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Isotopes of barium: Difference between revisions

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{{Short description|Nuclides with atomic number of 56 but with different mass numbers}}
{{infobox barium isotopes}}
{{Infobox barium isotopes}}
Naturally occurring [[barium]] (<sub>56</sub>Ba) is a mix of six stable [[isotope]]s 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.<ref name=Ba130>{{cite journal |last=Meshik |first=A.P. |last2=Hohenberg |first2=C.M. |last3=Pravdivtseva |first3=O.V. |last4=Kapusta |first4=Y.S. |title=Weak decay of <sup>130</sup>Ba and <sup>132</sup>Ba: Geochemical measurements |date=2001 |journal=Physical Review C |volume=64 |issue=3 |pages=035205–1–035205–6 |doi=10.1103/PhysRevC.64.035205|url=https://zenodo.org/record/1063702 |bibcode=2001PhRvC..64c5205M }}</ref> This nuclide decays by [[double electron capture]] (absorbing two electrons and emitting two neutrinos), with a half-life of (0.5–2.7)×10<sup>21</sup> years (about 10<sup>11</sup> times the age of the universe).
Naturally occurring [[barium]] (<sub>56</sub>Ba) is a mix of six stable [[isotope]]s 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.<ref name="Ba130">{{cite journal |last=Meshik |first=A.P. |last2=Hohenberg |first2=C.M. |last3=Pravdivtseva |first3=O.V. |last4=Kapusta |first4=Y.S. |title=Weak decay of <sup>130</sup>Ba and <sup>132</sup>Ba: Geochemical measurements |date=2001 |journal=Physical Review C |volume=64 |issue=3 |pages=035205–1–035205–6 |doi=10.1103/PhysRevC.64.035205|url=https://zenodo.org/record/1063702 |bibcode=2001PhRvC..64c5205M }}</ref> This nuclide decays by [[double electron capture]] (absorbing two electrons and emitting two neutrinos), with a half-life of (0.5–2.7)×10<sup>21</sup> years (about 10<sup>11</sup> times the age of the universe).


There are a total of thirty-three known [[radioisotope]]s in addition to <sup>130</sup>Ba. The longest-lived of these is <sup>133</sup>Ba, which has a half-life of 10.51 years. All other radioisotopes have half-lives shorter than two weeks. The longest-lived [[nuclear isomer|isomer]] is <sup>133m</sup>Ba, which has a half-life of 38.9 hours, though the shorter-lived <sup>137m</sup>Ba (half-life 2.55 minutes) arises as the decay product of the common fission product [[caesium-137]].
There are a total of thirty-three known [[radioisotope]]s in addition to <sup>130</sup>Ba. The longest-lived of these is <sup>133</sup>Ba, which has a half-life of 10.51 years. All other radioisotopes have half-lives shorter than two weeks. The longest-lived [[nuclear isomer|isomer]] is <sup>133m</sup>Ba, which has a half-life of 38.9 hours. The shorter-lived <sup>137m</sup>Ba (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 [[Carbon-12|<sup>12</sup>C]] to produce <sup>102</sup>Sn. However this decay is not yet observed; the upper limit on the branching ratio of such decay is 0.0034%.
Barium-114 is predicted to undergo [[cluster decay]], emitting a nucleus of stable [[Carbon-12|<sup>12</sup>C]] to produce <sup>102</sup>Sn. However this decay is not yet observed; the upper limit on the branching ratio of such decay is 0.0034%.
