Изотопи на родиумот

Природно настанатиот родиум (45Rh) има само еден стабилен изотоп, 103Rh. Најстабилни радиоизотопи се 101Rh со време на полураспад од 3,3 години, 102Rh со време на полураспад од 207 дена и 99Rh со време на полураспад од 16,1 дена. Триесет други радиоизотопи се одликуваат со атомска тежина која се движи од 88,949 u (89Rh) до 121.943 u (122Rh). Повеќето од нив имаат време на полураспад помало од еден час, освен 100Rh (време на полураспад: 20,8 часа) и 105Rh (време на полураспад: 35,36 часа). Исто така, постојат бројни мета состојби со најстабилен 102mRh (0,141&nbsp;MeV) со време на полураспад од околу 3,7 години и 101mRh (0,157 MeV) со време на полураспад од 4,34 дена.

Примарниот режим на распаѓање пред единствениот стабилен изотоп, 103Rh, е електронскиот зафат, а примарниот режим после е бета емисија. Примарниот распаден производ пред 103Rh е рутениум, а примарниот производ после е паладиум.

## Список на изотопи

|-id=Родиум-90
| rowspan=2|90Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 45
| rowspan=2|89,94457(22)#
| rowspan=2|29(3)&nbsp;ms
| β<sup>+</sup>
| 90Ru
| rowspan=2|(0+)
| rowspan=2|
|-
| β+, p? (89Tc
|-id=Родиум-90m
| rowspan=2 style="text-indent:1em" | 90mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 0(500)#&nbsp;keV
| rowspan=2|0,56(2)&nbsp;s
| β+ (90,4%)
| 90Ru
| rowspan=2|(7+)
| rowspan=2|
|-
| β+, p (9,6%)
| 89Tc
|-id=Родиум-91
| rowspan=2|91Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 46
| rowspan=2|90,93712(32)#
| rowspan=2|1,47(22)&nbsp;s
| β+ (98,7%)
| 91Ru
| rowspan=2|(9/2+)
| rowspan=2|
|-
| β+, p (1,3%)
| 90Tc
|-id=Родиум-91m
| rowspan=3 style="text-indent:1em" | 91mRh
| rowspan=3 colspan="3" style="text-indent:2em" | 172,9(4)&nbsp;keV
| rowspan=3|1,8#&nbsp;s
| β+?
| 91Ru
| rowspan=3|1/2−#
| rowspan=3|
|-
| β+, p?
| 90Tc
|-
| IT?
| 91Rh
|-id=Родиум-92
| rowspan=2|92Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 47
| rowspan=2|91,9323677(47)
| rowspan=2|5,61(8)&nbsp;s
| β+ (97,95%)
| 92Ru
| rowspan=2|(6+)
| rowspan=2|
|-
| β+, p (2,05%)
| 91Tc
|-id=Родиум-92m1
| rowspan=2 style="text-indent:1em" | 92m1Rh
| rowspan=2 colspan="3" style="text-indent:2em" | 50(100)#&nbsp;keV
| rowspan=2|3,18(22)&nbsp;s
| β+ (98,3%)
| 92Ru
| rowspan=2|(2+)
| rowspan=2|
|-
| β+, p (1,7%)
| 91Tc
|-id=Родиум-92m2
| style="text-indent:1em" | 92m2Rh
| colspan="3" style="text-indent:2em" | 105(100)#&nbsp;keV
| 232(15)&nbsp;ns
| IT
| 92Rh
| (4+)
| 
|-id=Родиум-93
| 93Rh
| style="text-align:right" | 45
| style="text-align:right" | 48
| 92,9259128(28)
| 13,9(16)&nbsp;s
| β+
| 93Ru
| 9/2+#
|
|-id=Родиум-94
| rowspan=2|94Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 49
| rowspan=2|93,9217305(36)
| rowspan=2|70,6(6)&nbsp;s
| β+ (98,2%)
| 94Ru
| rowspan=2|(4+)
| rowspan=2|
|-
| β+, p (1,8%)
| 93Tc
|-id=Родиум-94m1
| style="text-indent:1em" | 94m1Rh
| colspan="3" style="text-indent:2em" | 54,60(20)#&nbsp;keV
| 480(30)&nbsp;ns
| IT
| 94Rh
| (2+)
| 
|-id=Родиум-94m2
| style="text-indent:1em" | 94m2Rh
| colspan="3" style="text-indent:2em" | 300(200)#&nbsp;keV
| 25,8(2)&nbsp;s
