Isotopes of palladium: Difference between revisions

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{{Short description|none}}
{{infobox palladium isotopes}}
{{Infobox palladium isotopes}}
Naturally occurring [[palladium]] (<sub>46</sub>Pd) is composed of six stable [[isotope]]s, <sup>102</sup>Pd, <sup>104</sup>Pd, <sup>105</sup>Pd, <sup>106</sup>Pd, <sup>108</sup>Pd, and <sup>110</sup>Pd, although <sup>102</sup>Pd and <sup>110</sup>Pd are theoretically unstable. The most stable [[radioisotope]]s are [[Pd-107|<sup>107</sup>Pd]] with a [[half-life]] of 6.5 million years, [[Pd-103|<sup>103</sup>Pd]] with a half-life of 17 days, and <sup>100</sup>Pd with a half-life of 3.63 days. Twenty-three other radioisotopes have been characterized with [[atomic weight]]s ranging from 90.949 [[atomic mass unit|u]] (<sup>91</sup>Pd) to 128.96 u (<sup>129</sup>Pd). Most of these have half-lives that are less than a half an hour except <sup>101</sup>Pd (half-life: 8.47 hours), <sup>109</sup>Pd (half-life: 13.7 hours), and <sup>112</sup>Pd (half-life: 21 hours).
Natural [[palladium]] ({{sub|46}}Pd) is composed of six stable [[isotope]]s, {{sup|102}}Pd, {{sup|104}}Pd, {{sup|105}}Pd, {{sup|106}}Pd, {{sup|108}}Pd, and {{sup|110}}Pd, although {{sup|102}}Pd and {{sup|110}}Pd are theoretically unstable. The most stable [[radioisotope]]s are [[Pd-107|{{sup|107}}Pd]] with a [[half-life]] of 6.5 million years, [[Pd-103|{{sup|103}}Pd]] with a half-life of 17 days, and {{sup|100}}Pd with a half-life of 3.63 days. Twenty-three other radioisotopes have been characterized with [[atomic weight]]s ranging from 90.949 [[atomic mass unit|u]] ({{sup|91}}Pd) to 128.96 u ({{sup|129}}Pd). Most of these have half-lives that are less than 30 minutes except {{sup|101}}Pd (half-life: 8.47 hours), {{sup|109}}Pd (half-life: 13.7 hours), and {{sup|112}}Pd (half-life: 21 hours).
 
The primary [[decay mode]] before the most abundant stable isotope, <{{sup>|106</sup>}}Pd, is [[electron capture]] and the primary mode after is [[beta decay]]. The primary [[decay product]] before <{{sup>|106</sup>}}Pd is [[rhodium]] and the primary product after is [[silver]].
 
[[Radiogenic]] <{{sup>|107</sup>}}Ag is a decay product of <{{sup>|107</sup>}}Pd and was first discovered in the [[Santa Clara, Durango|Santa Clara]] meteorite of 1978.<ref>{{cite journal
| author= W. R. Kelly |author2=G. J. Wasserburg
| year = 1978
Line 12 ⟶ 13:
| doi =10.1029/GL005i012p01079
| bibcode=1978GeoRL...5.1079K
|url=https://authors.library.caltech.edu/43037/
}}</ref> The discoverers suggest that the coalescence and differentiation of iron-cored small planets may have occurred 10 million years after a [[nucleosynthetic]] event. <sup>107</sup>Pd versus Ag correlations observed in bodies, which have clearly been melted since accretion of the [[solar system]], must reflect the presence of short-lived nuclides in the early solar system.<ref>
}}</ref> The discoverers suggest that the coalescence and differentiation of iron-cored small planets may have occurred 10 million years after a [[nucleosynthetic]] event. {{sup|107}}Pd versus Ag correlations observed in bodies, which have clearly been melted since accretion of the [[Solar System]], must reflect the presence of short-lived nuclides in the early Solar System.<ref>
{{cite journal
| author= J. H. Chen |author2=G. J. Wasserburg
Line 24 ⟶ 26:
== List of isotopes ==
{{Isotopes table
|symbol=PaPd
|refs=NUBASE2020, AME2020 II
|refs=<!-- not NUBASE2016 yet (2019-07-14) -->
|notes=m, unc(), mass#, exen#, hl#, spin(), spin#, daughter-st, IT, EC, p
}}
|-id=Palladium-90
| rowspan=3|<sup>90</sup>Pd
| rowspan=3 style="text-align:right" | 46
| rowspan=3 style="text-align:right" | 44
| rowspan=3|89.95737(43)#
| rowspan=3|10#&nbsp;ms<br>[>400&nbsp;ns]
| [[beta decay|β<sup>+</sup>]]?
| <sup>90</sup>Rh
| rowspan=3|0+
| rowspan=3|
| rowspan=3|
|-
| β<sup>91+</sup>Pd, [[proton emission|p]]?
| <sup>89</sup>Ru
| style="text-align:right" | 46
|-
| style="text-align:right" | 45
| 2p?