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{{Isotopes table
{{Isotopes table
|symbol=Ba
|symbol=Ba
|refs=NUBASE2020, AME2020 II
|refs=<!-- not NUBASE2016 yet (2019-07-14) -->
|notes=m, unc(), mass#, spin(), spin#, daughter-st, daughter-nst, CD, EC, IT, n, p
|notes=m, unc(), mass#, spin(), spin#, daughter-st, daughter-nst, CD, EC, IT, n, p
}}
}}
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| rowspan=4 style="text-align:right" | 56
| rowspan=4 style="text-align:right" | 56
| rowspan=4 style="text-align:right" | 58
| rowspan=4 style="text-align:right" | 58
| rowspan=4|113.95068(15)
| rowspan=4|113.95072(11)
| rowspan=4|530(230)&nbsp;ms<br>[0.43(+30−15)&nbsp;s]
| rowspan=4|460(125)&nbsp;ms
| [[beta decay|β<sup>+</sup>]], [[proton emission|p]] (99.59%)
| [[beta decay|β<sup>+</sup>]] (79%)
| <sup>113</sup>Xe
| <sup>114</sup>Cs
| rowspan=4|0+
| rowspan=4|0+
| rowspan=4|
| rowspan=4|
| rowspan=4|
| rowspan=4|
|-
|-
| [[alpha decay|α]] (.37%)
| [[alpha decay|α]] (0.9%)
| <sup>110</sup>Xe
| <sup>110</sup>Xe
|-
|-
| β<sup>+</sup> (.04%)
| β<sup>+</sup>, [[proton emission|p]] (20%)
| <sup>114</sup>Cs
| <sup>113</sup>Xe
|-
|-
| [[cluster decay|CD]] (<.0034%)<ref group="n">Cluster decay is predicted but had never been observed.</ref>
| [[cluster decay|CD]] (<.0034%)
| <sup>102</sup>Sn, '''[[carbon-12|<sup>12</sup>C]]'''
| <sup>102</sup>Sn, '''[[carbon-12|<sup>12</sup>C]]'''
|-
|-
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| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 59
| rowspan=2 style="text-align:right" | 59
| rowspan=2|114.94737(64)#
| rowspan=2|114.94748(22)#
| rowspan=2|0.45(5)&nbsp;s
| rowspan=2|0.45(5)&nbsp;s
| β<sup>+</sup>
| β<sup>+</sup>
| <sup>115</sup>Cs
| <sup>115</sup>Cs
| rowspan=2|(5/2+)#
| rowspan=2|5/2+#
| rowspan=2|
| rowspan=2|
| rowspan=2|
| rowspan=2|
|-
|-
| β<sup>+</sup>, p
| β<sup>+</sup>, p (>15%)
| <sup>114</sup>Xe
| <sup>114</sup>Xe
|-
|-
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| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 60
| rowspan=2 style="text-align:right" | 60
| rowspan=2|115.94138(43)#
| rowspan=2|115.94162(22)#
| rowspan=2|1.3(2)&nbsp;s
| rowspan=2|1.3(2)&nbsp;s
| β<sup>+</sup>
| β<sup>+</sup> (97%)
| <sup>116</sup>Cs
| <sup>116</sup>Cs
| rowspan=2|0+
| rowspan=2|0+
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| rowspan=2|
| rowspan=2|
|-
|-
| β<sup>+</sup>, p
| β<sup>+</sup>, p (3%)
| <sup>115</sup>Xe
| <sup>115</sup>Xe
|-
|-
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| rowspan=3 style="text-align:right" | 56
| rowspan=3 style="text-align:right" | 56
| rowspan=3 style="text-align:right" | 61
| rowspan=3 style="text-align:right" | 61
| rowspan=3|116.93850(32)#
| rowspan=3|116.93832(27)
| rowspan=3|1.75(7)&nbsp;s
| rowspan=3|1.75(7)&nbsp;s
| β<sup>+</sup>
| β<sup>+</sup> (87%)
| <sup>117</sup>Cs
| <sup>117</sup>Cs
| rowspan=3|(3/2)(+#)
| rowspan=3|(3/2+)
| rowspan=3|
| rowspan=3|
| rowspan=3|
| rowspan=3|
|-
|-
| β<sup>+</sup>, α
| β<sup>+</sup>, p (13%)
| <sup>116</sup>Xe
|-
| β<sup>+</sup>, α (0.024%)
| <sup>113</sup>I
| <sup>113</sup>I
|-
|-
| β<sup>+</sup>, p
| <sup>118</sup>Ba
| style="text-align:right" | 56
| <sup>116</sup>Xe
| style="text-align:right" | 62
|-
| 117.93323(22)#
| rowspan=2|<sup>118</sup>Ba
| 5.2(2)&nbsp;s
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 62
| rowspan=2|117.93304(21)#
| rowspan=2|5.2(2)&nbsp;s
| β<sup>+</sup>
| β<sup>+</sup>
| <sup>118</sup>Cs
| <sup>118</sup>Cs
| rowspan=2|0+
