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Isotopes of rhodium

Naturally occurring rhodium (<sub>45</sub>Rh) is composed of only one stable isotope, <sup>103</sup>Rh. The most stable radioisotopes are <sup>101</sup>Rh with a half-life of 4.07 years, <sup>102</sup>Rh with a half-life of 207 days, and <sup>99</sup>Rh with a half-life of 16.1 days. Thirty other radioisotopes have been characterized ranging from <sup>89</sup>Rh to <sup>122</sup>Rh - these have half-lives that are less than an hour except <sup>100</sup>Rh (20.8 hours) and <sup>105</sup>Rh (35.34 hours). There are also numerous meta states with the most stable being <sup>102m</sup>Rh with a half-life of 3.74 years and <sup>101m</sup>Rh with a half-life of 4.34 days.

The primary decay mode before the only stable isotope, <sup>103</sup>Rh, is electron capture to ruthenium isotopes, and the primary mode after is beta emission to palladium isotopes. Mass numbers 102 and 104 are capable of decay in either sense.

List of isotopes

|-id=Rhodium-90 | rowspan=2|<sup>90</sup>Rh | 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> | <sup>90</sup>Ru | rowspan=2|(0+) | rowspan=2| |- | β<sup>+</sup>, p? (<0.7%) | <sup>89</sup>Tc |-id=Rhodium-90m | rowspan=2 style="text-indent:1em" | <sup>90m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 0(500)#&nbsp;keV | rowspan=2|0.56(2)&nbsp;s | β<sup>+</sup> (90.4%) | <sup>90</sup>Ru | rowspan=2|(7+) | rowspan=2| |- | β<sup>+</sup>, p (9.6%) | <sup>89</sup>Tc |-id=Rhodium-91 | rowspan=2|<sup>91</sup>Rh | 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<sup>+</sup> (98.7%) | <sup>91</sup>Ru | rowspan=2|(9/2+) | rowspan=2| |- | β<sup>+</sup>, p (1.3%) | <sup>90</sup>Tc |-id=Rhodium-91m | rowspan=3 style="text-indent:1em" | <sup>91m</sup>Rh | rowspan=3 colspan="3" style="text-indent:2em" | 172.9(4)&nbsp;keV | rowspan=3|1.8#&nbsp;s | β<sup>+</sup>? | <sup>91</sup>Ru | rowspan=3|1/2−# | rowspan=3| |- | β<sup>+</sup>, p? | <sup>90</sup>Tc |- | IT? | <sup>91</sup>Rh |-id=Rhodium-92 | rowspan=2|<sup>92</sup>Rh | 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<sup>+</sup> (97.95%) | <sup>92</sup>Ru | rowspan=2|(6+) | rowspan=2| |- | β<sup>+</sup>, p (2.05%) | <sup>91</sup>Tc |-id=Rhodium-92m1 | rowspan=2 style="text-indent:1em" | <sup>92m1</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 50(100)#&nbsp;keV | rowspan=2|3.18(22)&nbsp;s | β<sup>+</sup> (98.3%) | <sup>92</sup>Ru | rowspan=2|(2+) | rowspan=2| |- | β<sup>+</sup>, p (1.7%) | <sup>91</sup>Tc |-id=Rhodium-92m2 | style="text-indent:1em" | <sup>92m2</sup>Rh | colspan="3" style="text-indent:2em" | 105(100)#&nbsp;keV | 232(15)&nbsp;ns | IT | <sup>92</sup>Rh | (4+) | |-id=Rhodium-93 | <sup>93</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 48 | 92.9259128(28) | 13.9(16)&nbsp;s | β<sup>+</sup> | <sup>93</sup>Ru | 9/2+# | |-id=Rhodium-93m | style="text-indent:1em" | <sup>93m</sup>Rh | colspan="3" style="text-indent:2em" | 267(48)&nbsp;keV | | | | (1/2−) | |-id=Rhodium-94 | rowspan=2|<sup>94</sup>Rh | 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<sup>+</sup> (98.2%) | <sup>94</sup>Ru | rowspan=2|(4+) | rowspan=2| |- | β<sup>+</sup>, p (1.8%) | <sup>93</sup>Tc |-id=Rhodium-94m1 | style="text-indent:1em" | <sup>94m1</sup>Rh | colspan="3" style="text-indent:2em" | 54.60(20)#&nbsp;keV | 480(30)&nbsp;ns | IT | <sup>94</sup>Rh | (2+) | |-id=Rhodium-94m2 | style="text-indent:1em" | <sup>94m2</sup>Rh | colspan="3" style="text-indent:2em" | 300(200)#&nbsp;keV | 25.8(2)&nbsp;s | β<sup>+</sup> | <sup>94</sup>Ru | (8+) | |-id=Rhodium-95 | <sup>95</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 50 | 94.9158979(42) | 5.02(10)&nbsp;min | β<sup>+</sup> | <sup>95</sup>Ru | (9/2)+ | |-id=Rhodium-95m | rowspan=2 style="text-indent:1em" | <sup>95m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 543.3(3)&nbsp;keV | rowspan=2|1.96(4)&nbsp;min | IT (88%) | <sup>95</sup>Rh | rowspan=2|(1/2)− | rowspan=2| |- | β<sup>+</sup> (12%) | <sup>95</sup>Ru |-id=Rhodium-96 | <sup>96</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 51 | 95.914452(11) | 9.90(10)&nbsp;min | β<sup>+</sup> | <sup>96</sup>Ru | 6+ | |-id=Rhodium-96m | rowspan=2 style="text-indent:1em" | <sup>96m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 51.98(9)&nbsp;keV | rowspan=2|1.51(2)&nbsp;min | IT (60%) | <sup>96</sup>Rh | rowspan=2|3+ | rowspan=2| |- | β<sup>+</sup> (40%) | <sup>96</sup>Ru |-id=Rhodium-97 | <sup>97</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 52 | 96.911328(38) | 30.7(6)&nbsp;min | β<sup>+</sup> | <sup>97</sup>Ru | 9/2+ | |-id=Rhodium-97m | rowspan=2 style="text-indent:1em" | <sup>97m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 258.76(18)&nbsp;keV | rowspan=2|46.2(16)&nbsp;min | β<sup>+</sup> (94.4%) | <sup>97</sup>Ru | rowspan=2|1/2− | rowspan=2| |- | IT (5.6%) | <sup>97</sup>Rh |-id=Rhodium-98 | <sup>98</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 53 | 97.910708(13) | 8.72(12)&nbsp;min | β<sup>+</sup> | <sup>98</sup>Ru | (2)+ | |-id=Rhodium-98m | rowspan=2 style="text-indent:1em" | <sup>98m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 56.3(10)&nbsp;keV | rowspan=2|3.6(2)&nbsp;min | IT (89%) | <sup>98</sup>Rh | rowspan=2|(5+) | rowspan=2| |- | β<sup>+</sup> (11%) | <sup>98</sup>Ru |-id=Rhodium-99 | <sup>99</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 54 | 98.908121(21) | 16.1(2)&nbsp;d | β<sup>+</sup> | <sup>99</sup>Ru | 1/2− | |-id=Rhodium-99m | rowspan=2 style="text-indent:1em" | <sup>99m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 64.4(5)&nbsp;keV | rowspan=2|4.7(1)&nbsp;h | β<sup>+</sup> | <sup>99</sup>Ru | rowspan=2|9/2+ | rowspan=2| |- | IT? | <sup>99</sup>Rh |-id=Rhodium-100 | rowspan=2|<sup>100</sup>Rh | 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<sup>+</sup> (4.9%) | <sup>100</sup>Ru |-id=Rhodium-100m1 | style="text-indent:1em" | <sup>100m1</sup>Rh | colspan="3" style="text-indent:2em" | 74.782(14)&nbsp;keV | 214.0(20)&nbsp;ns | IT | <sup>100</sup>Rh | (2)+ | |-id=Rhodium-100m2 | rowspan=2 style="text-indent:1em" | <sup>100m2</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 107.6(2)&nbsp;keV | rowspan=2|4.6(2)&nbsp;min | IT (98.3%) | <sup>100</sup>Rh | rowspan=2|(5+) | rowspan=2| |- | β<sup>+</sup> (1.7%) | <sup>100</sup>Ru |-id=Rhodium-100m3 | style="text-indent:1em" | <sup>100m3</sup>Rh | colspan="3" style="text-indent:2em" | 219.61(22)&nbsp;keV | 130(10)&nbsp;ns | IT | <sup>100</sup>Rh | (7+) | |-id=Rhodium-101 | <sup>101</sup>Rh | 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=Rhodium-101m | rowspan=2 style="text-indent:1em" | <sup>101m</sup>Rh | 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%) | <sup>101</sup>Rh |-id=Rhodium-102 | rowspan=2|<sup>102</sup>Rh | 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<sup>+</sup> (78%) | <sup>102</sup>Ru | rowspan=2|2− | rowspan=2| |- | β<sup>−</sup> (22%) | <sup>102</sup>Pd |-id=Rhodium-102m | rowspan=2 style="text-indent:1em" | <sup>102m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 140.73(9)&nbsp;keV | rowspan=2|3.742(10)&nbsp;y | β<sup>+</sup> (99.77%) | <sup>102</sup>Ru | rowspan=2|6+ | rowspan=2| |- | IT (0.233%) | <sup>102</sup>Rh |-id=Rhodium-103 | <sup>103</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 58 | 102.9054941(25) | colspan=3 align=center|Stable | 1/2− | 1.0000 |-id=Rhodium-103m | style="text-indent:1em" | <sup>103m</sup>Rh | colspan="3" style="text-indent:2em" | 39.753(6)&nbsp;keV | 56.114(9)&nbsp;min | IT | <sup>103</sup>Rh | 7/2+ | |-id=Rhodium-104 | rowspan=2|<sup>104</sup>Rh | 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<sup>−</sup> (99.55%) | <sup>104</sup>Pd | rowspan=2|1+ | rowspan=2| |- | β<sup>+</sup> (0.45%) | <sup>104</sup>Ru |-id=Rhodium-104m | rowspan=2 style="text-indent:1em" | <sup>104m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 128.9679(5)&nbsp;keV | rowspan=2|4.34(3)&nbsp;min | IT (99.87%) | <sup>104</sup>Rh | rowspan=2|5+ | rowspan=2| |- | β<sup>−</sup> (0.13%) | <sup>104</sup>Pd |-id=Rhodium-105 | <sup>105</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 60 | 104.9056878(27) | 35.341(19)&nbsp;h | β<sup>−</sup> | <sup>105</sup>Pd | 7/2+ | |-id=Rhodium-105m | style="text-indent:1em" | <sup>105m</sup>Rh | colspan="3" style="text-indent:2em" | 129.742(4)&nbsp;keV | 42.8(3)&nbsp;s | IT | <sup>105</sup>Rh | 1/2− | |-id=Rhodium-106 | <sup>106</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 61 | 105.9072859(58) | 30.07(35)&nbsp;s | β<sup>−</sup> | <sup>106</sup>Pd | 1+ | |-id=Rhodium-106m | style="text-indent:1em" | <sup>106m</sup>Rh | colspan="3" style="text-indent:2em" | 132(11)&nbsp;keV | 131(2)&nbsp;min | β<sup>−</sup> | <sup>106</sup>Pd | (6)+ | |-id=Rhodium-107 | <sup>107</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 62 | 106.906748(13) | 21.7(4)&nbsp;min | β<sup>−</sup> | <sup>107</sup>Pd | 7/2+ |-id=Rhodium-107m | style="text-indent:1em" | <sup>107m</sup>Rh | colspan="3" style="text-indent:2em" | 268.36(4)&nbsp;keV | >10&nbsp;μs | IT | <sup>107</sup>Rh | 1/2− | |-id=Rhodium-108 | <sup>108</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 63 | 107.908715(15) | 16.8(5)&nbsp;s | β<sup>−</sup> | <sup>108</sup>Pd | 1+ | |-id=Rhodium-108m | style="text-indent:1em" | <sup>108m</sup>Rh | colspan="3" style="text-indent:2em" | 115(18)&nbsp;keV | 6.0(3)&nbsp;min | β<sup>−</sup> | <sup>108</sup>Pd | (5+) | |-id=Rhodium-109 | <sup>109</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 