| 90.94911(61)#
| <sup>88</sup>Ru
| 10#&nbsp;ms [>1.5&nbsp;µs]
|-id=Palladium-91
| [[beta decay|β<sup>+</sup>]]
| rowspan=2|<sup>91</sup>Pd
| rowspan=2 style="text-align:right" | 46
| rowspan=2 style="text-align:right" | 45
| rowspan=2|90.95044(45)#
| rowspan=2|32(3)&nbsp;ms
| β<sup>+</sup> (96.9%)
| <sup>91</sup>Rh
| rowspan=2|7/2+#
| rowspan=2|
|
| rowspan=2|
|
|-
| β<sup>92+</sup>Pd, p (3.1%)
| <sup>90</sup>Ru
| style="text-align:right" | 46
|-id=Palladium-92
| style="text-align:right" | 46
| rowspan=2|<sup>92</sup>Pd
| 91.94042(54)#
| rowspan=2 style="text-align:right" | 46
| 1.1(3)&nbsp;s [0.7(+4−2)&nbsp;s]
| rowspan=2 style="text-align:right" | 46
| β<sup>+</sup>
| rowspan=2|91.94119(37)
| rowspan=2|1.06(3)&nbsp;s
| β<sup>+</sup> (98.4%)
| <sup>92</sup>Rh
| rowspan=2|0+
| rowspan=2|
|
| rowspan=2|
|
|-
| β<sup>93+</sup>Pd, p (1.6%)
| <sup>91</sup>Ru
| style="text-align:right" | 46
|-id=Palladium-93
| style="text-align:right" | 47
| rowspan=2|<sup>93</sup>Pd
| 92.93591(43)#
| rowspan=2 style="text-align:right" | 46
| 1.07(12)&nbsp;s
| rowspan=2 style="text-align:right" | 47
| β<sup>+</sup>
| rowspan=2|92.93668(40)
| rowspan=2|1.17(2)&nbsp;s
| β<sup>+</sup> (92.6%)
| <sup>93</sup>Rh
| rowspan=2|(9/2+)
| rowspan=2|
|
| rowspan=2|
|
|-
| style="text-indent:1em" | β<sup>93m+</sup>Pd, p (7.4%)
| <sup>91</sup>Ru
| colspan="3" style="text-indent:2em" | 0+X&nbsp;keV
|-id=Palladium-94
| 9.3(+25−17)&nbsp;s
| rowspan=2|<sup>94</sup>Pd
|
| rowspan=2 style="text-align:right" | 46
|
| rowspan=2 style="text-align:right" | 48
|
| rowspan=2|93.9290363(46)
|
| rowspan=2|9.1(3)&nbsp;s
|
| β<sup>+</sup> (>99.87%)
| <sup>94</sup>Rh
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| β<sup>+</sup>, p (<0.13%)
| <sup>93</sup>Ru
|-id=Palladium-94m1
| style="text-indent:1em" | <sup>94m1</sup>Pd
| colspan="3" style="text-indent:2em" | 4883.1(4)&nbsp;keV
| 515(1)&nbsp;ns
| [[isomeric transition|IT]]
| <sup>94</sup>Pd
| (14+)
| style="text-align:right" | 46
| style="text-align:right" | 48
| 93.92877(43)#
| 9.0(5)&nbsp;s
| β<sup>+</sup>
| <sup>94</sup>Rh
| 0+
|
|
|-id=Palladium-94m2
|-
| style="text-indent:1em" | <sup>94m94m2</sup>Pd
| colspan="3" style="text-indent:2em" | 48847209.48(58)&nbsp;keV
| 530206(1018)&nbsp;ns
| IT
| <sup>94</sup>Pd
|
| (14+19−)
|
|
|-id=Palladium-95
| rowspan=2|<sup>95</sup>Pd
| rowspan=2 style="text-align:right" | 46
| rowspan=2 style="text-align:right" | 49
| rowspan=2|94.9248885(33)
| rowspan=2|7.4(4)&nbsp;s
| β<sup>+</sup> (99.77%)
| <sup>95</sup>Rh
| rowspan=2|9/2+#
| rowspan=2|
| rowspan=2|
|-
| β<sup>95+</sup>Pd, p (0.23%)
| style="text-align:right" | 46
| style="text-align:right" | 49
| 94.92469(43)#
| 10# s
| β<sup>+</sup>
| <sup>95</sup>Rh
|-id=Palladium-95m
| 9/2+#
|
|
|-
| rowspan=3 style="text-indent:1em" | <sup>95m</sup>Pd
| rowspan=3 colspan="3" style="text-indent:2em" | 18601875.13(50014)#&nbsp;keV
| rowspan=3|13.3(32)&nbsp;s
| β<sup>+</sup> (94.188%)
| <sup>95</sup>Rh
| rowspan=3|(21/2+)
Line 111 ⟶ 145:
| rowspan=3|
|-
| [[Isomeric transition|IT]] (511%)
| <sup>95</sup>Pd
|-
| β<sup>+</sup>, [[proton emission|p]] (0.971%)
| <sup>94</sup>Ru
|-id=Palladium-96
|-
| <sup>96</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 50
| 95.918169182137(1645)
| 122(2)&nbsp;s
| β<sup>+</sup>
Line 127 ⟶ 161:
|
|
|-id=Palladium-96m
|-
| style="text-indent:1em" | <sup>96m</sup>Pd
| colspan="3" style="text-indent:2em" | 2530.857(123)&nbsp;keV