| β+
| 94Ru
| (8+)
| 
|-id=Родиум-95
| 95Rh
| style="text-align:right" | 45
| style="text-align:right" | 50
| 94,9158979(42)
| 5,02(10)&nbsp;min
| β+
| 95Ru
| (9/2)+
|
|-id=Родиум-95m
| rowspan=2 style="text-indent:1em" | 95mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 543,3(3)&nbsp;keV
| rowspan=2|1,96(4)&nbsp;min
| IT (88%)
| 95Rh
| rowspan=2|(1/2)−
| rowspan=2|
|-
| β+ (12%)
| 95Ru
|-id=Родиум-96
| 96Rh
| style="text-align:right" | 45
| style="text-align:right" | 51
| 95 914452(11)
| 9,90(10)&nbsp;min
| β+
| **<sup>96</sup>Ru**
| 6+
|
|-id=Родиум-96m
| rowspan=2 style="text-indent:1em" | 96mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 51,98(9)&nbsp;keV
| rowspan=2|1,51(2)&nbsp;min
| IT (60%)
| 96Rh
| rowspan=2|3+
| rowspan=2|
|-
| β+ (40%)
| **<sup>96</sup>Ru**
|-id=Родиум-97
| 97Rh
| style="text-align:right" | 45
| style="text-align:right" | 52
| 96,911328(38)
| 30,7(6)&nbsp;min
| β+
| 97Ru
| 9/2+
|
|-id=Родиум-97m
| rowspan=2 style="text-indent:1em" | 97mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 258,76(18)&nbsp;keV
| rowspan=2|46,2(16)&nbsp;min
| β+ (94,4%)
| 97Ru
| rowspan=2|1/2−
| rowspan=2|
|-
| IT (5,6%)
| 97Rh
|-id=Родиум-98
| 98Rh
| style="text-align:right" | 45
| style="text-align:right" | 53
| 97,910708(13)
| 8,72(12)&nbsp;min
| β+
| **<sup>98</sup>Ru**
| (2)+
|
|-id=Родиум-98m
| rowspan=2 style="text-indent:1em" | 98mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 56,3(10)&nbsp;keV
| rowspan=2|3,6(2)&nbsp;min
| IT (89%)
| 98Rh
| rowspan=2|(5+)
| rowspan=2|
|-
| β+ (11%)
| **<sup>98</sup>Ru**
|-id=Родиум-99
| 99Rh
| style="text-align:right" | 45
| style="text-align:right" | 54
| 98,908121(21)
| 16,1(2)&nbsp;d
| β+
| **<sup>99</sup>Ru**
| 1/2−
|
|-id=Родиум-99m
| rowspan=2 style="text-indent:1em" | 99mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 64,4(5)&nbsp;keV
| rowspan=2|4,7(1)&nbsp;h
| β+
| **<sup>99</sup>Ru**
| rowspan=2|9/2+
| rowspan=2|
|-
| IT?
| 99Rh
|-id=Родиум-100
| rowspan=2|100Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 55
| rowspan=2|99,908114(19)
| rowspan=2|20,8(1)&nbsp;h
| EC (95,1%)
| **<sup>100</sup>Ru**
| rowspan=2|1−
| rowspan=2|
|-
| β+ (4,9%)
| **<sup>100</sup>Ru**
|-id=Родиум-100m1
| style="text-indent:1em" | 100m1Rh
| colspan="3" style="text-indent:2em" | 74,782(14)&nbsp;keV
| 214,0(20)&nbsp;ns
| IT
| 100Rh
| (2)+
| 
|-id=Родиум-100m2
| rowspan=2 style="text-indent:1em" | 100m2Rh
| rowspan=2 colspan="3" style="text-indent:2em" | 107,6(2)&nbsp;keV
| rowspan=2|4,6(2)&nbsp;min
| IT (98,3%)
| 100Rh
| rowspan=2|(5+)
| rowspan=2|
|-
| β+ (1,7%)
| **<sup>100</sup>Ru**
|-id=Родиум-100m3
| style="text-indent:1em" | 100m3Rh
| colspan="3" style="text-indent:2em" | 219,61(22)&nbsp;keV
| 130(10)&nbsp;ns
| IT
| 100Rh
| (7+)
|
|-id=Родиум-101
| 101Rh
| style="text-align:right" | 45
| style="text-align:right" | 56
| 100,9061589(63)
| 4,07(5)&nbsp;y
| EC
| **<sup>101</sup>Ru**
| 1/2−
|
|-id=Родиум-101m
| rowspan=2 style="text-indent:1em" | 101mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 157,32(3)&nbsp;keV