| 0+
|
| rowspan=2|
|
| rowspan=2|
|-
| β<sup>+</sup>, p
| <sup>117</sup>Xe
|-
|-
| rowspan=2|<sup>119</sup>Ba
| rowspan=2|<sup>119</sup>Ba
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| rowspan=2|118.93066(21)
| rowspan=2|118.93066(21)
| rowspan=2|5.4(3)&nbsp;s
| rowspan=2|5.4(3)&nbsp;s
| β<sup>+</sup>
| β<sup>+</sup> (75%)
| <sup>119</sup>Cs
| <sup>119</sup>Cs
| rowspan=2|(5/2+)
| rowspan=2|(5/2+)
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| rowspan=2|
| rowspan=2|
|-
|-
| β<sup>+</sup>, p
| β<sup>+</sup>, p (25%)
| <sup>118</sup>Xe
| <sup>118</sup>Xe
|-
|-
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| β<sup>+</sup> (99.98%)
| β<sup>+</sup> (99.98%)
| <sup>121</sup>Cs
| <sup>121</sup>Cs
| rowspan=2|5/2(+)
| rowspan=2|5/2+
| rowspan=2|
| rowspan=2|
| rowspan=2|
| rowspan=2|
|-
|-
| β<sup>+</sup>, p (.02%)
| β<sup>+</sup>, p (0.02%)
| <sup>120</sup>Xe
| <sup>120</sup>Xe
|-
|-
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| β<sup>+</sup>
| β<sup>+</sup>
| <sup>123</sup>Cs
| <sup>123</sup>Cs
| 5/2(+)
| 5/2+
|
|
|-
| style="text-indent:1em" | <sup>123m</sup>Ba
| colspan="3" style="text-indent:2em" | 120.95(8)&nbsp;keV
| 830(60)&nbsp;ns
| [[Isomeric transition|IT]]
| <sup>123</sup>Ba
| 1/2+#
|
|
|
|
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 69
| style="text-align:right" | 69
| 124.914473(12)
| 124.914472(12)
| 3.5(4)&nbsp;min
| 3.3(3)&nbsp;min
| β<sup>+</sup>
| β<sup>+</sup>
| <sup>125</sup>Cs
| <sup>125</sup>Cs
| 1/2(+#)
| 1/2+
|
|
|-
| style="text-indent:1em" | <sup>125m</sup>Ba
| colspan="3" style="text-indent:2em" | 120(20)#&nbsp;keV
| 2.76(14)&nbsp;μs
| IT
| <sup>125</sup>Ba
| (7/2−)
|
|
|
|
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 71
| style="text-align:right" | 71
| 126.911094(12)
| 126.911091(12)
| 12.7(4)&nbsp;min
| 12.7(4)&nbsp;min
| β<sup>+</sup>
| β<sup>+</sup>
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|-
|-
| style="text-indent:1em" | <sup>127m</sup>Ba
| style="text-indent:1em" | <sup>127m</sup>Ba
| colspan="3" style="text-indent:2em" | 80.33(12)&nbsp;keV
| colspan="3" style="text-indent:2em" | 80.32(11)&nbsp;keV
| 1.9(2)&nbsp;s
| 1.93(7)&nbsp;s
| IT
| [[Isomeric transition|IT]]
| <sup>127</sup>Ba
| <sup>127</sup>Ba
| 7/2−
| 7/2−
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 72
| style="text-align:right" | 72
| 127.908318(11)
| 127.9083524(17)
| 2.43(5)&nbsp;d
| 2.43(5)&nbsp;d
| [[electron capture|EC]]
| β<sup>+</sup>
| <sup>128</sup>Cs
| <sup>128</sup>Cs
| 0+
| 0+
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 73
| style="text-align:right" | 73
| 128.908679(12)
| 128.908683(11)
| 2.23(11)&nbsp;h
| 2.23(11)&nbsp;h
| β<sup>+</sup>
| β<sup>+</sup>
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| rowspan=2 style="text-indent:1em" | <sup>129m</sup>Ba
| rowspan=2 style="text-indent:1em" | <sup>129m</sup>Ba
| rowspan=2 colspan="3" style="text-indent:2em" | 8.42(6)&nbsp;keV
| rowspan=2 colspan="3" style="text-indent:2em" | 8.42(6)&nbsp;keV
| rowspan=2|2.16(2)&nbsp;h
| rowspan=2|2.135(10)&nbsp;h
| β<sup>+</sup>
| β<sup>+</sup>
| <sup>129</sup>Cs
| <sup>129</sup>Cs
| rowspan=2|7/2+#
| rowspan=2|7/2+
| rowspan=2|
| rowspan=2|
| rowspan=2|
| rowspan=2|
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 74
| style="text-align:right" | 74
| 129.9063208(30)
| 129.9063260(3)
| '''1.6(±1.1)×10<sup>21</sup>&nbsp;y'''
| '''≈&nbsp;1×10<sup>21</sup>&nbsp;y'''
| [[Double electron capture|Double EC]]
| [[Double electron capture|2EC]]?
