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Isotopes of protactinium

Protactinium (<sub>91</sub>Pa) has no stable isotopes. As <sup>231</sup>Pa occurs in usable quantity, and comprises virtually all of the element, it defines the standard atomic weight.

Thirty radioisotopes of protactinium have been characterized, ranging from <sup>210</sup>Pa to <sup>239</sup>Pa. The most stable isotopes are <sup>231</sup>Pa with a half-life of 32,700 years, <sup>233</sup>Pa with a half-life of 26.975 days, and <sup>230</sup>Pa with a half-life of 17.4 days. All of the remaining radioactive isotopes have half-lives less than 1.6 days, and the majority of these have half-lives less than 1.8 seconds. This element also has five meta states, <sup>217m</sup>Pa (t<sub>1/2</sub> 1.15 milliseconds), <sup>220m1</sup>Pa (t<sub>1/2</sub>&nbsp;= 308 nanoseconds), <sup>220m2</sup>Pa (t<sub>1/2</sub>&nbsp;= 69 nanoseconds), <sup>229m</sup>Pa (t<sub>1/2</sub>&nbsp;= 420 nanoseconds), and <sup>234m</sup>Pa (t<sub>1/2</sub>&nbsp;= 1.16 minutes).

The only naturally occurring isotopes are <sup>231</sup>Pa, <sup>233</sup>Pa, <sup>234</sup>Pa, and <sup>234m</sup>Pa. The first occurs as an intermediate decay product of <sup>235</sup>U, the second of (rare) <sup>237</sup>Np, and the last two as intermediate decay products of <sup>238</sup>U. <sup>231</sup>Pa dominates solely because of its longer life.

The primary decay mode for isotopes of Pa lighter than (and including) the most stable isotope <sup>231</sup>Pa is alpha decay to isotopes of actinium, except <sup>228</sup>Pa to <sup>230</sup>Pa, which primarily decay by electron capture to isotopes of thorium. The primary mode for the heavier isotopes is beta minus (β<sup>−</sup>) decay to isotopes of uranium.

