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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, recently identified as being unstable by geochemical means (from analysis of the presence of its daughter xenon-130 in rocks). 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, but most of these are highly [[radioactive]] with [[half-life|half-lives]] in the several millisecond to several minute range. The only notable exceptions are <sup>133</sup>Ba, which has a half-life of 10.51 years, <sup>131</sup>Ba (11.5 days), and <sup>137m</sup>Ba (2.55 minutes), which is the decay product of [[Caesium-137|<sup>137</sup>Cs]] (30.17 years, and a common [[fission product]]).
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%.


== List of isotopes ==
== List of isotopes ==
{{anchor|Barium-114|Barium-115|Barium-116|Barium-117|Barium-118|Barium-119|Barium-120|Barium-121|Barium-122|Barium-123|Barium-124|Barium-125|Barium-126|Barium-127|Barium-128|Barium-129|Barium-130|Barium-131|Barium-132|Barium-133|Barium-134|Barium-135|Barium-136|Barium-137|Barium-138|Barium-139|Barium-140|Barium-141|Barium-142|Barium-143|Barium-144|Barium-145|Barium-146|Barium-147|Barium-148|Barium-149|Barium-150|Barium-151|Barium-152|Barium-153}}
{| class="wikitable" style="font-size:95%; white-space:nowrap"

! rowspan="2" | nuclide<br />symbol
<!--Please delete anchor(s) from the list above if adding a dedicated isotope section(s).-->
! Z([[proton|p]])

! N([[neutron|n]])
{{Isotopes table
! &nbsp;<br />isotopic mass (u)<br />&nbsp;
|symbol=Ba
! rowspan="2" | half-life<ref group="n">Bold for isotopes with half-lives longer than the age of the universe (nearly stable)</ref>
|refs=NUBASE2020, AME2020 II
! rowspan="2" | decay<br>mode(s)<ref>{{cite web |url=http://www.nucleonica.net/unc.aspx |title=Universal Nuclide Chart |publisher=nucleonica |registration=yes}}</ref><ref group="n">Abbreviations:<br>CD: [[Cluster decay]]<br>EC: [[Electron capture]]<br>IT: [[Isomeric transition]]</ref>
|notes=m, unc(), mass#, spin(), spin#, daughter-st, daughter-nst, CD, EC, IT, n, p
! rowspan="2" | daughter<br>isotope(s)<ref group="n">Bold for stable isotopes, bold italics for nearly-stable isotopes (half-life longer than the [[age of the universe]])</ref>
}}
! rowspan="2" | nuclear<br />spin
! rowspan="2" | representative<br />isotopic<br />composition<br />(mole fraction)
! rowspan="2" | range of natural<br />variation<br />(mole fraction)
|-
! colspan="3" | excitation energy
|-
|-
| rowspan=4|<sup>114</sup>Ba
| rowspan=4|<sup>114</sup>Ba
| 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−
Line 217: Line 229:
| 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'''<ref group="n" name="SF">Theoretically capable of [[spontaneous fission]]</ref>
| 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'''<ref group="n" name="SF" />
| 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+)
|
|
|
|
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| 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'''<ref group="n" name="SF" />
| 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 368: 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'''<ref group="n" name="SF" />
| colspan=3 align=center|'''Stable'''
| 3/2+
| 3/2+
| 0.11232(24)
| 0.1123(23)
|
|
|-
|-
Line 384: 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−)
|
|
|
|
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| 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'''<ref group="n" name="SF" />
| 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 413: 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 424: 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 435: 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 446: 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 457: 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 468: 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 479: 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 487: 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 518: 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 526: 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 532: 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 540: 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 546: 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 554: 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}}
|}
<references group="n" />

=== Notes ===
* Geologically exceptional samples are known in which the isotopic composition lies outside the reported range. The uncertainty in the atomic mass may exceed the stated value for such specimens.
* Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
* Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use expanded uncertainties.

