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Isotopes of neodymium

Naturally occurring neodymium (<sub>60</sub>Nd) is composed of five stable isotopes, <sup>142</sup>Nd, <sup>143</sup>Nd, <sup>145</sup>Nd, <sup>146</sup>Nd and <sup>148</sup>Nd, with <sup>142</sup>Nd being the most abundant (27.2% natural abundance), and two long-lived radioisotopes, <sup>144</sup>Nd and <sup>150</sup>Nd. In all, 35 radioisotopes of neodymium have been characterized up to now, with the most stable being naturally occurring isotopes <sup>144</sup>Nd (alpha decay, a half-life (t<sub>1/2</sub>) of years) and <sup>150</sup>Nd (double beta decay, t<sub>1/2</sub> of years), and for practical purposes they can be considered to be stable as well. The radioactivity of <sup>144</sup>Nd is due to it having 84 neutrons (two more than 82, which is a magic number corresponding to a stable neutron configuration), and so it may emit an alpha particle (which has 2 neutrons) to form cerium-140 with 82 neutrons.

All of the remaining radioactive isotopes have half-lives that are less than 11 days, and the majority of these have half-lives that are less than 70 seconds. The most stable artificial isotope is <sup>147</sup>Nd, the parent of promethium, with a half-life of 10.98 days. This element also has 15 known meta states with the most stable being <sup>139m</sup>Nd (t<sub>1/2</sub> 5.5 hours), <sup>135m</sup>Nd (t<sub>1/2</sub> 5.5 minutes) and <sup>133m1</sup>Nd (t<sub>1/2</sub> ~70 seconds).

The primary decay modes for isotopes lighter than the lightest and most abundant stable isotope, which is also the only theoretically stable isotope, <sup>142</sup>Nd, are electron capture and positron decay, and the primary mode for heavier radioisotopes is beta decay. The primary decay products for lighter radioisotopes are praseodymium isotopes and the primary products for heavier ones are promethium isotopes.

Neodymium isotopes as fission products

Neodymium is one of the more common fission products that results from the splitting of uranium-233, uranium-235, plutonium-239 and plutonium-241. The distribution of resulting neodymium isotopes is distinctly different than those found in crustal rock formation on Earth. One of the methods used to verify that the Oklo Fossil Reactors in Gabon had produced a natural nuclear fission reactor some two billion years before present was to compare the relative abundances of neodymium isotopes found at the reactor site with those found elsewhere on Earth.