64 | 108.9087496(43) | 80.8(7)&nbsp;s | β<sup>−</sup> | <sup>109</sup>Pd | 7/2+ | |-id=Rhodium-109m | style="text-indent:1em" | <sup>109m</sup>Rh | colspan="3" style="text-indent:2em" | 225.873(19)&nbsp;keV | 1.66(4)&nbsp;μs | IT | <sup>109</sup>Rh | 3/2+ | |-id=Rhodium-110 | <sup>110</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 65 | 109.911080(19) | 3.35(12)&nbsp;s | β<sup>−</sup> | <sup>110</sup>Pd | (1+) | |-id=Rhodium-110m | style="text-indent:1em" | <sup>110m</sup>Rh | colspan="3" style="text-indent:2em" | 220(150)#&nbsp;keV | 28.5(13)&nbsp;s | β<sup>−</sup> | <sup>110</sup>Pd | (6+) | |-id=Rhodium-111 | <sup>111</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 66 | 110.9116432(74) | 11(1)&nbsp;s | β<sup>−</sup> | <sup>111</sup>Pd | (7/2+) | |-id=Rhodium-112 | <sup>112</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 67 | 111.914405(47) | 3.4(4)&nbsp;s | β<sup>−</sup> | <sup>112</sup>Pd | (1+) | |-id=Rhodium-112m | style="text-indent:1em" | <sup>112m</sup>Rh | colspan="3" style="text-indent:2em" | 340(70)&nbsp;keV | 6.73(15)&nbsp;s | β<sup>−</sup> | <sup>112</sup>Pd | (6+) | |-id=Rhodium-113 | <sup>113</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 68 | 112.9154402(77) | 2.80(12)&nbsp;s | β<sup>−</sup> | <sup>113</sup>Pd | (7/2+) | |-id=Rhodium-114 | <sup>114</sup>Rh | style="text-align:right" | 45 | style="text-align:right" | 69 | 113.918722(77) | 1.85(5)&nbsp;s | β<sup>−</sup> | <sup>114</sup>Pd | 1+ | |-id=Rhodium-114m | style="text-indent:1em" | <sup>114m</sup>Rh | colspan="3" style="text-indent:2em" | 200(150)#&nbsp;keV | 1.85(5)&nbsp;s | β<sup>−</sup> | <sup>114</sup>Pd | (7−) | |-id=Rhodium-115 | rowspan=2|<sup>115</sup>Rh | 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<sup>−</sup> | <sup>115</sup>Pd | rowspan=2|(7/2+) | rowspan=2| |- | β<sup>−</sup>, n? | <sup>114</sup>Pd |-id=Rhodium-116 | rowspan=2|<sup>116</sup>Rh | 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<sup>−</sup> (>97.9%) | <sup>116</sup>Pd | rowspan=2|1+ | rowspan=2| |- | β<sup>−</sup>, n? (<2.1%) | <sup>115</sup>Pd |-id=Rhodium-116m | rowspan=2 style="text-indent:1em" | <sup>116m</sup>Rh | rowspan=2 colspan="3" style="text-indent:2em" | 200(150)#&nbsp;keV | rowspan=2|570(50)&nbsp;ms | β<sup>−</sup> (>97.9%) | <sup>116</sup>Pd | rowspan=2|(6−) | rowspan=2| |- | β<sup>−</sup>, n? (<2.1%) | <sup>115</sup>Pd |-id=Rhodium-117 | rowspan=2|<sup>117</sup>Rh | 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<sup>−</sup> | <sup>117</sup>Pd | rowspan=2|7/2+# | rowspan=2| |- | β<sup>−</sup>, n? (<7.6%) | <sup>116</sup>Pd |-id=Rhodium-117m | style="text-indent:1em" | <sup>117m</sup>Rh | colspan="3" style="text-indent:2em" | 321.2(10)&nbsp;keV | 138(17)&nbsp;ns | IT | <sup>117</sup>Rh | 3/2+# | |-id=Rhodium-118 | rowspan=2|<sup>118</sup>Rh | 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<sup>−</sup> (96.9%) | <sup>118</sup>Pd | rowspan=2|1+# | rowspan=2| |- | β<sup>−</sup>, n (3.1%) | <sup>117</sup>Pd |-id=Rhodium-118m | rowspan=3 style="text-indent:1em" | <sup>118m</sup>Rh | rowspan=3 colspan="3" style="text-indent:2em" | 200(150)#&nbsp;keV | rowspan=3|310(30)&nbsp;ms | β<sup>−</sup> (96.9%) | <sup>118</sup>Pd | rowspan=3|6−# | rowspan=3| |- | β<sup>−</sup>, n (3.1%) | <sup>117</sup>Pd |- | IT? | <sup>118</sup>Rh |-id=Rhodium-119 | rowspan=2|<sup>119</sup>Rh | 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<sup>−</sup> (93.6%) | <sup>119</sup>Pd | rowspan=2|7/2+# | rowspan=2| |- | β<sup>−</sup>, n (6.4%) | <sup>118</sup>Pd |-id=Rhodium-120 | rowspan=3| <sup>120</sup>Rh | 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<sup>−</sup> | <sup>120</sup>Pd | rowspan=3| 8−# | rowspan=3| |- | β<sup>−</sup>, n (<9.3%) | <sup>119</sup>Pd |- | β<sup>−</sup>, 2n? | <sup>118</sup>Pd |-id=Rhodium-120m | style="text-indent:1em" | <sup>120m</sup>Rh | colspan="3" style="text-indent:2em" | 157.2(7)&nbsp;keV | 295(16)&nbsp;ns | IT | <sup>120</sup>Rh | 6# | |-id=Rhodium-121 | rowspan=2| <sup>121</sup>Rh | 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<sup>−</sup> | <sup>121</sup>Pd | rowspan=2| 7/2+# | rowspan=2| |- | β<sup>−</sup>, n (>11%) | <sup>120</sup>Pd |-id=Rhodium-122 | rowspan=3| <sup>122</sup>Rh | 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<sup>−</sup> | <sup>122</sup>Pd | rowspan=3| 7−# | rowspan=3| |- | β<sup>−</sup>, n (<3.9%) | <sup>121</sup>Pd |- | β<sup>−</sup>, 2n? | <sup>120</sup>Pd |-id=Rhodium-122m | style="text-indent:1em" | <sup>122m</sup>Rh | colspan="3" style="text-indent:2em" | 271.0(7)&nbsp;keV | 830(120)&nbsp;ns | IT | <sup>122</sup>Rh | 4+# | |-id=Rhodium-123 | rowspan=3| <sup>123</sup>Rh | 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<sup>−</sup> | <sup>123</sup>Pd | rowspan=3| 7/2+# | rowspan=3| |- | β<sup>−</sup>, n (>24%) | <sup>122</sup>Pd |- | β<sup>−</sup>, 2n? | <sup>121</sup>Pd |-id=Rhodium-124 | rowspan=3| <sup>124</sup>Rh | 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<sup>−</sup> | <sup>124</sup>Pd | rowspan=3| 2+# | rowspan=3| |- | β<sup>−</sup>, n (<31%) | <sup>123</sup>Pd |- | β<sup>−</sup>, 2n? | <sup>122</sup>Pd |-id=Rhodium-125 | rowspan=3|<sup>125</sup>Rh | 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<sup>−</sup> | <sup>125</sup>Pd | rowspan=3|7/2+# | rowspan=3| |- | β<sup>−</sup>, n? | <sup>124</sup>Pd |- | β<sup>−</sup>, 2n? | <sup>123</sup>Pd |-id=Rhodium-126 | rowspan=3|<sup>126</sup>Rh | 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<sup>−</sup> | <sup>126</sup>Pd | rowspan=3|1−# | rowspan=3| |- | β<sup>−</sup>, n? | <sup>125</sup>Pd |- | β<sup>−</sup>, 2n? | <sup>124</sup>Pd |-id=Rhodium-127 | rowspan=3|<sup>127</sup>Rh | 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<sup>−</sup> | <sup>127</sup>Pd | rowspan=3|7/2+# | rowspan=3| |- | β<sup>−</sup>, n? | <sup>126</sup>Pd |- | β<sup>−</sup>, 2n? | <sup>125</sup>Pd |-id=Rhodium-128 | rowspan=3|<sup>128</sup>Rh | rowspan=3 style="text-align:right" | 45 | rowspan=3 style="text-align:right" | 83 | rowspan=3|127.97065(32)# | rowspan=3|8#&nbsp;ms[>&nbsp;550&nbsp;ns] | β<sup>−</sup>? | <sup>128</sup>Pd | rowspan=3| | rowspan=3| |- | β<sup>−</sup>, n? | <sup>127</sup>Pd |- | β<sup>−</sup>, 2n? | <sup>126</sup>Pd

See also

Daughter products other than rhodium

References

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