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


== References ==
== References ==
{{Reflist}}
<references />
* Isotope masses from:
* Isotope masses from:
**{{NUBASE 2003}}
**{{cite journal|author=G. Audi |author2=A. H. Wapstra |author3=C. Thibault |author4=J. Blachot |author5=O. Bersillon |year=2003 |title=The NUBASE evaluation of nuclear and decay properties |url=http://www.nndc.bnl.gov/amdc/nubase/Nubase2003.pdf |journal=[[Nuclear Physics A]] |volume=729 |issue= |pages=3–128 |doi=10.1016/j.nuclphysa.2003.11.001 |bibcode=2003NuPhA.729....3A |deadurl=yes |archiveurl=https://web.archive.org/web/20080923135135/http://www.nndc.bnl.gov/amdc/nubase/Nubase2003.pdf |archivedate=2008-09-23 |df= }}
* Isotopic compositions and standard atomic masses from:
* Isotopic compositions and standard atomic masses from:
**{{CIAAW2003}}
**{{cite journal |author=J. R. de Laeter |author2=J. K. Böhlke |author3=P. De Bièvre |author4=H. Hidaka |author5=H. S. Peiser |author6=K. J. R. Rosman |author7=P. D. P. Taylor |year=2003 |title=Atomic weights of the elements. Review 2000 (IUPAC Technical Report) |url=http://www.iupac.org/publications/pac/75/6/0683/pdf/ |journal=[[Pure and Applied Chemistry]] |volume=75 |issue=6 |pages=683–800 |doi=10.1351/pac200375060683}}
**{{CIAAW 2005}}
**{{cite journal |author=M. E. Wieser |year=2006 |title=Atomic weights of the elements 2005 (IUPAC Technical Report) |url=http://iupac.org/publications/pac/78/11/2051/pdf/ |journal=[[Pure and Applied Chemistry]] |volume=78 |issue=11 |pages=2051–2066 |doi=10.1351/pac200678112051 |laysummary=http://old.iupac.org/news/archives/2005/atomic-weights_revised05.html}}
* Half-life, spin, and isomer data selected from the following sources. See editing notes on [[Talk:Isotopes of barium|this article's talk page]].
* Half-life, spin, and isomer data selected from the following sources.
**{{NUBASE 2003}}
**{{cite journal|author=G. Audi |author2=A. H. Wapstra |author3=C. Thibault |author4=J. Blachot |author5=O. Bersillon |year=2003 |title=The NUBASE evaluation of nuclear and decay properties |url=http://www.nndc.bnl.gov/amdc/nubase/Nubase2003.pdf |journal=[[Nuclear Physics A]] |volume=729 |issue= |pages=3–128 |doi=10.1016/j.nuclphysa.2003.11.001 |bibcode=2003NuPhA.729....3A |deadurl=yes |archiveurl=https://web.archive.org/web/20080923135135/http://www.nndc.bnl.gov/amdc/nubase/Nubase2003.pdf |archivedate=2008-09-23 |df= }}
**{{NNDC}}
**{{cite web |author=[[National Nuclear Data Center]] |year= |title=NuDat 2.1 database |url=http://www.nndc.bnl.gov/nudat2/ |publisher=[[Brookhaven National Laboratory]] |accessdate=September 2005}}
**{{CRC85|chapter=11}}
**{{cite book |author=N. E. Holden |year=2004 |editor=D. R. Lide |chapter=Table of the Isotopes |title=[[CRC Handbook of Chemistry and Physics]] |page=Section 11 |nopp=yes |edition=85th |publisher=[[CRC Press]] |isbn=978-0-8493-0485-9}}
* Half-life of <sup>130</sup>Ba from:
* Half-life of <sup>130</sup>Ba from:
**{{cite journal |author=A. P. Meshik |author2=C. M. Hohenberg |author3=O. V. Pravdivtseva |author4=Ya. S. Kapusta |year=2001 |title=Weak decay of <sup>130</sup>Ba and <sup>132</sup>Ba: Geochemical measurements |url=http://prc.aps.org/abstract/PRC/v64/i3/e035205 |journal=[[Physical Review C]] |volume=64 |issue=3 |pages=035205 [6 pages] |doi=10.1103/PhysRevC.64.035205|bibcode = 2001PhRvC..64c5205M }}
**{{cite journal |author=A. P. Meshik |author2=C. M. Hohenberg |author3=O. V. Pravdivtseva |author4=Ya. S. Kapusta |year=2001 |title=Weak decay of <sup>130</sup>Ba and <sup>132</sup>Ba: Geochemical measurements |journal=[[Physical Review C]] |volume=64 |issue=3 |pages=035205 [6 pages] |doi=10.1103/PhysRevC.64.035205|bibcode = 2001PhRvC..64c5205M |url=https://zenodo.org/record/1063702 }}
**{{cite journal |author=M. Pujol |author2=B. Marty |author3=P. Burnard |author4=P. Philippot |year=2009|title=Xenon in Archean barite: Weak decay of <sup>130</sup>Ba, mass-dependent isotopic fractionation and implication for barite formation |url=http://www.sciencedirect.com/science/article/pii/S0016703709005055 |journal=[[Geochimica et Cosmochimica Acta]] |volume=73|issue=22 |pages=6834–6846 |doi=10.1016/j.gca.2009.08.002|bibcode = 2009GeCoA..73.6834P }}
**{{cite journal |author=M. Pujol |author2=B. Marty |author3=P. Burnard |author4=P. Philippot |year=2009|title=Xenon in Archean barite: Weak decay of <sup>130</sup>Ba, mass-dependent isotopic fractionation and implication for barite formation |journal=[[Geochimica et Cosmochimica Acta]] |volume=73|issue=22 |pages=6834–6846 |doi=10.1016/j.gca.2009.08.002|bibcode = 2009GeCoA..73.6834P }}


{{Navbox element isotopes}}
{{Isotope nav | element=barium | lighter=Isotopes of caesium | heavier=Isotopes of lanthanum }}
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[[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.