List of isotopes

|-id=Neodymium-123 | <sup>123</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 63 | | >310&nbsp;ns | | | | | |-id=Neodymium-124 | <sup>124</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 64 | 123.95187(54)# | 500#&nbsp;ms<br>[>310&nbsp;ns] | | | 0+ | | |-id=Neodymium-125 | rowspan=2|<sup>125</sup>Nd | rowspan=2 style="text-align:right" | 60 | rowspan=2 style="text-align:right" | 65 | rowspan=2|124.94840(43)# | rowspan=2|0.65(15)&nbsp;s | β<sup>+</sup> | <sup>125</sup>Pr | rowspan=2|(5/2)(+#) | rowspan=2| | rowspan=2| |- | β<sup>+</sup>, p (?%) | <sup>124</sup>Ce |-id=Neodymium-126 | <sup>126</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 66 | 125.94269(32)# | 1#&nbsp;s<br />[>310&nbsp;ns] | | | 0+ | | |-id=Neodymium-127 | rowspan=2|<sup>127</sup>Nd | rowspan=2 style="text-align:right" | 60 | rowspan=2 style="text-align:right" | 67 | rowspan=2|126.93998(32)# | rowspan=2|1.8(4)&nbsp;s | β<sup>+</sup> | <sup>127</sup>Pr | rowspan=2|5/2+# | rowspan=2| | rowspan=2| |- | β<sup>+</sup>, p (?%) | <sup>126</sup>Ce |-id=Neodymium-128 | <sup>128</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 68 | 127.93502(22)# | 5#&nbsp;s | | | 0+ | | |-id=Neodymium-129 | rowspan=2|<sup>129</sup>Nd | rowspan=2 style="text-align:right" | 60 | rowspan=2 style="text-align:right" | 69 | rowspan=2|128.93304(22)# | rowspan=2|6.8(6)&nbsp;s | β<sup>+</sup> | <sup>129</sup>Pr | rowspan=2|7/2− | rowspan=2| | rowspan=2| |- | β<sup>+</sup>, p (?%) | <sup>128</sup>Ce |-id=Neodymium-129m1 | rowspan=2 style="text-indent:1em" | <sup>129m1</sup>Nd | rowspan=2 colspan="3" style="text-indent:2em" | 17&nbsp;keV | rowspan=2|2.6(4)&nbsp;s | β<sup>+</sup> | <sup>129</sup>Pr | rowspan=2|1/2+ | rowspan=2| | rowspan=2| |- | β<sup>+</sup>, p (?%) | <sup>128</sup>Ce |-id=Neodymium-129m2 | rowspan=2 style="text-indent:1em" | <sup>129m2</sup>Nd | rowspan=2 colspan="3" style="text-indent:2em" | 39&nbsp;keV | rowspan=2|2.6(4)&nbsp;s | β<sup>+</sup> | <sup>129</sup>Pr | rowspan=2|3/2+ | rowspan=2| | rowspan=2| |- | β<sup>+</sup>, p (?%) | <sup>128</sup>Ce |-id=Neodymium-129m3 | rowspan=2 style="text-indent:1em" | <sup>129m3</sup>Nd | rowspan=2 colspan="3" style="text-indent:2em" | 108&nbsp;keV | rowspan=2| | IT (?%) | <sup>129m2</sup>Nd | rowspan=2|5/2+ | rowspan=2| | rowspan=2| |- | IT (?%) | <sup>129</sup>Nd |-id=Neodymium-129m4 | style="text-indent:1em" | <sup>129m4</sup>Nd | colspan="3" style="text-indent:2em" | 1893&nbsp;keV | | IT | <sup>129</sup>Nd | (17/2+) | | |-id=Neodymium-129m5 | style="text-indent:1em" | <sup>129m5</sup>Nd | colspan="3" style="text-indent:2em" | 2109&nbsp;keV | | IT | <sup>129</sup>Nd | (19/2+) | | |-id=Neodymium-129m6 | style="text-indent:1em" | <sup>129m6</sup>Nd | colspan="3" style="text-indent:2em" | 2284&nbsp;keV | 0.48(4)&nbsp;μs | IT | <sup>129</sup>Nd | (21/2+) | | |-id=Neodymium-130 | <sup>130</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 70 | 129.928506(30) | 21(3)&nbsp;s | β<sup>+</sup> | <sup>130</sup>Pr | 0+ | | |-id=Neodymium-131 | rowspan=2|<sup>131</sup>Nd | rowspan=2 style="text-align:right" | 60 | rowspan=2 style="text-align:right" | 71 | rowspan=2|130.927248(30) | rowspan=2|25.4(9)&nbsp;s | β<sup>+</sup> | <sup>131</sup>Pr | rowspan=2|(5/2+) | rowspan=2| | rowspan=2| |- | β<sup>+</sup>, p (?%) | <sup>130</sup>Ce |-id=Neodymium-132 | <sup>132</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 72 | 131.923321(26) | 1.56(10)&nbsp;min | β<sup>+</sup> | <sup>132</sup>Pr | 0+ | | |-id=Neodymium-133 | <sup>133</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 73 | 132.922348(50) | 70(10)&nbsp;s | β<sup>+</sup> | <sup>133</sup>Pr | (7/2+) | | |-id=Neodymium-133m1 | rowspan=2 style="text-indent:1em" | <sup>133m1</sup>Nd | rowspan=2 colspan="3" style="text-indent:2em" | 127.97(12)&nbsp;keV | rowspan=2|~70&nbsp;s | β<sup>+</sup> (?%) | <sup>133</sup>Pr | rowspan=2|(1/2)+ | rowspan=2| | rowspan=2| |- | IT (?