| '''<sup>130</sup>Xe'''
| '''<sup>130</sup>Xe'''
| 0+
| 0+
| 0.00106(1)
| 0.0011(1)
|
|
|-
|-
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 75
| style="text-align:right" | 75
| 130.906941(3)
| 130.9069463(4)
| 11.50(6)&nbsp;d
| 11.52(1)&nbsp;d
| β<sup>+</sup>
| β<sup>+</sup>
| <sup>131</sup>Cs
| <sup>131</sup>Cs
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|-
|-
| style="text-indent:1em" | <sup>131m</sup>Ba
| style="text-indent:1em" | <sup>131m</sup>Ba
| colspan="3" style="text-indent:2em" | 187.14(12)&nbsp;keV
| colspan="3" style="text-indent:2em" | 187.995(9)&nbsp;keV
| 14.6(2)&nbsp;min
| 14.26(9)&nbsp;min
| IT
| IT
| <sup>131</sup>Ba
| <sup>131</sup>Ba
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 76
| style="text-align:right" | 76
| 131.9050613(11)
| 131.9050612(11)
| colspan=3 align=center|[[Observationally Stable]]<ref group="n">Believed to undergo β<sup>+</sup>β<sup>+</sup> decay to '''<sup>132</sup>Xe''' with a [[half-life]] over 300×10<sup>18</sup> years</ref>
| colspan=3 align=center|'''[[Observationally Stable]]'''<ref group="n">Believed to undergo β<sup>+</sup>β<sup>+</sup> decay to '''<sup>132</sup>Xe''' with a [[half-life]] over 3×10<sup>20</sup> years</ref>
| 0+
| 0+
| 0.00101(1)
| 0.0010(1)
|
|
|-
|-
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 77
| style="text-align:right" | 77
| 132.9060075(11)
|132.9060074(11)
| 10.51(5)&nbsp;y
| 10.5379(16)&nbsp;y
| EC
| EC
| '''<sup>133</sup>Cs'''
| '''<sup>133</sup>Cs'''
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|-
|-
| rowspan=2 style="text-indent:1em" | <sup>133m</sup>Ba
| rowspan=2 style="text-indent:1em" | <sup>133m</sup>Ba
| rowspan=2 colspan="3" style="text-indent:2em" | 288.247(9)&nbsp;keV
| rowspan=2 colspan="3" style="text-indent:2em" | 288.252(9)&nbsp;keV
| rowspan=2|38.9(1)&nbsp;h
| rowspan=2|38.90(6)&nbsp;h
| IT (99.99%)
| IT (99.99%)
| <sup>133</sup>Ba
| <sup>133</sup>Ba
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| rowspan=2|
| rowspan=2|
|-
|-
| EC (.0096%)
| EC (0.0104%)
| '''<sup>133</sup>Cs'''
| '''<sup>133</sup>Cs'''
|-
|-
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 78
| style="text-align:right" | 78
| 133.9045084(4)
| 133.90450825(27)
| colspan=3 align=center|'''Stable'''
| colspan=3 align=center|'''Stable'''
| 0+
| 0+
| 0.02417(18)
| 0.0242(15)
|
|-
| style="text-indent:1em" | <sup>134m</sup>Ba
| colspan="3" style="text-indent:2em" | 2957.2(5)&nbsp;keV
| 2.61(13)&nbsp;μs
| IT
| '''<sup>134</sup>Ba'''
| 10+
|
|
|
|-
|-
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| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 79
| style="text-align:right" | 79
| 134.9056886(4)
| 134.90568845(26)
| colspan=3 align=center|'''Stable'''
| colspan=3 align=center|'''Stable'''
| 3/2+
| 3/2+
| 0.06592(12)
| 0.0659(10)
|
|
|-
|-
| style="text-indent:1em" | <sup>135m</sup>Ba
| style="text-indent:1em" | <sup>135m1</sup>Ba
| colspan="3" style="text-indent:2em" | 268.22(2)&nbsp;keV
| colspan="3" style="text-indent:2em" | 268.218(20)&nbsp;keV
| 28.7(2)&nbsp;h
| 28.11(2)&nbsp;h
| IT
| IT
| '''<sup>135</sup>Ba'''
| '''<sup>135</sup>Ba'''
| 11/2−
| 11/2−
|
|
|-
| style="text-indent:1em" | <sup>135m2</sup>Ba
| colspan="3" style="text-indent:2em" | 2388.0(5)&nbsp;keV
| 1.06(4)&nbsp;ms
| IT
| '''<sup>135</sup>Ba'''
| (23/2+)
|
|
|
|
Line 346: Line 380:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 80
| style="text-align:right" | 80
| 135.9045759(4)