| 1.81804(17)&nbsp;µsμs
| IT
| <sup>96</sup>Pd
| 8+#
|
|
|-id=Palladium-97
| 8+
|
|
|-
| <sup>97</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 51
| 96.916489164720(3252)
| 3.10(9)&nbsp;min
| β<sup>+</sup>
Line 147 ⟶ 181:
|
|
|-id=Palladium-98
|-
| <sup>98</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 52
| 97.9127219126983(2351)
| 17.7(34)&nbsp;min
| β<sup>+</sup>
| <sup>98</sup>Rh
Line 158 ⟶ 192:
|
|
|-id=Palladium-99
|-
| <sup>99</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 53
| 98.9117689117731(1655)
| 21.4(2)&nbsp;min
| β<sup>+</sup>
Line 169 ⟶ 203:
|
|
|-id=Palladium-100
|-
| <sup>100</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 54
| 99.908506908520(1219)
| 3.63(9)&nbsp;d
| [[Electron capture|EC]]
Line 180 ⟶ 214:
|
|
|-id=Palladium-101
|-
| <sup>101</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 55
| 100.9082899082848(1949)
| 8.47(6)&nbsp;h
| β<sup>+</sup>
Line 191 ⟶ 225:
|
|
|-id=Palladium-102
|-
| <sup>102</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 56
| 101.90560990563229(345)
| colspan=3 align=center|'''[[Observationally Stable]]'''<ref group="n">Believed to decay by β<sup>+</sup>β<sup>+</sup> to '''<sup>102</sup>Ru''' with a half-life over 7.6×10<sup>18</sup>&nbsp;y</ref>
| 0+
| 0.0102(1)
|
|-
| <sup>103</sup>Pd<ref group="n">Used in medicine</ref>
| style="text-align:right" | 46
| style="text-align:right" | 57
| 102.90608790611107(394)
| 16.991(19)&nbsp;d
| EC
Line 211 ⟶ 245:
|
|
|-id=Palladium-104
|-
| style="text-indent:1em" | <sup>103m</sup>Pd
| colspan="3" style="text-indent:2em" | 784.79(10)&nbsp;keV
| 25(2)&nbsp;ns
|
|
| 11/2−
|
|
|-
| <sup>104</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 58
| 103.9040369040304(414)
| colspan=3 align=center|'''Stable'''<ref group="n" name="SF">Theoretically capable of [[spontaneous fission]]</ref>
| 0+
| 0.1114(8)
|
|-id=Palladium-105
|-
| <sup>105</sup>Pd<ref group="n" name="FP">[[Fission product]]</ref>
| style="text-align:right" | 46
| style="text-align:right" | 59
| 104.9050859050795(412)
| colspan=3 align=center|'''Stable'''<ref group="n" name="SF"/>
| 5/2+
| 0.2233(8)
|
|-id=Palladium-105m
|-
| style="text-indent:1em" | <sup>105m</sup>Pd
| colspan="3" style="text-indent:2em" | 489.1(3)&nbsp;keV
| 35.5(5)&nbsp;μs
| IT
| '''<sup>105</sup>Pd'''
| 11/2−
|
|
|-id=Palladium-106
| <sup>106</sup>Pd<ref group="n" name="FP" />
| style="text-align:right" | 46
| style="text-align:right" | 60
| 105.9034869034803(412)
| colspan=3 align=center|'''Stable'''<ref group="n" name="SF"/>
| 0+
| 0.2733(3)
Line 251 ⟶ 285:
| style="text-align:right" | 46
| style="text-align:right" | 61
| 106.9051339051281(413)
| 6.5(3)×10<sup>6</sup> y
| β<sup>−</sup>
Line 258 ⟶ 292:
| trace<ref group="n">[[Cosmogenic]] nuclide, also found as nuclear contamination</ref>
|
|-id=Palladium-107m1
|-
| style="text-indent:1em" | <sup>107m1</sup>Pd
| colspan="3" style="text-indent:2em" | 115.74(12)&nbsp;keV
| 0.85(10)&nbsp;µsμs
| IT
| <sup>107</sup>Pd
|
| 1/2+
|
|
|-id=Palladium-107m2
|-
| style="text-indent:1em" | <sup>107m2</sup>Pd
| colspan="3" style="text-indent:2em" | 214.6(3)&nbsp;keV
Line 276 ⟶ 310:
|
|
|-id=Palladium-108
|-
| <sup>108</sup>Pd<ref group="n" name="FP" />
| style="text-align:right" | 46
| style="text-align:right" | 62
| 107.9038929038918(412)
| colspan=3 align=center|'''Stable'''<ref group="n" name="SF"/>
| 0+
| 0.2646(9)
|
|-id=Palladium-109
|-
| <sup>109</sup>Pd<ref group="n" name="FP" />