%) | <sup>133</sup>Nd |-id=Neodymium-133m2 | style="text-indent:1em" | <sup>133m2</sup>Nd | colspan="3" style="text-indent:2em" | 176.10(10)&nbsp;keV | 301(18)&nbsp;ns | IT | <sup>133</sup>Nd | (9/2–) | | |-id=Neodymium-134 | <sup>134</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 74 | 133.918790(13) | 8.5(15)&nbsp;min | β<sup>+</sup> | <sup>134</sup>Pr | 0+ | | |-id=Neodymium-134m | style="text-indent:1em" | <sup>134m</sup>Nd | colspan="3" style="text-indent:2em" | 2293.0(4)&nbsp;keV | 389(17)&nbsp;μs | IT | <sup>134</sup>Nd | 8– | | |-id=Neodymium-135 | <sup>135</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 75 | 134.918181(21) | 12.4(6)&nbsp;min | β<sup>+</sup> | <sup>135</sup>Pr | 9/2– | | |-id=Neodymium-135m | style="text-indent:1em" | <sup>135m</sup>Nd | colspan="3" style="text-indent:2em" | 64.95(24)&nbsp;keV | 5.5(5)&nbsp;min | β<sup>+</sup> | <sup>135</sup>Pr | (1/2+) | | |-id=Neodymium-136 | <sup>136</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 76 | 135.914976(13) | 50.65(33)&nbsp;min | β<sup>+</sup> | <sup>136</sup>Pr | 0+ | | |-id=Neodymium-137 | <sup>137</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 77 | 136.914563(13) | 38.5(15)&nbsp;min | β<sup>+</sup> | <sup>137</sup>Pr | 1/2+ | | |-id=Neodymium-137m | style="text-indent:1em" | <sup>137m</sup>Nd | colspan="3" style="text-indent:2em" | 519.43(20)&nbsp;keV | 1.60(15)&nbsp;s | IT | <sup>137</sup>Nd | 11/2– | | |-id=Neodymium-138 | <sup>138</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 78 | 137.911951(12) | 5.04(9)&nbsp;h | β<sup>+</sup> | <sup>138</sup>Pr | 0+ | | |-id=Neodymium-138m | style="text-indent:1em" | <sup>138m</sup>Nd | colspan="3" style="text-indent:2em" | 3174.5(4)&nbsp;keV | 370(5)&nbsp;ns | IT | <sup>138</sup>Nd | 10+ | | |-id=Neodymium-139 | <sup>139</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 79 | 138.911951(30) | 29.7(5)&nbsp;min | β<sup>+</sup> | <sup>139</sup>Pr | 3/2+ | | |-id=Neodymium-139m1 | rowspan=2 style="text-indent:1em" | <sup>139m1</sup>Nd | rowspan=2 colspan="3" style="text-indent:2em" | 231.16(5)&nbsp;keV | rowspan=2|5.50(20)&nbsp;h | β<sup>+</sup> (87.0%) | <sup>139</sup>Pr | rowspan=2|11/2– | rowspan=2| | rowspan=2| |- | IT (13.0%) | <sup>139</sup>Nd |-id=Neodymium-139m2 | style="text-indent:1em" | <sup>139m2</sup>Nd | colspan="3" style="text-indent:2em" | 2616.9(6)&nbsp;keV | 276.8(18)&nbsp;ns | IT | <sup>139</sup>Nd | 23/2 | | |-id=Neodymium-140 | <sup>140</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 80 | 139.9095461(35) | 3.37(2)&nbsp;d | EC | <sup>140</sup>Pr | 0+ | | |-id=Neodymium-140m1 | style="text-indent:1em" | <sup>140m1</sup>Nd | colspan="3" style="text-indent:2em" | 2221.65(9)&nbsp;keV | 600(50)&nbsp;μs | IT | <sup>140</sup>Nd | 7– | | |-id=Neodymium-140m2 | style="text-indent:1em" | <sup>140m2</sup>Nd | colspan="3" style="text-indent:2em" | 7435.1(4)&nbsp;keV | 1.22(6)&nbsp;μs | IT | <sup>140</sup>Nd | 20+ | | |-id=Neodymium-141 | rowspan=2|<sup>141</sup>Nd | rowspan=2 style="text-align:right" | 60 | rowspan=2 style="text-align:right" | 81 | rowspan=2|140.9096167(34) | rowspan=2|2.49(3)&nbsp;h | EC (97.28%) | rowspan=2|<sup>141</sup>Pr | rowspan=2|3/2+ | rowspan=2| | rowspan=2| |- | β<sup>+</sup> (2.72%) |-id=Neodymium-141m | rowspan=2 style="text-indent:1em" | <sup>141m</sup>Nd | rowspan=2 colspan="3" style="text-indent:2em" | 756.51(5)&nbsp;keV | rowspan=2|62.0(8)&nbsp;s | IT (99.97%) | <sup>141</sup>Nd | rowspan=2|11/2– | rowspan=2| | rowspan=2| |- | β<sup>+</sup> (0.032%) | <sup>141</sup>Pr |-id=Neodymium-142 | <sup>142</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 82 | 141.9077288(13) | colspan=3 align=center|Stable | 0+ | 0.27153(40) | |-id=Neodymium-143 | <sup>143</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 83 | 142.9098198(13) | colspan=3 align=center|Observationally Stable | 7/2− | 0.12173(26) | |-id=Neodymium-144 | <sup>144</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 84 | 143.9100928(13) | 2.29(16)×10<sup>15</sup>&nbsp;y | α | <sup>140</sup>Ce | 0+ | 0.23798(19) | |-id=Neodymium-145 | <sup>145</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 85 | 144.9125792(14) | colspan=3 align=center|Observationally Stable | 7/2− | 0.08293(12) | |-id=Neodymium-146 | <sup>146</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 86 | 145.9131225(14) | colspan=3 align=center|Observationally Stable | 0+ | 0.17189(32) | |-id=Neodymium-147 | <sup>147</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 87 | 146.9161060(14) | 10.98(1)&nbsp;d | β<sup>−</sup> | <sup>147</sup>Pm | 5/2− | | |-id=Neodymium-148 | <sup>148</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 88 | 147.9168990(22) | colspan=3 align=center|Observationally Stable | 0+ | 0.05756(21) | |-id=Neodymium-149 | <sup>149</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 89 | 148.9201546(22) | 1.728(1)&nbsp;h | β<sup>−</sup> | <sup>149</sup>Pm | 5/2− | | |-id=Neodymium-150 | <sup>150</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 90 | 149.9209013(12) | 9.3(7)×10<sup>18</sup>&nbsp;y | β<sup>−</sup>β<sup>−</sup> | <sup>150</sup>Sm | 0+ | 0.05638(28) | |-id=Neodymium-151 | <sup>151</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 91 | 150.9238394(12) | 12.44(7)&nbsp;min | β<sup>−</sup> | <sup>151</sup>Pm | 3/2+ | | |-id=Neodymium-152 | <sup>152</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 92 | 151.924691(26) | 11.4(2)&nbsp;min | β<sup>−</sup> | <sup>152</sup>Pm | 0+ | | |-id=Neodymium-153 | <sup>153</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 93 | 152.9277179(29) | 31.6(10)&nbsp;s | β<sup>−</sup> | <sup>153</sup>Pm | (3/2)− | | |-id=Neodymium-153m | style="text-indent:1em" | <sup>153m</sup>Nd | colspan="3" style="text-indent:2em" | 191.71(16)&nbsp;keV | 1.10(4)&nbsp;μs | IT | <sup>153</sup>Nd | (5/2)+ | | |-id=Neodymium-154 | <sup>154</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 94 | 153.9295974(11) | 25.9(2)&nbsp;s | β<sup>−</sup> | <sup>154</sup>Pm | 0+ | | |-id=Neodymium-154m | style="text-indent:1em" | <sup>154m</sup>Nd | colspan="3" style="text-indent:2em" | 1297.9(4)&nbsp;keV | 3.2(3)&nbsp;μs | IT | <sup>154</sup>Nd | (4−) | | |-id=Neodymium-155 | <sup>155</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 95 | 154.9331356(98) | 8.9(2)&nbsp;s | β<sup>−</sup> | <sup>155</sup>Pm | (3/2−) | | |-id=Neodymium-156 | <sup>156</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 96 | 155.9353704(14) | 5.06(13)&nbsp;s | β<sup>−</sup> | <sup>156</sup>Pm | 0+ | | |-id=Neodymium-156m | style="text-indent:1em" | <sup>156m</sup>Nd | colspan="3" style="text-indent:2em" | 1431.3(4)&nbsp;keV | 365(145)&nbsp;ns | IT | <sup>156</sup>Nd | 5− | | |-id=Neodymium-157 | <sup>157</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 97 | 156.9393511(23) | 1.17(4)&nbsp;s | β<sup>−</sup> | <sup>157</sup>Pm | 5/2−# | | |-id=Neodymium-158 | <sup>158</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 98 | 157.9422056(14) | 810(30)&nbsp;ms | β<sup>−</sup> | <sup>158</sup>Pm | 0+ | | |-id=Neodymium-158m | style="text-indent:1em" | <sup>158m</sup>Nd | colspan="3" style="text-indent:2em" | 1648.1(14)&nbsp;keV | 339(20)&nbsp;ns | IT | <sup>158</sup>Nd | (6−) | | |-id=Neodymium-159 | <sup>159</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 99 | 158.946619(32) | 500(30)&nbsp;ms | β<sup>−</sup> | <sup>159</sup>Pm | 7/2+# | | |-id=Neodymium-160 | <sup>160</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 100 | 159.949839(50) | 439(37)&nbsp;ms | β<sup>−</sup> | <sup>160</sup>Pm | 0+ | | |-id=Neodymium-160m | style="text-indent:1em" | <sup>160m</sup>Nd | colspan="3" style="text-indent:2em" | 1107.9(9)&nbsp;keV | 1.63(21)&nbsp;μs | IT | <sup>160</sup>Nd | (4−) | | |-id=Neodymium-161 | <sup>161</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 101 | 160.95466(43)# | 215(76)&nbsp;ms | β<sup>−</sup> | <sup>161</sup>Pm | 1/2−# | | |-id=Neodymium-162 | <sup>162</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 102 | 161.95812(43)# | 310(200)&nbsp;ms | β<sup>−</sup> | <sup>162</sup>Pm | 0+ | | |-id=Neodymium-163 | <sup>163</sup>Nd | style="text-align:right" | 60 | style="text-align:right" | 103 | 162.96341(54)# | 80#&nbsp;ms<br />[>550&nbsp;ns] | | | 5/2−# | |

See also

Daughter products other than neodymium

References

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