List of isotopes

|-id=Protactinium-210 | <sup>210</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 119 | | | α | <sup>206</sup>Ac | 3+ | |-id=Protactinium-211 | <sup>211</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 120 | 211.023674(75) | 6(3)&nbsp;ms | α | <sup>207</sup>Ac | 9/2− | |-id=Protactinium-212 | <sup>212</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 121 | 212.023185(94) | 5.8(19)&nbsp;ms | α | <sup>208</sup>Ac | 3+# | |-id=Protactinium-213 | <sup>213</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 122 | 213.021100(61) | 7.4(24)&nbsp;ms | α | <sup>209</sup>Ac | 9/2− | |-id=Protactinium-214 | <sup>214</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 123 | 214.020891(87) | 17(3)&nbsp;ms | α | <sup>210</sup>Ac | 7+# | |-id=Protactinium-215 | <sup>215</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 124 | 215.019114(89) | 14(2)&nbsp;ms | α | <sup>211</sup>Ac | 9/2− | |-id=Protactinium-216 | <sup>216</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 125 | 216.019135(26) | 105(12)&nbsp;ms | α | <sup>212</sup>Ac | 5+# | |-id=Protactinium-217 | <sup>217</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 126 | 217.018309(13) | 3.8(2)&nbsp;ms | α | <sup>213</sup>Ac | 9/2− | |-id=Protactinium-217m | rowspan=2 style="text-indent:1em" | <sup>217m</sup>Pa | rowspan=2| | rowspan=2 colspan="3" style="text-indent:2em" | 1860(7)&nbsp;keV | rowspan=2|1.08(3)&nbsp;ms | α (73%) | <sup>213</sup>Ac | rowspan=2|(23/2−) | rowspan=2| |- | IT (27%) | <sup>217</sup>Pa |-id=Protactinium-218 | <sup>218</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 127 | 218.020021(19) | 108(5)&nbsp;μs | α | <sup>214</sup>Ac | 8−# | |-id=Protactinium-218m | style="text-indent:1em" | <sup>218m</sup>Pa | | colspan="3" style="text-indent:2em" | 81(19)&nbsp;keV | 150(50)&nbsp;μs | α | <sup>214</sup>Ac | | |-id=Protactinium-219 | <sup>219</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 128 | 219.019950(75) | 56(9)&nbsp;ns | α | <sup>215</sup>Ac | 9/2− | |-id=Protactinium-220 | <sup>220</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 129 | 220.021770(16) | 850(60)&nbsp;ns | α | <sup>216</sup>Ac | 1−# | |-id=Protactinium-220m1 | style="text-indent:1em" | <sup>220m1</sup>Pa | | colspan="3" style="text-indent:2em" | 26(23)&nbsp;keV | 410(180)&nbsp;ns | α | <sup>216</sup>Ac | | |-id=Protactinium-220m2 | style="text-indent:1em" | <sup>220m2</sup>Pa | | colspan="3" style="text-indent:2em" | 290(50)&nbsp;keV | 260(210)&nbsp;ns | α | <sup>216</sup>Ac | | |-id=Protactinium-221 | <sup>221</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 130 | 221.021873(64) | 5.9(17)&nbsp;μs | α | <sup>217</sup>Ac | 9/2− | |-id=Protactinium-222 | <sup>222</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 131 | 222.023687(93) | 3.8(2)&nbsp;ms | α | <sup>218</sup>Ac | 1−# | |-id=Protactinium-223 | <sup>223</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 132 | 223.023980(81) | 5.3(3)&nbsp;ms | α | <sup>219</sup>Ac | 9/2− | |-id=Protactinium-224 | <sup>224</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 133 | 224.0256173(81) | 844(19)&nbsp;ms | α | <sup>220</sup>Ac | (5−) | |-id=Protactinium-225 | <sup>225</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 134 | 225.026148(88) | 1.71(10)&nbsp;s | α | <sup>221</sup>Ac | 5/2−# | |-id=Protactinium-226 | rowspan=2|<sup>226</sup>Pa | rowspan=2| | rowspan=2 style="text-align:right" | 91 | rowspan=2 style="text-align:right" | 135 | rowspan=2|226.027948(12) | rowspan=2|1.8(2)&nbsp;min | α (74%) | <sup>222</sup>Ac | rowspan=2|1−# | rowspan=2| |- | β<sup>+</sup> (26%) | <sup>226</sup>Th |-id=Protactinium-227 | rowspan=2|<sup>227</sup>Pa | rowspan=2| | rowspan=2 style="text-align:right" | 91 | rowspan=2 style="text-align:right" | 136 | rowspan=2|227.0288036(78) | rowspan=2|38.3(3)&nbsp;min | α (85%) | <sup>223</sup>Ac | rowspan=2|(5/2−) | rowspan=2| |- | EC (15%) | <sup>227</sup>Th |-id=Protactinium-228 | rowspan=2|<sup>228</sup>Pa | rowspan=2| | rowspan=2 style="text-align:right" | 91 | rowspan=2 style="text-align:right" | 137 | rowspan=2|228.0310508(47) | rowspan=2|22(1)&nbsp;h | β<sup>+</sup> (98.15%) | <sup>228</sup>Th | rowspan=2|3+ | rowspan=2| |- | α (1.85%) | <sup>224</sup>Ac |-id=Protactinium-229 | rowspan=2|<sup>229</sup>Pa | rowspan=2| | rowspan=2 style="text-align:right" | 91 | rowspan=2 style="text-align:right" | 138 | rowspan=2|229.0320956(35) | rowspan=2|1.55(4)&nbsp;d | EC (99.51%) | <sup>229</sup>Th | rowspan=2|5/2+ | rowspan=2| |- | α (0.49%) | <sup>225</sup>Ac |-id=Protactinium-229m | style="text-indent:1em" | <sup>229m</sup>Pa | | colspan="3" style="text-indent:2em" | 12.20(4)&nbsp;keV | 420(30)&nbsp;ns | IT | <sup>229</sup>Pa | 3/2− | |- | rowspan=3|<sup>230</sup>Pa | rowspan=3| | rowspan=3 style="text-align:right" | 91 | rowspan=3 style="text-align:right" | 139 | rowspan=3|230.0345397(33) | rowspan=3|17.4(5)&nbsp;d | β<sup>+</sup> (92.2%) | <sup>230</sup>Th | rowspan=3|2− | rowspan=3| |- | β<sup>−</sup> (7.8%) | <sup>230</sup>U |- | α (0.0032%) | <sup>226</sup>Ac |- | rowspan=4|<sup>231</sup>Pa | rowspan=4|Protoactinium<br/>Protactinium | rowspan=4 style="text-align:right" | 91 | rowspan=4 style="text-align:right" | 140 | rowspan=4|231.0358825(19) | rowspan=4|3.265(20)×10<sup>4</sup>&nbsp;y | α | <sup>227</sup>Ac | rowspan=4|3/2− | rowspan=4|1.0000 |- | CD (1.34×10<sup>−9</sup>%) | <sup>207</sup>Tl<br /><sup>24</sup>Ne |- | SF (<3×10<sup>−10</sup>%) | (various) |- | CD (~10<sup>−12</sup>%) | <sup>208</sup>Pb<br /><sup>23</sup>F |-id=Protactinium-232 | <sup>232</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 141 | 232.0385902(82) | 1.32(2)&nbsp;d | β<sup>−</sup> | <sup>232</sup>U | (2−) | |- | <sup>233</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 142 | 233.0402465(14) | 26.975(13)&nbsp;d | β<sup>−</sup> | <sup>233</sup>U | 3/2− | Trace |- | <sup>234</sup>Pa | Uranium Z | style="text-align:right" | 91 | style="text-align:right" | 143 | 234.0433056(44) | 6.70(5)&nbsp;h | β<sup>−</sup> | <sup>234</sup>U | 4+ | Trace |- | rowspan=2 style="text-indent:1em" | <sup>234m</sup>Pa | rowspan=2|Uranium X<sub>2</sub><br />Brevium | rowspan=2 colspan="3" style="text-indent:2em" | 79(3)&nbsp;keV | rowspan=2|1.159(11)&nbsp;min | β<sup>−</sup> (99.84%) | <sup>234</sup>U | rowspan=2|(0−) | rowspan=2|Trace |- | IT (0.16%) | <sup>234</sup>Pa |-id=Protactinium-235 | <sup>235</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 144 | 235.045399(15) | 24.4(2)&nbsp;min | β<sup>−</sup> | <sup>235</sup>U | 3/2− | |-id=Protactinium-236 | rowspan=2|<sup>236</sup>Pa | rowspan=2| | rowspan=2 style="text-align:right" | 91 | rowspan=2 style="text-align:right" | 145 | rowspan=2|236.048668(15) | rowspan=2|9.1(1)&nbsp;min | β<sup>−</sup> | <sup>236</sup>U | rowspan=2|1(−) | rowspan=2| |- | β<sup>−</sup>, SF (6×10<sup>−8</sup>%) | (various) |-id=Protactinium-237 | <sup>237</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 146 | 237.051023(14) | 8.7(2)&nbsp;min | β<sup>−</sup> | <sup>237</sup>U | 1/2+ | |-id=Protactinium-238 | rowspan=2|<sup>238</sup>Pa | rowspan=2| | rowspan=2 style="text-align:right" | 91 | rowspan=2 style="text-align:right" | 147 | rowspan=2|238.054637(17) | rowspan=2|2.28(9)&nbsp;min | β<sup>−</sup> | <sup>238</sup>U | rowspan=2|3−# | rowspan=2| |- | β<sup>−</sup>, SF (2.6×10<sup>−6</sup>%) | (various) |-id=Protactinium-239 | <sup>239</sup>Pa | | style="text-align:right" | 91 | style="text-align:right" | 148 | 239.05726(21)# | 1.8(5)&nbsp;h | β<sup>−</sup> | <sup>239</sup>U | 1/2+# |