| style="text-align:right" | 46
| style="text-align:right" | 63
| 108.9059509059506(412)
| 13.701259(2412)&nbsp;h
| β<sup>−</sup>
| '''<sup>109m109</sup>Ag'''
| 5/2+
|
|
|-id=Palladium-109m1
|-
| style="text-indent:1em" | <sup>109m1</sup>Pd
| colspan="3" style="text-indent:2em" | 113.4004000(1014)&nbsp;keV
| 380(50)&nbsp;ns
| IT
| <sup>109</sup>Pd
|
| 1/2+
|
|
|-id=Palladium-109m2
|-
| style="text-indent:1em" | <sup>109m2</sup>Pd
| colspan="3" style="text-indent:2em" | 188.9909903(10)&nbsp;keV
| 4.696703(39)&nbsp;min
| IT
| <sup>109</sup>Pd
Line 314 ⟶ 348:
|
|
|-id=Palladium-110
|-
| <sup>110</sup>Pd<ref group="n" name="FP" />
| style="text-align:right" | 46
| style="text-align:right" | 64
| 109.90515390517288(1266)
| colspan=3 align=center|'''Observationally Stable'''<ref group="n">Believed to decay by β<sup>−</sup>β<sup>−</sup> to '''<sup>110</sup>Cd''' with a [[half-life]] over 6×102.9×10<sup>1720</sup> years</ref>
| 0+
| 0.1172(9)
|
|-id=Palladium-111
|-
| <sup>111</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 65
| 110.90767190769036(1279)
| 23.456(29)&nbsp;min
| β<sup>−</sup>
| <sup>111m111</sup>Ag
| 5/2+
|
|
|-id=Palladium-111m
|-
| rowspan=2 style="text-indent:1em" | <sup>111m</sup>Pd
| rowspan=2 colspan="3" style="text-indent:2em" | 172.18(8)&nbsp;keV
| rowspan=2|5.5563(113)&nbsp;h
| IT (76.8%)
| <sup>111</sup>Pd
| rowspan=2|11/2−
Line 344 ⟶ 378:
| rowspan=2|
|-
| β<sup>−</sup> (23.2%)
| <sup>111m111</sup>Ag
|-id=Palladium-112
|-
| <sup>112</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 66
| 111.9073149073306(1970)
| 21.0304(517)&nbsp;h
| β<sup>−</sup>
| <sup>112</sup>Ag
Line 357 ⟶ 391:
|
|
|-id=Palladium-113
|-
| <sup>113</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 67
| 112.910159102619(475)
| 93(5)&nbsp;s
| β<sup>−</sup>
| <sup>113m113</sup>Ag
| (5/2+)
|
|
|-id=Palladium-113m
|-
| style="text-indent:1em" | <sup>113m</sup>Pd
| colspan="3" style="text-indent:2em" | 81.1(3)&nbsp;keV
Line 377 ⟶ 411:
|
|
|-id=Palladium-114
|-
| <sup>114</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 68
| 113.9103639103694(2575)
| 2.42(6)&nbsp;min
| β<sup>−</sup>
Line 388 ⟶ 422:
|
|
|-id=Palladium-115
|-
| <sup>115</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 69
| 114.9136650(19)<ref name="jaries2024">{{cite journal |last1=Jaries |first1=A. |last2=Stryjczyk |first2=M. |last3=Kankainen |first3=A. |last4=Ayoubi |first4=L. Al |last5=Beliuskina |first5=O. |last6=Canete |first6=L. |last7=de Groote |first7=R. P. |last8=Delafosse |first8=C. |last9=Delahaye |first9=P. |last10=Eronen |first10=T. |last11=Flayol |first11=M. |last12=Ge |first12=Z. |last13=Geldhof |first13=S. |last14=Gins |first14=W. |last15=Hukkanen |first15=M. |last16=Imgram |first16=P. |last17=Kahl |first17=D. |last18=Kostensalo |first18=J. |last19=Kujanpää |first19=S. |last20=Kumar |first20=D. |last21=Moore |first21=I. D. |last22=Mougeot |first22=M. |last23=Nesterenko |first23=D. A. |last24=Nikas |first24=S. |last25=Patel |first25=D. |last26=Penttilä |first26=H. |last27=Pitman-Weymouth |first27=D. |last28=Pohjalainen |first28=I. |last29=Raggio |first29=A. |last30=Ramalho |first30=M. |last31=Reponen |first31=M. |last32=Rinta-Antila |first32=S. |last33=de Roubin |first33=A. |last34=Ruotsalainen |first34=J. |last35=Srivastava |first35=P. C. |last36=Suhonen |first36=J. |last37=Vilen |first37=M. |last38=Virtanen |first38=V. |last39=Zadvornaya |first39=A. |title=Physical Review C - Accepted Paper: Isomeric states of fission fragments explored via Penning trap mass spectrometry at IGISOL |journal=journals.aps.org |url=https://journals.aps.org/prc/accepted/fe077P3cDac1f601a8c16c34b19fb124fc3509f19 |arxiv=2403.04710}}</ref>