|135.90457580(26)
| colspan=3 align=center|'''Stable'''
| colspan=3 align=center|'''Stable'''
| 0+
| 0+
| 0.07854(24)
| 0.0785(24)
|
|
|-
|-
| style="text-indent:1em" | <sup>136m</sup>Ba
| style="text-indent:1em" | <sup>136m1</sup>Ba
| colspan="3" style="text-indent:2em" | 2030.466(18)&nbsp;keV
| colspan="3" style="text-indent:2em" | 2030.535(18)&nbsp;keV
| 308.4(19)&nbsp;ms
| 308.4(19)&nbsp;ms
| IT
| IT
| '''<sup>136</sup>Ba'''
| '''<sup>136</sup>Ba'''
| 7−
| 7−
|
|
|-
| style="text-indent:1em" | <sup>136m2</sup>Ba
| colspan="3" style="text-indent:2em" | 3357.19(25)&nbsp;keV
| 91(2)&nbsp;ns
| IT
| '''<sup>136</sup>Ba'''
| 10+
|
|
|
|
Line 364: Line 407:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 81
| style="text-align:right" | 81
| 136.9058274(5)
|136.90582721(27)
| colspan=3 align=center|'''Stable'''
| colspan=3 align=center|'''Stable'''
| 3/2+
| 3/2+
| 0.11232(24)
| 0.1123(23)
|
|
|-
|-
Line 380: Line 423:
|-
|-
| style="text-indent:1em" | <sup>137m2</sup>Ba
| style="text-indent:1em" | <sup>137m2</sup>Ba
| colspan="3" style="text-indent:2em" | 2349.1(4)&nbsp;keV
| colspan="3" style="text-indent:2em" | 2349.1(5)&nbsp;keV
| 0.59(10)&nbsp;µs
| 589(20)&nbsp;ns
|
| IT
| '''<sup>137</sup>Ba'''
|
| (17/2−)
| (19/2−)
|
|
|
|
Line 391: Line 434:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 82
| style="text-align:right" | 82
| 137.9052472(5)
| 137.90524706(27)
| colspan=3 align=center|'''Stable'''
| colspan=3 align=center|'''Stable'''
| 0+
| 0+
| 0.71698(42)
| 0.7170(29)
|
|
|-
|-
| style="text-indent:1em" | <sup>138m</sup>Ba
| style="text-indent:1em" | <sup>138m</sup>Ba
| colspan="3" style="text-indent:2em" | 2090.54(6)&nbsp;keV
| colspan="3" style="text-indent:2em" | 2090.536(21)&nbsp;keV
| 800(100)&nbsp;ns
| 850(100)&nbsp;ns
|
| IT
| '''<sup>138</sup>Ba'''
|
| 6+
| 6+
|
|
Line 409: Line 452:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 83
| style="text-align:right" | 83
| 138.9088413(5)
| 138.90884116(27)
| 83.06(28)&nbsp;min
| 82.93(9)&nbsp;min
| β<sup>−</sup>
| β<sup>−</sup>
| '''<sup>139</sup>La'''
| '''<sup>139</sup>La'''
Line 420: Line 463:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 84
| style="text-align:right" | 84
| 139.910605(9)
| 139.910608(8)
| 12.752(3)&nbsp;d
| 12.7534(21)&nbsp;d
| β<sup>−</sup>
| β<sup>−</sup>
| <sup>140</sup>La
| <sup>140</sup>La
Line 431: Line 474:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 85
| style="text-align:right" | 85
| 140.914411(9)
| 140.914404(6)
| 18.27(7)&nbsp;min
| 18.27(7)&nbsp;min
| β<sup>−</sup>
| β<sup>−</sup>
Line 442: Line 485:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 86
| style="text-align:right" | 86
| 141.916453(7)
| 141.916433(6)
| 10.6(2)&nbsp;min
| 10.6(2)&nbsp;min
| β<sup>−</sup>
| β<sup>−</sup>
Line 453: Line 496:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 87
| style="text-align:right" | 87
| 142.920627(14)
| 142.920625(7)
| 14.5(3)&nbsp;s
| 14.5(3)&nbsp;s
| β<sup>−</sup>
| β<sup>−</sup>
Line 464: Line 507:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 88
| style="text-align:right" | 88
| 143.922953(14)
|143.922955(8)
| 11.5(2)&nbsp;s
| 11.73(8)&nbsp;s
| β<sup>−</sup>
| β<sup>−</sup>
| <sup>144</sup>La
| <sup>144</sup>La
Line 475: Line 518:
| style="text-align:right" | 56
| style="text-align:right" | 56
| style="text-align:right" | 89
| style="text-align:right" | 89
| 144.92763(8)
| 144.927518(9)
| 4.31(16)&nbsp;s
| 4.31(16)&nbsp;s