| rowspan=2|4,343(10)&nbsp;d
| EC (92,80%)
| **<sup>101</sup>Ru**
| rowspan=2|9/2+
| rowspan=2|
|-
| IT (7,20%)
| 101Rh
|-id=Родиум-102
| rowspan=2|102Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 57
| rowspan=2|101,9068343(69)
| rowspan=2|207,0(15)&nbsp;d
| β+ (78%)
| **<sup>102</sup>Ru**
| rowspan=2|2−
| rowspan=2|
|-
| β− (22%)
| **<sup>102</sup>Pd**
|-id=Родиум-102m
| rowspan=2 style="text-indent:1em" | 102mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 140,73(9)&nbsp;keV
| rowspan=2|3,742(10)&nbsp;y
| β+ (99,77%)
| **<sup>102</sup>Ru**
| rowspan=2|6+
| rowspan=2|
|-
| IT (0,233%)
| 102Rh
|-id=Родиум-103
| 103Rh
| style="text-align:right" | 45
| style="text-align:right" | 58
| 102,9054941(25)
| colspan=3 align=center|**Stable**
| 1/2−
| 1,0000
|-id=Родиум-103m
| style="text-indent:1em" | 103mRh
| colspan="3" style="text-indent:2em" | 39,753(6)&nbsp;keV
| 56,114(9)&nbsp;min
| IT
| **<sup>103</sup>Rh**
| 7/2+
|
|-id=Родиум-104
| rowspan=2|104Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 59
| rowspan=2|103,9066453(25)
| rowspan=2|42,3(4)&nbsp;s
| β− (99,55%)
| **<sup>104</sup>Pd**
| rowspan=2|1+
| rowspan=2|
|-
| β+ (0,45%)
| **<sup>104</sup>Ru**
|-id=Родиум-104m
| rowspan=2 style="text-indent:1em" | 104mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 128,9679(5)&nbsp;keV
| rowspan=2|4,34(3)&nbsp;min
| IT (99,87%)
| 104Rh
| rowspan=2|5+
| rowspan=2|
|-
| β− (0,13%)
| **<sup>104</sup>Pd**
|-id=Родиум-105
| 105Rh
| style="text-align:right" | 45
| style="text-align:right" | 60
| 104,9056878(27)
| 35,341(19)&nbsp;h
| β−
| **<sup>105</sup>Pd**
| 7/2+
|
|-id=Родиум-105m
| style="text-indent:1em" | 105mRh
| colspan="3" style="text-indent:2em" | 129,742(4)&nbsp;keV
| 42,8(3)&nbsp;s
| IT
| 105Rh
| 1/2−
| 
|-id=Родиум-106
| 106Rh
| style="text-align:right" | 45
| style="text-align:right" | 61
| 105,9072859(58)
| 30,07(35)&nbsp;s
| β−
| **<sup>106</sup>Pd**
| 1+
|
|-id=Родиум-106m
| style="text-indent:1em" | 106mRh
| colspan="3" style="text-indent:2em" | 132(11)&nbsp;keV
| 131(2)&nbsp;min
| β−
| **<sup>106</sup>Pd**
| (6)+
|
|-id=Родиум-107
| 107Rh
| style="text-align:right" | 45
| style="text-align:right" | 62
| 106,906748(13)
| 21,7(4)&nbsp;min
| β−
| 107Pd
| 7/2+
|-id=Родиум-107m
| style="text-indent:1em" | 107mRh
| colspan="3" style="text-indent:2em" | 268,36(4)&nbsp;keV
| >10&nbsp;μs
| IT
| 107Rh
| 1/2−
|
|-id=Родиум-108
| 108Rh
| style="text-align:right" | 45
| style="text-align:right" | 63
| 107,908715(15)
| 16,8(5)&nbsp;s
| β−
| **<sup>108</sup>Pd**
| 1+
|
|-id=Родиум-108m
| style="text-indent:1em" | 108mRh
| colspan="3" style="text-indent:2em" | 115(18)&nbsp;keV
| 6,0(3)&nbsp;min
| β−
| **<sup>108</sup>Pd**
| (5+)
|
|-id=Родиум-109
| 109Rh
| style="text-align:right" | 45
| style="text-align:right" | 64
| 108,9087496(43)
| 80,8(7)&nbsp;s
| β−
| 109Pd
| 7/2+
|
|-id=Родиум-109m
| style="text-indent:1em" | 109mRh
| colspan="3" style="text-indent:2em" | 225,873(19)&nbsp;keV
| 1,66(4)&nbsp;μs
| IT
| 109Pd
| 3/2+
|
|-id=Родиум-110
| 110Rh
| style="text-align:right" | 45
| style="text-align:right" | 65