| 114.91368(7)
| 25(2)&nbsp;s
| β<sup>−</sup>
| <sup>115m115</sup>Ag
| (51/2+)#+
|
|
|-id=Palladium-115m
|-
| rowspan=2 style="text-indent:1em" | <sup>115m</sup>Pd
| rowspan=2 colspan="3" style="text-indent:2em" | 8986.188(2529)&nbsp;keV<ref name="jaries2024"/>
| rowspan=2|50(3)&nbsp;s
| β<sup>−</sup> (92.0%)
| <sup>115</sup>Ag
| rowspan=2|(117/2−)#
| rowspan=2|
| rowspan=2|
|-
| IT (8.0%)
| <sup>115</sup>Pd
|-id=Palladium-116
|-
| <sup>116</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 70
| 115.914169142979(677)
| 11.8(4)&nbsp;s
| β<sup>−</sup>
Line 422 ⟶ 456:
|
|
|-id=Palladium-117
|-
| <sup>117</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 71
| 116.917849179556(678)
| 4.3(3)&nbsp;s
| β<sup>−</sup>
| <sup>117m117</sup>Ag
| (53/2+)
|
|
|-id=Palladium-117m
|-
| style="text-indent:1em" | <sup>117m</sup>Pd
| colspan="3" style="text-indent:2em" | 203.23(3)&nbsp;keV
| 19.1(7)&nbsp;ms
| IT
| <sup>117</sup>Pd
| (119/2−)#
|
|
|-id=Palladium-118
|-
| <sup>118</sup>Pd
| style="text-align:right" | 46
| style="text-align:right" | 72
| 117.918989190673(2327)
| 1.9(1)&nbsp;s
| β<sup>−</sup>
Line 453 ⟶ 487:
|
|
|-id=Palladium-119
|-
| rowspan=2|<sup>119</sup>Pd
| rowspan=2 style="text-align:right" | 46
| rowspan=2 style="text-align:right" | 73
| rowspan=2|118.9231238(45)<ref name="jaries2024"/>
| 118.92311(32)#
| rowspan=2|0.9288(132)&nbsp;s
| β<sup>−</sup>
| <sup>119</sup>Ag
| rowspan=2|1/2+, 3/2+<ref name="kurpeta2022">{{cite journal |last1=Kurpeta |first1=J. |last2=Abramuk |first2=A. |last3=Rząca-Urban |first3=T. |last4=Urban |first4=W. |last5=Canete |first5=L. |last6=Eronen |first6=T. |last7=Geldhof |first7=S. |last8=Gierlik |first8=M. |last9=Greene |first9=J. P. |last10=Jokinen |first10=A. |last11=Kankainen |first11=A. |last12=Moore |first12=I. D. |last13=Nesterenko |first13=D. A. |last14=Penttilä |first14=H. |last15=Pohjalainen |first15=I. |last16=Reponen |first16=M. |last17=Rinta-Antila |first17=S. |last18=de Roubin |first18=A. |last19=Simpson |first19=G. S. |last20=Smith |first20=A. G. |last21=Vilén |first21=M. |title=β - and γ -spectroscopy study of Pd 119 and Ag 119 |journal=Physical Review C |date=14 March 2022 |volume=105 |issue=3 |doi=10.1103/PhysRevC.105.034316}}</ref>
| rowspan=2|
| rowspan=2|
|-
| β<sup>−</sup>, n?
| <sup>118</sup>Ag
|-id=Palladium-119m
| style="text-indent:1em" | <sup>119m</sup>Pd<ref name="jaries2024"/>
| colspan="3" style="text-indent:2em" | 199.1(30)&nbsp;keV
| 0.85(1)&nbsp;s
| IT
| <sup>119</sup>Pd
| (11/2−)<ref name="kurpeta2022"/>
|
|
|-id=Palladium-120
|
| rowspan=2|<sup>120</sup>Pd
| rowspan=2 style="text-align:right" | 46
| rowspan=2 style="text-align:right" | 74
| rowspan=2|119.9245517(25)
| rowspan=2|492(33)&nbsp;ms
| β<sup>−</sup> (>99.3%)
| <sup>120</sup>Ag
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| β<sup>120</sup>Pd, n (<0.7%)
| <sup>119</sup>Ag
| style="text-align:right" | 46
|-id=Palladium-121
| style="text-align:right" | 74
| rowspan=2|<sup>121</sup>Pd
| 119.92469(13)
| rowspan=2 style="text-align:right" | 46
| 0.5(1)&nbsp;s
| rowspan=2 style="text-align:right" | 75
| β<sup>−</sup>
| rowspan=2|120.9289513(40)<ref name="jaries2024"/>
