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| Standard atomic weightAr°(Pa) | ||||||||||||||||||||||||||||||||||||||||||||||||||||
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Protactinium (91Pa) has no stableisotopes. As231Pa occurs in usable quantity, and comprises virtually all of the element, it defines the standard atomic weight.
Thirtyradioisotopes of protactinium have been characterized, ranging from210Pa to239Pa. The most stable isotopes are231Pa with ahalf-life of 32,700 years,233Pa with a half-life of 26.975 days, and230Pa with a half-life of 17.4 days. All of the remainingradioactive 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 fivemeta states,217mPa (t1/2 1.15 milliseconds),220m1Pa (t1/2 = 308 nanoseconds),220m2Pa (t1/2 = 69 nanoseconds),229mPa (t1/2 = 420 nanoseconds), and234mPa (t1/2 = 1.16 minutes).
The only naturally occurring isotopes are231Pa,233Pa,234Pa, and234mPa. The first occurs as an intermediate decay product of235U, the second of (rare)237Np, and the last two as intermediate decay products of238U.231Pa dominates solely because of its longer life.
The primarydecay mode for isotopes of Pa lighter than (and including) the most stable isotope231Pa isalpha decay toisotopes of actinium, except228Pa to230Pa, which primarily decay by electron capture toisotopes of thorium. The primary mode for the heavier isotopes isbeta minus (β−) decay toisotopes of uranium.
| Nuclide [n 1] | Historic name | Z | N | Isotopic mass(Da)[4] [n 2][n 3] | Half-life[1] [n 4] | Decay mode[1] [n 5] | Daughter isotope [n 6] | Spin and parity[1] [n 7][n 4] | Isotopic abundance | ||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Excitation energy | |||||||||||||||||||
| 210Pa[5] | 91 | 119 | 6.0+1.5 −1.1 ms | α | 206Ac | 3+ | |||||||||||||
| 211Pa | 91 | 120 | 211.023674(75) | 6(3) ms | α | 207Ac | 9/2− | ||||||||||||
| 212Pa | 91 | 121 | 212.023185(94) | 5.8(19) ms | α | 208Ac | 3+# | ||||||||||||
| 213Pa | 91 | 122 | 213.021100(61) | 7.4(24) ms | α | 209Ac | 9/2− | ||||||||||||
| 214Pa | 91 | 123 | 214.020891(87) | 17(3) ms | α | 210Ac | 7+# | ||||||||||||
| 215Pa | 91 | 124 | 215.019114(89) | 14(2) ms | α | 211Ac | 9/2− | ||||||||||||
| 216Pa | 91 | 125 | 216.019135(26) | 105(12) ms | α | 212Ac | 5+# | ||||||||||||
| 217Pa | 91 | 126 | 217.018309(13) | 3.8(2) ms | α | 213Ac | 9/2− | ||||||||||||
| 217mPa | 1860(7) keV | 1.08(3) ms | α (73%) | 213Ac | (23/2−) | ||||||||||||||
| IT (27%) | 217Pa | ||||||||||||||||||
| 218Pa | 91 | 127 | 218.020021(19) | 108(5) μs | α | 214Ac | 8−# | ||||||||||||
| 218mPa | 81(19) keV | 150(50) μs | α | 214Ac | |||||||||||||||
| 219Pa | 91 | 128 | 219.019950(75) | 56(9) ns | α | 215Ac | 9/2− | ||||||||||||
| 220Pa | 91 | 129 | 220.021770(16) | 850(60) ns | α | 216Ac | 1−# | ||||||||||||
| 220m1Pa[n 8] | 26(23) keV | 410(180) ns | α | 216Ac | |||||||||||||||
| 220m2Pa | 290(50) keV | 260(210) ns | α | 216Ac | |||||||||||||||
| 221Pa | 91 | 130 | 221.021873(64) | 5.9(17) μs | α | 217Ac | 9/2− | ||||||||||||
| 222Pa | 91 | 131 | 222.023687(93) | 3.8(2) ms | α | 218Ac | 1−# | ||||||||||||
| 223Pa | 91 | 132 | 223.023980(81) | 5.3(3) ms | α | 219Ac | 9/2− | ||||||||||||
| 224Pa | 91 | 133 | 224.0256173(81) | 844(19) ms | α | 220Ac | (5−) | ||||||||||||
| 225Pa | 91 | 134 | 225.026148(88) | 1.71(10) s | α | 221Ac | 5/2−# | ||||||||||||
| 226Pa | 91 | 135 | 226.027948(12) | 1.8(2) min | α (74%) | 222Ac | 1−# | ||||||||||||
| β+ (26%) | 226Th | ||||||||||||||||||
| 227Pa | 91 | 136 | 227.0288036(78) | 38.3(3) min | α (85%) | 223Ac | (5/2−) | ||||||||||||
| EC (15%) | 227Th | ||||||||||||||||||
| 228Pa | 91 | 137 | 228.0310508(47) | 22(1) h | β+ (98.15%) | 228Th | 3+ | ||||||||||||
| α (1.85%) | 224Ac | ||||||||||||||||||
| 229Pa | 91 | 138 | 229.0320956(35) | 1.55(4) d | EC (99.51%) | 229Th | 5/2+ | ||||||||||||
| α (0.49%) | 225Ac | ||||||||||||||||||
