#167(5) msβ151La3/2−#
β, n?150La
152Ba5696151.95533(43)#139(8) msβ152La0+
β, n?151La
153Ba5697152.96085(43)#113(39) msβ153La5/2−#
β, n?152La
β, 2n?151La
154Ba5698153.96466(54)#53(48) msβ154La0+
This table header & footer:
  1. ^mBa – Excitednuclear isomer.
  2. ^( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
  3. ^# – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  4. ^Modes of decay:
    EC:Electron capture
    CD:Cluster decay
    IT:Isomeric transition
    n:Neutron emission
    p:Proton emission
  5. ^Bold italics symbol as daughter – Daughter product is nearly stable.
  6. ^Bold symbol as daughter – Daughter product is stable.
  7. ^( ) spin value – Indicates spin with weak assignment arguments.
  8. ^# – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  9. ^Primordial radionuclide
  10. ^Believed to undergo β+β+ decay to132Xe with ahalf-life over 3×1020 years
  11. ^abcdefFission product

See also

[edit]

Daughter products other than barium

References

[edit]
  1. ^abcdeKondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021)."The NUBASE2020 evaluation of nuclear properties"(PDF).Chinese Physics C.45 (3) 030001.doi:10.1088/1674-1137/abddae.
  2. ^"Standard Atomic Weights: Barium".CIAAW. 1985.
  3. ^Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04)."Standard atomic weights of the elements 2021 (IUPAC Technical Report)".Pure and Applied Chemistry.doi:10.1515/pac-2019-0603.ISSN 1365-3075.
  4. ^Meshik, A.P.; Hohenberg, C.M.; Pravdivtseva, O.V.; Kapusta, Y.S. (2001)."Weak decay of130Ba and132Ba: Geochemical measurements".Physical Review C.64 (3): 035205–1–035205–6.Bibcode:2001PhRvC..64c5205M.doi:10.1103/PhysRevC.64.035205.
  5. ^M. Pujol; B. Marty; P. Burnard; P. Philippot (2009). "Xenon in Archean barite: Weak decay of130Ba, mass-dependent isotopic fractionation and implication for barite formation".Geochimica et Cosmochimica Acta.73 (22):6834–6846.Bibcode:2009GeCoA..73.6834P.doi:10.1016/j.gca.2009.08.002.
  6. ^Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*".Chinese Physics C.45 (3) 030003.doi:10.1088/1674-1137/abddaf.
  7. ^abZheng, K. K.; Petrache, C. M.; Zhang, Z. H.; Astier, A.; Lv, B. F.; Greenlees, P. T.; Grahn, T.; Julin, R.; Juutinen, S.; Luoma, M.; Ojala, J.; Pakarinen, J.; Partanen, J.; Rahkila, P.; Ruotsalainen, P.; Sandzelius, M.; Sarén, J.; Tann, H.; Uusitalo, J.; Zimba, G.; Cederwall, B.; Aktas, ö.; Ertoprak, A.; Zhang, W.; Guo, S.; Liu, M. L.; Zhou, X. H.; Kuti, I.; Nyakó, B. M.; Sohler, D.; Timár, J.; Andreoiu, C.; Doncel, M.; Joss, D. T.; Page, R. D. (30 July 2021)."Neutron excitations in Ba 119"(PDF).Physical Review C.104 (1) 014326.doi:10.1103/PhysRevC.104.014326.
Group12 3456789101112131415161718
PeriodHydrogen and
alkali metals
Alkaline
earth metals
Pnicto­gensChal­co­gensHalo­gensNoble gases
12
345678910
1112131415161718
192021222324252627282930313233343536
373839404142434445464748495051525354
55561 asterisk71727374757677787980818283848586
87881 asterisk103104105106107108109110111112113114115116117118
119120
1 asterisk5758596061626364656667686970 
1 asterisk8990919293949596979899100101102
Authority control databasesEdit this at Wikidata
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