| β<sup>−</sup>
| β<sup>−</sup>
Line 483: Line 526:
|
|
|-
|-
| rowspan=2|<sup>146</sup>Ba
| <sup>146</sup>Ba
| rowspan=2 style="text-align:right" | 56
| style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 90
| style="text-align:right" | 90
| rowspan=2|145.93022(8)
| 145.9303632(19)
| rowspan=2|2.22(7)&nbsp;s
| 2.15(4)&nbsp;s
| β<sup>−</sup> (99.98%)
| β<sup>−</sup>
| <sup>146</sup>La
| <sup>146</sup>La
| rowspan=2|0+
| 0+
|
| rowspan=2|
|
| rowspan=2|
|-
| β<sup>−</sup>, [[neutron emission|n]] (.02%)
| <sup>145</sup>La
|-
|-
| rowspan=2|<sup>147</sup>Ba
| rowspan=2|<sup>147</sup>Ba
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 91
| rowspan=2 style="text-align:right" | 91
| rowspan=2|146.93495(22)#
| rowspan=2|146.935304(21)
| rowspan=2|0.893(1)&nbsp;s
| rowspan=2|893(1)&nbsp;ms
| β<sup>−</sup> (99.94%)
| β<sup>−</sup> (99.93%)
| <sup>147</sup>La
| <sup>147</sup>La
| rowspan=2|(3/2+)
| rowspan=2|5/2−
| rowspan=2|
| rowspan=2|
| rowspan=2|
| rowspan=2|
|-
|-
| β<sup>−</sup>, n (.06%)
| β<sup>−</sup>, n (0.07%)
| <sup>146</sup>La
| <sup>146</sup>La
|-
|-
Line 514: Line 554:
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 92
| rowspan=2 style="text-align:right" | 92
| rowspan=2|147.93772(9)
| rowspan=2| 147.9382230(16)
| rowspan=2|0.612(17)&nbsp;s
| rowspan=2|620(5)&nbsp;ms
| β<sup>−</sup> (99.6%)
| β<sup>−</sup> (99.6%)
| <sup>148</sup>La
| <sup>148</sup>La
Line 522: Line 562:
| rowspan=2|
| rowspan=2|
|-
|-
| β<sup>−</sup>, n (.4%)
| β<sup>−</sup>, n (0.4%)
| <sup>147</sup>La
| <sup>147</sup>La
|-
|-
Line 528: Line 568:
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 93
| rowspan=2 style="text-align:right" | 93
| rowspan=2|148.94258(21)#
| rowspan=2|148.9432840(27)
| rowspan=2|344(7)&nbsp;ms
| rowspan=2|349(4)&nbsp;ms
| β<sup>−</sup> (99.57%)
| β<sup>−</sup> (96.1%)
| <sup>149</sup>La
| <sup>149</sup>La
| rowspan=2|3/2−#
| rowspan=2|3/2−#
Line 536: Line 576:
| rowspan=2|
| rowspan=2|
|-
|-
| β<sup>−</sup>, n (.43%)
| β<sup>−</sup>, n (3.9%)
| <sup>148</sup>La
| <sup>148</sup>La
|-
|-
Line 542: Line 582:
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 94
| rowspan=2 style="text-align:right" | 94
| rowspan=2|149.94568(43)#
| rowspan=2| 149.946441(6)
| rowspan=2|300&nbsp;ms
| rowspan=2|258(5)&nbsp;ms
| β<sup>−</sup>
| β<sup>−</sup> (99.0%)
| <sup>150</sup>La
| <sup>150</sup>La
| rowspan=2|0+
| rowspan=2|0+
Line 550: Line 590:
| rowspan=2|
| rowspan=2|
|-
|-
| β<sup>−</sup>, n (rare)
| β<sup>−</sup>, n (1.0%)
| <sup>149</sup>La
| <sup>149</sup>La
|-
|-
| <sup>151</sup>Ba
| rowspan=2|<sup>151</sup>Ba
| style="text-align:right" | 56
| rowspan=2 style="text-align:right" | 56
| style="text-align:right" | 95
| rowspan=2 style="text-align:right" | 95
| 150.95081(43)#
| rowspan=2|150.95176(43)#
| 200#&nbsp;ms [>300&nbsp;ns]
| rowspan=2|167(5)&nbsp;ms
| β<sup>−</sup>
| β<sup>−</sup>
| <sup>151</sup>La
| <sup>151</sup>La
| 3/2−#
| rowspan=2|3/2−#
| rowspan=2|
|
| rowspan=2|
|
|-
|-
| <sup>152</sup>Ba
| β<sup></sup>, n?
| <sup>150</sup>La
| style="text-align:right" | 56
|-
| style="text-align:right" | 96
| rowspan=2|<sup>152</sup>Ba
| 151.95427(54)#
| rowspan=2 style="text-align:right" | 56
| 100#&nbsp;ms
| rowspan=2 style="text-align:right" | 96
| rowspan=2|151.95533(43)#
| rowspan=2|139(8)&nbsp;ms
| β<sup>−</sup>
| β<sup>−</sup>
| <sup>152</sup>La
| <sup>152</sup>La
| 0+
| rowspan=2|0+
| rowspan=2|
|
| rowspan=2|
|
|-
|-
| <sup>153</sup>Ba
| β<sup></sup>, n?