| 229mPa | 12.20(4) keV | 420(30) ns | IT | 229Pa | 3/2− | ||||||||||||||
| 230Pa | 91 | 139 | 230.0345397(33) | 17.4(5) d | β+ (92.2%) | 230Th | 2− | ||||||||||||
| β− (7.8%) | 230U | ||||||||||||||||||
| α (0.0032%) | 226Ac | ||||||||||||||||||
| 231Pa | Protoactinium Protactinium[n 9] | 91 | 140 | 231.0358825(19) | 3.265(20)×104 y | α | 227Ac | 3/2− | 1.0000[n 10] | ||||||||||
| CD (1.34×10−9%) | 207Tl 24Ne | ||||||||||||||||||
| SF (<3×10−10%) | (various) | ||||||||||||||||||
| CD (~10−12%)[6] | 208Pb 23F | ||||||||||||||||||
| 232Pa | 91 | 141 | 232.0385902(82) | 1.32(2) d | β− | 232U | (2−) | ||||||||||||
| 233Pa | 91 | 142 | 233.0402465(14) | 26.975(13) d | β− | 233U | 3/2− | Trace[n 11] | |||||||||||
| 234Pa | Uranium Z | 91 | 143 | 234.0433056(44) | 6.70(5) h | β− | 234U | 4+ | Trace[n 12] | ||||||||||
| 234mPa | Uranium X2 Brevium | 79(3) keV | 1.159(11) min | β− (99.84%) | 234U | (0−) | Trace[n 12] | ||||||||||||
| IT (0.16%) | 234Pa | ||||||||||||||||||
| 235Pa | 91 | 144 | 235.045399(15) | 24.4(2) min | β− | 235U | 3/2− | ||||||||||||
| 236Pa | 91 | 145 | 236.048668(15) | 9.1(1) min | β− | 236U | 1(−) | ||||||||||||
| β−, SF (6×10−8%) | (various) | ||||||||||||||||||
| 237Pa | 91 | 146 | 237.051023(14) | 8.7(2) min | β− | 237U | 1/2+ | ||||||||||||
| 238Pa | 91 | 147 | 238.054637(17) | 2.28(9) min | β− | 238U | 3−# | ||||||||||||
| β−, SF (2.6×10−6%) | (various) | ||||||||||||||||||
| 239Pa | 91 | 148 | 239.05726(21)# | 1.8(5) h | β− | 239U | 1/2+# | ||||||||||||
| This table header & footer: | |||||||||||||||||||
| EC: | Electron capture |
| CD: | Cluster decay |
| IT: | Isomeric transition |
| SF: | Spontaneous fission |
Protactinium-230 has 139neutrons and a half-life of 17.4 days. Most of the time (92%), it undergoes beta plus decay to230Th, with a smaller (8%) beta-minus decay branch leading to230U. It also has a very rare (0.0032%) alpha decay mode leading to226Ac. It is not found in nature because its half-life is short and it is not found in thedecay chains of235U,238U, or232Th.
Protactinium-230 is of interest as a progenitor of uranium-230, an isotope that has been considered for use intargeted alpha-particle therapy (TAT). It can be produced through proton ordeuteron irradiation of natural thorium.[7]
Protactinium-231 is the longest-lived isotope of protactinium,[8] with a half-life of 32,760 years.[9][10] In nature, it is found in trace amounts as part of theactinium series,[10][11] which starts with theprimordial isotopeuranium-235;[12] theequilibrium concentration in uranium ore is 46.5 atoms of231Pa per million of235U. Innuclear reactors, it is one of the few long-lived radioactiveactinides produced as a byproduct of the projectedthorium fuel cycle,[13] as a result of (n,2n) reactions where afast neutron removes aneutron from232Th or232U, and can also be destroyed byneutron capture, though thecross section for this reaction is also low.

binding energy: 1759860 keV
beta decay energy: −382 keV
spin: 3/2−
mode of decay:alpha to227Ac, also others
possible parent nuclides:beta from231Th,EC from231U,alpha from235Np.
Protactinium-233 is also part of the thorium fuel cycle. It is an intermediate beta decay product betweenthorium-233 (produced from natural thorium-232 by neutron capture) anduranium-233 (the fissile fuel of the thorium cycle).[14] 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 is a member of theuranium series with a half-life of 6.70 hours. It was discovered byOtto Hahn in 1921.[15]
Protactinium-234m is a member of the uranium series with a half-life of 1.17 minutes. It was discovered in 1913 byKazimierz Fajans andOswald Helmuth Göhring, who named itbrevium for its short half-life.[16] It is now believed that all decays of the parentthorium-234 produce this isomer[17] 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 callednuclear isomerism.[18]