Actinides and fission products

Protactinium-230

Protactinium-230 has 139 neutrons and a half-life of 17.4 days. Most of the time (92%), it undergoes beta plus decay to <sup>230</sup>Th, with a smaller (8%) beta-minus decay branch leading to <sup>230</sup>U. It also has a very rare (0.0032%) alpha decay mode leading to <sup>226</sup>Ac. It is not found in nature because its half-life is short and it is not found in the decay chains of <sup>235</sup>U, <sup>238</sup>U, or <sup>232</sup>Th.

Protactinium-230 is of interest as a progenitor of uranium-230, an isotope that has been considered for use in targeted alpha-particle therapy (TAT). It can be produced through proton or deuteron irradiation of natural thorium.

Protactinium-231

Protactinium-231 is the longest-lived isotope of protactinium, with a half-life of 32,760 years. In nature, it is found in trace amounts as part of the actinium series, which starts with the primordial isotope uranium-235; the equilibrium concentration in uranium ore is 46.5 atoms of <sup>231</sup>Pa per million of <sup>235</sup>U. In nuclear reactors, it is one of the few long-lived radioactive actinides produced as a byproduct of the projected thorium fuel cycle, as a result of (n,2n) reactions where a fast neutron removes a neutron from <sup>232</sup>Th or <sup>232</sup>U, and can also be destroyed by neutron capture, though the cross section for this reaction is also low.

binding energy: 1759860&nbsp;keV<br /> beta decay energy: −382&nbsp;keV

spin: 3/2−<br /> mode of decay: alpha to <sup>227</sup>Ac, also others

possible parent nuclides: beta from <sup>231</sup>Th, EC from <sup>231</sup>U, alpha from <sup>235</sup>Np.

Protactinium-233

Protactinium-233 is also part of the thorium fuel cycle. It is an intermediate beta decay product between thorium-233 (produced from natural thorium-232 by neutron capture) and uranium-233 (the fissile fuel of the thorium cycle). Some thorium-cycle reactor designs try to protect Pa-233 from further neutron capture producing Pa-234 and U-234, which are not useful as fuel.

Protactinium-234

Protactinium-234 is a member of the uranium series with a half-life of 6.70 hours. It was discovered by Otto Hahn in 1921.

Protactinium-234m

Protactinium-234m is a member of the uranium series with a half-life of 1.17 minutes. It was discovered in 1913 by Kazimierz Fajans and Oswald Helmuth Göhring, who named it brevium for its short half-life. It is now believed that all decays of the parent thorium-234 produce this isomer and the ground state is observed because of (invisible) IT decay. Protactinium-234m has the same mass (same number of protons and neutrons) as Protactinium-234, the difference merely visible in their non-identical half-life, with Protactinium-234m having a noticeably shorter lifespan. This phenomenon is called nuclear isomerism.

References

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