| 109,911080(19)
| 3,35(12)&nbsp;s
| β−
| **<sup>110</sup>Pd**
| (1+)
|
|-id=Родиум-110m
| style="text-indent:1em" | 110mRh
| colspan="3" style="text-indent:2em" | 220(150)#&nbsp;keV
| 28,5(13)&nbsp;s
| β−
| **<sup>110</sup>Pd**
| (6+)
|
|-id=Родиум-111
| 111Rh
| style="text-align:right" | 45
| style="text-align:right" | 66
| 110,9116432(74)
| 11(1)&nbsp;s
| β−
| 111Pd
| (7/2+)
|
|-id=Родиум-112
| 112Rh
| style="text-align:right" | 45
| style="text-align:right" | 67
| 111,914405(47)
| 3,4(4)&nbsp;s
| β−
| 112Pd
| (1+)
|
|-id=Родиум-112m
| style="text-indent:1em" | 112mRh
| colspan="3" style="text-indent:2em" | 340(70)&nbsp;keV
| 6,73(15)&nbsp;s
| β−
| 112Pd
| (6+)
|
|-id=Родиум-113
| 113Rh
| style="text-align:right" | 45
| style="text-align:right" | 68
| 112,9154402(77)
| 2,80(12)&nbsp;s
| β−
| 113Pd
| (7/2+)
|
|-id=Родиум-114
| 114Rh
| style="text-align:right" | 45
| style="text-align:right" | 69
| 113,918722(77)
| 1,85(5)&nbsp;s
| β−
| 114Pd
| 1+
| 
|-id=Родиум-114m
| style="text-indent:1em" | 114mRh
| colspan="3" style="text-indent:2em" | 200(150)#&nbsp;keV
| 1,85(5)&nbsp;s
| β−
| 114Pd
| (7−)
|
|-id=Родиум-115
| rowspan=2|115Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 70
| rowspan=2|114,9203116(79)
| rowspan=2|1,03(3)&nbsp;s
| β−
| 115Pd
| rowspan=2|(7/2+)
| rowspan=2|
|-
| β−, n?
| 114Pd
|-id=Родиум-116
| rowspan=2|116Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 71
| rowspan=2|115,924062(79)
| rowspan=2|685(39)&nbsp;ms
| β− (>97,9%)
| 116Pd
| rowspan=2|1+
| rowspan=2|
|-
| β−, n? (115Pd
|-id=Родиум-116m
| rowspan=2 style="text-indent:1em" | 116mRh
| rowspan=2 colspan="3" style="text-indent:2em" | 200(150)#&nbsp;keV
| rowspan=2|570(50)&nbsp;ms
| β− (>97,9%)
| 116Pd
| rowspan=2|(6−)
| rowspan=2|
|-
| β−, n? (115Pd
|-id=Родиум-117
| rowspan=2|117Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 72
| rowspan=2|116,9260363(95)
| rowspan=2|421(30)&nbsp;ms
| β−
| 117Pd
| rowspan=2|7/2+#
| rowspan=2|
|-
| β−, n? (115Pd
|-id=Родиум-117m
| style="text-indent:1em" | 117mRh
| colspan="3" style="text-indent:2em" | 321,2(10)&nbsp;keV
| 138(17)&nbsp;ns
| IT
| 117Rh
| 3/2+#
|
|-id=Родиум-118
| rowspan=2|118Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 73
| rowspan=2|117,930341(26)
| rowspan=2|282(9)&nbsp;ms
| β− (96,9%)
| 118Pd
| rowspan=2|1+#
| rowspan=2|
|-
| β−, n (3,1%)
| 117Pd
|-id=Родиум-118m
| rowspan=3 style="text-indent:1em" | 118mRh
| rowspan=3 colspan="3" style="text-indent:2em" | 200(150)#&nbsp;keV
| rowspan=3|310(30)&nbsp;ms
| β− (96,9%)
| 118Pd
| rowspan=3|6−#
| rowspan=3|
|-
| β−, n (3,1%)
| 117Pd
|-
| IT?
| 118Rh
|-id=Родиум-119
| rowspan=2|119Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 74
| rowspan=2|118,932557(10)
| rowspan=2|190(6)&nbsp;ms
| β− (93,6%)
| 119Pd
| rowspan=2|7/2+#
| rowspan=2|
|-
| β−, n (6,4%)
| 118Pd
|-id=Родиум-120
| rowspan=3| 120Rh
| rowspan=3 style="text-align:right" | 45
| rowspan=3 style="text-align:right" | 75
| rowspan=3| 119,93707(22)#
| rowspan=3| 129,6(42)&nbsp;ms
| β−
| 120Pd
| rowspan=3| 8−#
| rowspan=3|
|-
| β−, n (119Pd
|-
| β−, 2n?