| rowspan=2|290(1)&nbsp;ms
| β<sup>−</sup> (>99.2%)
| <sup>121</sup>Ag
| rowspan=2|3/2+#
| rowspan=2|
| rowspan=2|
|-
| β<sup>−</sup>, n (<0.8%)
| <sup>120</sup>Ag
|-id=Palladium-121m1
| 0+
| style="text-indent:1em" | <sup>121m1</sup>Pd
| colspan="3" style="text-indent:2em" | 135.5(5)&nbsp;keV
| 460(90)&nbsp;ns
| IT
| <sup>121</sup>Pd
| 7/2+#
|
|
|-id=Palladium-121m2
|-
| style="text-indent:1em" | <sup>121m2</sup>Pd
| colspan="3" style="text-indent:2em" | 160(14)&nbsp;keV
| 460(90)&nbsp;ns
| IT
| <sup>121</sup>Pd
| 11/2−#
| style="text-align:right" | 46
| style="text-align:right" | 75
| 120.92887(54)#
| 285&nbsp;ms
| β<sup>−</sup>
| <sup>121</sup>Ag
|
|
|-id=Palladium-122
|
| rowspan=2|<sup>122</sup>Pd
|-
| rowspan=2 style="text-align:right" | 46
| <sup>122</sup>Pd
| rowspan=2 style="text-align:right" | 4676
| rowspan=2|121.930632(21)
| style="text-align:right" | 76
| rowspan=2|193(5)&nbsp;ms
| 121.93055(43)#
| 175&nbsp;ms [>300&nbsp;ns]
| β<sup>−</sup>
| <sup>122</sup>Ag
| rowspan=2|0+
| rowspan=2|
|
| rowspan=2|
|
|-
| β<sup>123</sup>Pd, n (<2.5%)
| <sup>121</sup>Ag
| style="text-align:right" | 46
|-id=Palladium-123
| style="text-align:right" | 77
| rowspan=2|<sup>123</sup>Pd
| 122.93493(64)#
| rowspan=2 style="text-align:right" | 46
| 108&nbsp;ms
| rowspan=2 style="text-align:right" | 77
| rowspan=2|122.93513(85)
| rowspan=2|108(1)&nbsp;ms
| β<sup>−</sup> (90%)
| <sup>123</sup>Ag
| rowspan=2|3/2+#
| rowspan=2|
| rowspan=2|
|-
| β<sup>−</sup>, n (10%)
| <sup>122</sup>Ag
|-id=Palladium-123m
| rowspan=2 style="text-indent:1em" | <sup>123m</sup>Pd
| rowspan=2 colspan="3" style="text-indent:2em" | 100(50)#&nbsp;keV
| rowspan=2|100#&nbsp;ms
| β<sup>−</sup>
| <sup>123</sup>Ag
| rowspan=2|11/2−#
|
| rowspan=2|
|
| rowspan=2|
|
|-
| IT?
| <sup>123</sup>Pd
|-id=Palladium-124
| rowspan=2|<sup>124</sup>Pd
| rowspan=2 style="text-align:right" | 46
| rowspan=2 style="text-align:right" | 78
| rowspan=2|123.93731(32)#
| rowspan=2|88(15)&nbsp;ms
| β<sup>−</sup> (83%)
| <sup>124</sup>Ag
| rowspan=2|0+
| rowspan=2|
| rowspan=2|
|-
| β<sup>−</sup>, n (17%)
| <sup>123</sup>Ag
|-id=Palladium-124m
| style="text-indent:1em" | <sup>124m</sup>Pd
| colspan="3" style="text-indent:2em" | 1000(800)#&nbsp;keV
| >20&nbsp;μs
| IT
| <sup>124</sup>Pd
| 11/2−#
| style="text-align:right" | 46
| style="text-align:right" | 78
| 123.93688(54)#
| 38&nbsp;ms
| β<sup>−</sup>
| <sup>124</sup>Ag
| 0+
|
|
|-id=Palladium-125
| rowspan=2|<sup>125</sup>Pd
| rowspan=2 style="text-align:right" | 46
| rowspan=2 style="text-align:right" | 79
| rowspan=2|124.94207(43)#
| rowspan=2|60(6)&nbsp;ms
| β<sup>−</sup> (88%)
| <sup>125</sup>Ag
| rowspan=2|3/2+#
| rowspan=2|
| rowspan=2|
|-
| β<sup>−</sup>, n (12%)
| <sup>125</sup>Pd<ref>[http://www-win.gsi.de/tasca07/contributions/TASCA07_Contribution_Morita.pdf Future Plan of the Experimental Program on Synthesizing the Heaviest Element at RIKEN], Kosuke Morita {{webarchive |url=https://web.archive.org/web/20120917003601/http://www-win.gsi.de/tasca07/contributions/TASCA07_Contribution_Morita.pdf |date=September 17, 2012 }}</ref>
| <sup>124</sup>Ag
| style="text-align:right" | 46
|-id=Palladium-125m1
| style="text-align:right" | 79
| rowspan=2 style="text-indent:1em" | <sup>125m1</sup>Pd
|
| rowspan=2 colspan="3" style="text-indent:2em" | 100(50)#&nbsp;keV
| 57&nbsp;ms
| rowspan=2|50#&nbsp;ms
| β<sup>−</sup>
| <sup>125</sup>Ag
| rowspan=2|11/2−#
| rowspan=2|
| rowspan=2|
|-
| IT?