| <sup>151</sup>La
| style="text-align:right" | 56
|-
| style="text-align:right" | 97
| rowspan=3|<sup>153</sup>Ba
| 152.95961(86)#
| rowspan=3 style="text-align:right" | 56
| 80#&nbsp;ms
| rowspan=3 style="text-align:right" | 97
| rowspan=3|152.96085(43)#
| rowspan=3|113(39)&nbsp;ms
| β<sup>−</sup>
| β<sup>−</sup>
| <sup>153</sup>La
| <sup>153</sup>La
| 5/2−#
| rowspan=3|5/2−#
| rowspan=3|
| rowspan=3|
|-
| β<sup>−</sup>, n?
| <sup>152</sup>La
|-
| β<sup>−</sup>, 2n?
| <sup>151</sup>La
|-
| <sup>154</sup>Ba
| style="text-align:right" | 56
| style="text-align:right" | 98
|153.96466(54)#
| 53(48)&nbsp;ms
| β<sup>−</sup>
| <sup>154</sup>La
| 0+
|
|
|
|
{{Isotopes table/footer}}
{{Isotopes table/footer}}

==See also==
{{Wikipedia-Books|Barium}}
{{-}}


== References ==
== References ==
{{Reflist}}
<references />
* Isotope masses from:
* Isotope masses from:
**{{NUBASE 2003}}
**{{NUBASE 2003}}
* Isotopic compositions and standard atomic masses from:
* Isotopic compositions and standard atomic masses from:
**{{CAWIA 2003}}
**{{CIAAW2003}}
**{{CIAAW 2005}}
**{{CIAAW 2005}}
* Half-life, spin, and isomer data selected from the following sources.
* Half-life, spin, and isomer data selected from the following sources.
Line 607: Line 666:


{{Navbox element isotopes}}
{{Navbox element isotopes}}
{{Authority control}}


[[Category:Barium]]
[[Category:Isotopes of barium| ]]
[[Category:Isotopes of barium| ]]
[[Category:Barium]]
[[Category:Lists of isotopes by element|Barium]]
[[Category:Lists of isotopes by element|Barium]]

Latest revision as of 00:58, 11 July 2024

Isotopes of barium (56Ba)
Main isotopes[1] Decay
abun­dance half-life (t1/2) mode pro­duct
130Ba 0.11% (0.5–2.7)×1021 y εε 130Xe
132Ba 0.1% stable
133Ba synth 10.51 y ε 133Cs
134Ba 2.42% stable
135Ba 6.59% stable
136Ba 7.85% stable
137Ba 11.2% stable
138Ba 71.7% stable
Standard atomic weight Ar°(Ba)

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.[4] 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

[edit]


Nuclide
[n 1]
Z N Isotopic mass (Da)[5]
[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 energy Normal proportion[1] Range of variation
114Ba 56 58 113.95072(11) 460(125) ms β+ (79%) 114Cs 0+
α (0.9%) 110Xe
β+, p (20%) 113Xe
CD (<.0034%) 102Sn, 12C
115Ba 56 59 114.94748(22)# 0.45(5) s β+ 115Cs 5/2+#
β+, p (>15%) 114Xe
116Ba 56 60 115.94162(22)# 1.3(2) s β+ (97%) 116Cs 0+
β+, p (3%) 115Xe
117Ba 56 61 116.93832(27) 1.75(7) s β+ (87%) 117Cs (3/2+)
β+, p (13%) 116Xe
β+, α (0.024%) 113I
118Ba 56 62 117.93323(22)# 5.2(2) s β+ 118Cs 0+
119Ba 56 63 118.93066(21) 5.4(3) s β+ (75%) 119Cs (5/2+)
β+, p (25%) 118Xe
120Ba 56 64 119.92604(32) 24(2) s β+ 120Cs 0+
121Ba 56 65 120.92405(15) 29.7(15) s β+ (99.98%) 121Cs 5/2+
β+, p (0.02%) 120Xe
122Ba 56 66 121.91990(3) 1.95(15) min β+ 122Cs 0+
123Ba 56 67 122.918781(13) 2.7(4) min β+ 123Cs 5/2+
123mBa 120.95(8) keV 830(60) ns IT 123Ba 1/2+#
124Ba 56 68 123.915094(13) 11.0(5) min β+ 124Cs 0+
125Ba 56 69 124.914472(12) 3.3(3) min β+ 125Cs 1/2+
125mBa 120(20)# keV 2.76(14) μs IT 125Ba (7/2−)