| 118Pd
|-id=Родиум-120m
| style="text-indent:1em" | 120mRh
| colspan="3" style="text-indent:2em" | 157,2(7)&nbsp;keV
| 295(16)&nbsp;ns
| IT
| 120Rh
| 6#
|
|-id=Родиум-121
| rowspan=2| 121Rh
| rowspan=2 style="text-align:right" | 45
| rowspan=2 style="text-align:right" | 76
| rowspan=2| 120,93961(67)
| rowspan=2| 74(4)&nbsp;ms
| β−
| 121Pd
| rowspan=2| 7/2+#
| rowspan=2|
|-
| β−, n (>11%)
| 120Pd
|-id=Родиум-122
| rowspan=3| 122Rh
| rowspan=3 style="text-align:right" | 45
| rowspan=3 style="text-align:right" | 77
| rowspan=3| 121,94431(32)#
| rowspan=3| 51(6)&nbsp;ms
| β−
| 122Pd
| rowspan=3| 7−#
| rowspan=3|
|-
| β−, n (121Pd
|-
| β−, 2n?
| 120Pd
|-id=Родиум-122m
| style="text-indent:1em" | 122mRh
| colspan="3" style="text-indent:2em" | 271,0(7)&nbsp;keV
| 830(120)&nbsp;ns
| IT
| 122Rh
| 4+#
|
|-id=Родиум-123
| rowspan=3| 123Rh
| rowspan=3 style="text-align:right" | 45
| rowspan=3 style="text-align:right" | 78
| rowspan=3| 122,94719(43)#
| rowspan=3| 42(4)&nbsp;ms
| β−
| 123Pd
| rowspan=3| 7/2+#
| rowspan=3|
|-
| β−, n (>24%)
| 122Pd
|-
| β−, 2n?
| 121Pd
|-id=Родиум-124
| rowspan=3| 124Rh
| rowspan=3 style="text-align:right" | 45
| rowspan=3 style="text-align:right" | 79
| rowspan=3| 123,95200(43)#
| rowspan=3| 30(2)&nbsp;ms
| β−
| 124Pd
| rowspan=3| 2+#
| rowspan=3|
|-
| β−, n (123Pd
|-
| β−, 2n?
| 122Pd
|-id=Родиум-125
| rowspan=3|125Rh
| rowspan=3 style="text-align:right" | 45
| rowspan=3 style="text-align:right" | 80
| rowspan=3|124,95509(54)#
| rowspan=3|26,5(20)&nbsp;ms
| β−
| 125Pd
| rowspan=3|7/2+#
| rowspan=3|
|-
| β−, n?
| 124Pd
|-
| β−, 2n?
| 123Pd
|-id=Родиум-126
| rowspan=3|126Rh
| rowspan=3 style="text-align:right" | 45
| rowspan=3 style="text-align:right" | 81
| rowspan=3|125,96006(54)#
| rowspan=3|19(3)&nbsp;ms
| β−
| 126Pd
| rowspan=3|1−#
| rowspan=3|
|-
| β−, n?
| 125Pd
|-
| β−, 2n?
| 124Pd
|-id=Родиум-127
| rowspan=3|127Rh
| rowspan=3 style="text-align:right" | 45
| rowspan=3 style="text-align:right" | 82
| rowspan=3|126,96379(64)#
| rowspan=3|28(14)&nbsp;ms
| β−
| 127Pd
| rowspan=3|7/2+#
| rowspan=3|
|-
| β−, n?
| 126Pd
|-
| β−, 2n?
| 125Pd
|-id=Родиум-128
| rowspan=3|128Rh
| rowspan=3 style="text-align:right" | 45
| rowspan=3 style="text-align:right" | 83
| rowspan=3|127,97065(32)#
| rowspan=3|8#&nbsp;ms[>550&nbsp;ns]
| β−?
| 128Pd
| rowspan=3|
| rowspan=3|
|-
| β−, n?
| 127Pd
|-
| β−, 2n?
| 126Pd

## Белешки


## Наводи

* Isotope masses from:
**
* Half-life, spin, and isomer data selected from the following sources.
**
**
**

Родиум
Категорија:Родиум
Категорија:Изотопи на родиумот