| <sup>125</sup>Pd
|-id=Palladium-125m2
| style="text-indent:1em" | <sup>125m2</sup>Pd
| colspan="3" style="text-indent:2em" | 1805.23(18)&nbsp;keV
| 144(4)&nbsp;ns
| IT
| <sup>125</sup>Pd
| (23/2+)
|
|
|-id=Palladium-126
|
| rowspan=2|<sup>126</sup>Pd
|-
| rowspan=2 style="text-align:right" | 46
| <sup>126</sup>Pd<ref name="NM126A">{{cite journal |author=H. Watanabe |display-authors=et al. |title=Isomers in <sup>128</sup>Pd and <sup>126</sup>Pd: Evidence for a Robust Shell Closure at the Neutron Magic Number 82 in Exotic Palladium Isotopes |journal=Physical Review Letters |date=2013-10-08 |volume=111 |issue=15 |page=152501 |doi=10.1103/PhysRevLett.111.152501|bibcode=2013PhRvL.111o2501W |hdl=2437/215438 |url=https://openresearch-repository.anu.edu.au/bitstream/1885/75174/2/01_Watanabe_Isomers_in_Pd128_and_Pd126%3a_2013.pdf |hdl-access=free }}</ref><ref name="NM126B">{{cite web |url=http://phys.org/news/2013-11-neutron-rich-atomic-nuclei-scientists-nuclear.html |title=Experiments on neutron-rich atomic nuclei could help scientists to understand nuclear reactions in exploding stars |publisher=phys.org |date=2013-11-29}}</ref>
| rowspan=2 style="text-align:right" | 4680
| rowspan=2|125.94440(43)#
| style="text-align:right" | 80
| rowspan=2|48.6(8)&nbsp;ms
|
| β<sup>−</sup> (78%)
| 48.6&nbsp;ms
| β<sup>−</sup>
| <sup>126</sup>Ag
| rowspan=2|0+
| rowspan=2|
|
| rowspan=2|
|
|-
| β<sup>−</sup>, n (22%)
| <sup>125</sup>Ag
|-id=Palladium-126m1
| style="text-indent:1em" | <sup>126m1</sup>Pd
| colspan="3" style="text-indent:2em" | 2023.5(7)&nbsp;keV
| 330(40)&nbsp;ns
| IT
| <sup>126</sup>Pd
| (5−)
|
|
|-id=Palladium-126m2
|-
| style="text-indent:1em" | <sup>126m2</sup>Pd
| colspan="3" style="text-indent:2em" | 21102109.7(9)&nbsp;keV
| 440(30)&nbsp;ns
| IT
| <sup>126m1126</sup>Pd
| (7−)
|
|
|-id=Palladium-126m3
| rowspan=2 style="text-indent:1em" | <sup>126m3</sup>Pd
| rowspan=2 colspan="3" style="text-indent:2em" | 2406.0(10)&nbsp;keV
| rowspan=2|23.0(8)&nbsp;ms
| β<sup>−</sup> (72%)
| <sup>126</sup>Ag
| rowspan=2|(10+)
| rowspan=2|
| rowspan=2|
|-
| IT (28%)
| <sup>127</sup>Pd
| <sup>126</sup>Pd
| style="text-align:right" | 46
|-id=Palladium-127
| style="text-align:right" | 81
| rowspan=3|<sup>127</sup>Pd
|
| rowspan=3 style="text-align:right" | 46
| 38&nbsp;ms
| rowspan=3 style="text-align:right" | 81
| β<sup>−</sup>
| rowspan=3|126.94931(54)#
| rowspan=3|38(2)&nbsp;ms
| β<sup>−</sup> (>81%)
| <sup>127</sup>Ag
| rowspan=3|11/2−#
|
| rowspan=3|
|
| rowspan=3|
|
|-
| β<sup>128</sup>Pd<ref, name="NM126A"n />(<ref name="NM126B" />19%)
| <sup>126</sup>Ag
| style="text-align:right" | 46
|-
| style="text-align:right" | 82
| β<sup>−</sup>, 2n?
| <sup>125</sup>Ag
|-id=Palladium-127m
| style="text-indent:1em" | <sup>127m</sup>Pd
| colspan="3" style="text-indent:2em" | 1717.91(23)&nbsp;keV
| 39(6)&nbsp;μs
| IT
| <sup>127</sup>Pd
| (19/2+)
|
|
| 35&nbsp;ms
|-id=Palladium-128
| rowspan=2|<sup>128</sup>Pd
| rowspan=2 style="text-align:right" | 46
| rowspan=2 style="text-align:right" | 82
| rowspan=2|127.95235(54)#
| rowspan=2|35(3)&nbsp;ms
| β<sup>−</sup>
| <sup>128</sup>Ag
| rowspan=2|0+
| rowspan=2|
|
| rowspan=2|
|
|-
| β<sup>−</sup>, n?
| <sup>127</sup>Ag
|-id=Palladium-128m
| style="text-indent:1em" | <sup>128m</sup>Pd
| colspan="3" style="text-indent:2em" | 2151.0(10)&nbsp;keV
| 5.8(8)&nbsp;µsμs
| IT
| <sup>128</sup>Pd
| (8+)
|
|
|-id=Palladium-129
| rowspan=3|<sup>129</sup>Pd
| rowspan=3 style="text-align:right" | 46
| rowspan=3 style="text-align:right" | 83
| rowspan=3|128.95933(64)#
| rowspan=3|31(7)&nbsp;ms
| β<sup>−</sup>
| <sup>129</sup>Ag
| rowspan=3|7/2−#
| rowspan=3|
| rowspan=3|
|-
| β<sup>129</sup>Pd, n?
| <sup>128</sup>Ag
| style="text-align:right" | 46
|-
| style="text-align:right" | 83
| β<sup>−</sup>, 2n?