126Ba 56 70 125.911250(13) 100(2) min β+ 126Cs 0+
127Ba 56 71 126.911091(12) 12.7(4) min β+ 127Cs 1/2+
127mBa 80.32(11) keV 1.93(7) s IT 127Ba 7/2−
128Ba 56 72 127.9083524(17) 2.43(5) d EC 128Cs 0+
129Ba 56 73 128.908683(11) 2.23(11) h β+ 129Cs 1/2+
129mBa 8.42(6) keV 2.135(10) h β+ 129Cs 7/2+
IT 129Ba
130Ba[n 9] 56 74 129.9063260(3) ≈ 1×1021 y 2EC? 130Xe 0+ 0.0011(1)
130mBa 2475.12(18) keV 9.54(14) ms IT 130Ba 8−
131Ba 56 75 130.9069463(4) 11.52(1) d β+ 131Cs 1/2+
131mBa 187.995(9) keV 14.26(9) min IT 131Ba 9/2−
132Ba 56 76 131.9050612(11) Observationally Stable[n 10] 0+ 0.0010(1)
133Ba 56 77 132.9060074(11) 10.5379(16) y EC 133Cs 1/2+
133mBa 288.252(9) keV 38.90(6) h IT (99.99%) 133Ba 11/2−
EC (0.0104%) 133Cs
134Ba 56 78 133.90450825(27) Stable 0+ 0.0242(15)
134mBa 2957.2(5) keV 2.61(13) μs IT 134Ba 10+
135Ba 56 79 134.90568845(26) Stable 3/2+ 0.0659(10)
135m1Ba 268.218(20) keV 28.11(2) h IT 135Ba 11/2−
135m2Ba 2388.0(5) keV 1.06(4) ms IT 135Ba (23/2+)
136Ba 56 80 135.90457580(26) Stable 0+ 0.0785(24)
136m1Ba 2030.535(18) keV 308.4(19) ms IT 136Ba 7−
136m2Ba 3357.19(25) keV 91(2) ns IT 136Ba 10+
137Ba 56 81 136.90582721(27) Stable 3/2+ 0.1123(23)
137m1Ba 661.659(3) keV 2.552(1) min IT 137Ba 11/2−
137m2Ba 2349.1(5) keV 589(20) ns IT 137Ba (19/2−)
138Ba[n 11] 56 82 137.90524706(27) Stable 0+ 0.7170(29)
138mBa 2090.536(21) keV 850(100) ns IT 138Ba 6+
139Ba[n 11] 56 83 138.90884116(27) 82.93(9) min β 139La 7/2−
140Ba[n 11] 56 84 139.910608(8) 12.7534(21) d β 140La 0+
141Ba[n 11] 56 85 140.914404(6) 18.27(7) min β 141La 3/2−
142Ba[n 11] 56 86 141.916433(6) 10.6(2) min β 142La 0+
143Ba[n 11] 56 87 142.920625(7) 14.5(3) s β 143La 5/2−
144Ba[n 11] 56 88 143.922955(8) 11.73(8) s β 144La 0+
145Ba 56 89 144.927518(9) 4.31(16) s β 145La 5/2−
146Ba 56 90 145.9303632(19) 2.15(4) s β 146La 0+
147Ba 56 91 146.935304(21) 893(1) ms β (99.93%) 147La 5/2−
β, n (0.07%) 146La
148Ba 56 92 147.9382230(16) 620(5) ms β (99.6%) 148La 0+
β, n (0.4%) 147La
149Ba 56 93 148.9432840(27) 349(4) ms β (96.1%) 149La 3/2−#
β, n (3.9%) 148La
150Ba 56 94 149.946441(6) 258(5) ms β (99.0%) 150La 0+
β, n (1.0%) 149La
151Ba 56 95 150.95176(43)# 167(5) ms β 151La 3/2−#
β, n? 150La
152Ba 56 96 151.95533(43)# 139(8) ms β 152La 0+
β, n? 151La
153Ba 56 97 152.96085(43)# 113(39) ms β 153La 5/2−#
β, n? 152La
β, 2n? 151La
154Ba 56 98 153.96466(54)# 53(48) ms β 154La 0+
This table header & footer:
  1. ^ mBa – Excited nuclear 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:
    CD: Cluster decay
    EC: Electron capture
    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 radioisotope
  10. ^ Believed to undergo β+β+ decay to 132Xe with a half-life over 3×1020 years
  11. ^ a b c d e f g Fission product

References

[edit]
  1. ^ a b c d e Kondev, 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 of 130Ba and 132Ba: Geochemical measurements". Physical Review C. 64 (3): 035205–1–035205–6. Bibcode:2001PhRvC..64c5205M. doi:10.1103/PhysRevC.64.035205.
  5. ^ 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.