|
| <sup>127</sup>Ag
| 31&nbsp;ms
|-id=Palladium-130
| rowspan=3|<sup>130</sup>Pd
| rowspan=3 style="text-align:right" | 46
| rowspan=3 style="text-align:right" | 84
| rowspan=3|129.96486(32)#
| rowspan=3|27#&nbsp;ms<br>[>550&nbsp;ns]
| β<sup>−</sup>
| <sup>130</sup>Ag
| rowspan=3|0+
| rowspan=3|
| rowspan=3|
|-
| β<sup>−</sup>, n?
| <sup>129</sup>Ag
|-
| β<sup>−</sup>, 2n?
| <sup>128</sup>Ag
 
|-id=Palladium-131
| rowspan=3|<sup>131</sup>Pd
| rowspan=3 style="text-align:right" | 46
| rowspan=3 style="text-align:right" | 85
| rowspan=3|130.97237(32)#
| rowspan=3|20#&nbsp;ms<br>[>550&nbsp;ns]
| β<sup>−</sup>
| <sup>131</sup>Ag
| rowspan=3|7/2−#
| rowspan=3|
| rowspan=3|
|-
| β<sup>−</sup>, n?
| <sup>130</sup>Ag
|-
| β<sup>−</sup>, 2n?
| <sup>129</sup>Ag
|
|
|
{{Isotopes table/footer}}
 
Line 610 ⟶ 808:
'''Palladium-107''' is the second-longest lived ([[half-life]] of 6.5&nbsp;million years<ref name="webelements" />) and least radioactive ([[decay energy]] only 33&nbsp;[[keV]], [[specific activity]] 5{{e|-5}}&nbsp;Ci/g) of the 7 long-lived [[fission products]]. It undergoes pure [[beta decay]] (without [[gamma radiation]]) to [[Silver-107|<sup>107</sup>Ag]], which is stable.
 
Its yield from [[thermal neutron]] fission of [[uranium-235]] is 0.162914% per fission,<ref name=Pd107-2021>{{cite journal |title=Detection of the Fission Product Palladium-107 in a Pond Sediment Sample from Chernobyl |first1=A. |last1=Weller |first2=T. |last2=Ramaker |first3=F. |last3=Stäger |first4=T. |last4=Blenke |first5=M. |last5=Raiwa |first6=I. |last6=Chyzhevskyi |first7=S. |last7=Kirieiev|first8=S. |last8=Dubchak |first9=G. |last9=Steinhauser |journal=Environmental Science & Technology Letters |date=2021 |volume=8 |issue=8 |pages=656–661 |doi=10.1021/acs.estlett.1c00420 |bibcode=2021EnSTL...8..656W |url=https://www.researchgate.net/publication/352972522}}</ref> only 1/4 that of [[iodine-129]], and only 1/40 those of [[Technetium-99|<sup>99</sup>Tc]], [[Zirconium-93|<sup>93</sup>Zr]], and [[CesiumCaesium-135|<sup>135</sup>Cs]]. Yield from [[Uranium-233|<sup>233</sup>U]] is slightly lower, but yield from [[Plutonium-239|<sup>239</sup>Pu]] is much higher, 3.32%.<ref name=Pd107-2021/> [[Fast fission]] or fission of some heavier [[actinides]]<sup>''[which?]''</sup> will produce palladium-107 at higher yields.
 
One source<ref>{{cite journal |author=R. P. Bush |title=Recovery of Platinum Group Metals from High Level Radioactive Waste |journal=Platinum Metals Review |year=1991 |volume=35 |issue=4 |pages=202–208 |doi=10.1595/003214091X354202208 |url=http://www.platinummetalsreview.com/pdf/pmr-v35-i4-202-208.pdf |access-date=2011-04-02 |archive-date=2015-09-24 |archive-url=https://web.archive.org/web/20150924074421/http://www.platinummetalsreview.com/pdf/pmr-v35-i4-202-208.pdf |url-status=dead }}</ref> estimates that palladium produced from fission contains the isotopes <sup>104</sup>Pd (16.9%),<sup>105</sup>Pd (29.3%), <sup>106</sup>Pd (21.3%), <sup>107</sup>Pd (17%), <sup>108</sup>Pd (11.7%) and <sup>110</sup>Pd (3.8%). According to another source, the proportion of <sup>107</sup>Pd is 9.2% for palladium from thermal neutron fission of [[Uranium-235|<sup>235</sup>U]], 11.8% for <sup>233</sup>U, and 20.4% for <sup>239</sup>Pu (and the <sup>239</sup>Pu yield of palladium is about 10 times that of <sup>235</sup>U).
 
Because of this dilution and because <sup>105</sup>Pd has 11 times the [[neutron absorption]] [[Neutron cross section|cross section]], <sup>107</sup>Pd is not amenable to disposal by [[nuclear transmutation]]. However, as a [[noble metal]], palladium is not as mobile in the environment as iodine or technetium.
Line 622 ⟶ 820:
**{{NUBASE 2003}}
* Isotopic compositions and standard atomic masses from:
**{{CAWIA 2003CIAAW2003}}
**{{CIAAW 2005}}
* Half-life, spin, and isomer data selected from the following sources.