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Thorium's Atomic Tapestry

A comprehensive exploration into the fascinating world of Thorium's isotopes, their properties, and their profound implications.

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Introduction to Thorium Isotopes

Natural Occurrence

Thorium (90Th) is an element characterized by its naturally occurring isotopes. While it possesses seven naturally occurring isotopes, none are stable. A key isotope, 232Th, stands out with a remarkably long half-life of 1.40ร—1010 years, significantly exceeding the age of the Earth and even the estimated age of the universe. This extended stability means 232Th constitutes nearly all natural thorium, historically leading to its classification as a mononuclidic element.

Reclassification and Abundance

However, in 2013, the International Union of Pure and Applied Chemistry (IUPAC) reclassified thorium as binuclidic. This change was prompted by the discovery of significant quantities of 230Th in deep seawater. Thorium exhibits a characteristic terrestrial isotopic composition, allowing for the definition of a standard atomic weight.

Radioisotopes and Stability

Beyond the naturally abundant isotopes, thirty-one radioisotopes of thorium have been identified and characterized. Among these, 232Th, 230Th (with a half-life of 75,400 years), 229Th (7,916 years), and 228Th (1.91 years) are the most stable. The remaining radioactive isotopes possess half-lives of less than thirty days, with many decaying in mere minutes.

Comprehensive Isotope Data

Isotope Inventory

The following table provides a detailed overview of Thorium's isotopes, including their mass number, historical names, atomic and neutron counts, isotopic mass, half-life, decay modes, daughter products, nuclear spin, parity, and natural abundance where applicable.

Isotopes of Thorium (90Th)
Main isotopes[1] Decay
Isotope abun­dance half-life (t1/2) mode pro­duct
227Th trace 18.693 d ฮฑ 223Ra
228Th trace 1.9125 y ฮฑ 224Ra
229Th trace 7916 y ฮฑ 225Ra
230Th 0.02% 75400 y ฮฑ 226Ra
231Th trace 25.52 h ฮฒ- 231Pa
232Th 100.0% 1.40ร—1010 y ฮฑ 228Ra
233Th trace 21.83 min ฮฒ- 233Pa
234Th trace 24.11 d ฮฒ- 234Pa
Standard atomic weight Arยฐ(Th)
  • 232.0377ยฑ0.0004[2]
  • 232.04ยฑ0.01 (abridged)[3]
Nuclide
[n 1]
Historic
name
Z N Isotopic mass (Da)[11]
[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 8]
Natural abundance
Excitation energy Normal proportion[1] Range of variation
207Th[10] 90 117 9.7+46.6
โˆ’4.4
 ms
ฮฑ 203Ra
208Th 90 118 208.017915(34) 2.4(12) ms ฮฑ 204Ra 0+
209Th 90 119 209.017998(27) 3.1(12) ms ฮฑ 205Ra 13/2+
210Th 90 120 210.015094(20) 16.0(36) ms ฮฑ 206Ra 0+
211Th 90 121 211.014897(92) 48(20) ms ฮฑ 207Ra 5/2โˆ’#
212Th 90 122 212.013002(11) 31.7(13) ms ฮฑ 208Ra 0+
213Th 90 123 213.0130115(99) 144(21) ms ฮฑ 209Ra 5/2โˆ’
213mTh 1180.0(14) keV 1.4(4) ฮผs IT 213Th (13/2)+
214Th 90 124 214.011481(11) 87(10) ms ฮฑ 210Ra 0+
214mTh 2181.0(27) keV 1.24(12) ฮผs IT 214Th 8+#
215Th 90 125 215.0117246(68) 1.35(14) s ฮฑ 211Ra (1/2โˆ’)
215mTh 1471(50)# keV 770(60) ns IT 215Th 9/2+#
216Th 90 126 216.011056(12) 26.28(16) ms ฮฑ 212Ra 0+
216m1Th 2041(8) keV 135.4(29) ฮผs IT (97.2%) 216Th 8+
ฮฑ (2.8%) 212Ra
216m2Th 2648(8) keV 580(26) ns IT 216Th (11โˆ’)
216m3Th 3682(8) keV 740(70) ns IT 216Th (14+)
217Th 90 127 217.013103(11) 248(4) ฮผs ฮฑ 213Ra 9/2+#
217m1Th 673.3(1) keV 141(50) ns IT 217Th (15/2โˆ’)
217m2Th 2307(32) keV 71(14) ฮผs IT 217Th (25/2+)
218Th 90 128 218.013276(11) 122(5) ns ฮฑ 214Ra 0+
219Th 90 129 219.015526(61) 1.023(18) ฮผs ฮฑ 215Ra 9/2+#
220Th 90 130 220.015770(15) 10.2(3) ฮผs ฮฑ 216Ra 0+
221Th 90 131 221.0181858(86) 1.75(2) ms ฮฑ 217Ra 7/2+#
222Th 90 132 222.018468(11) 2.24(3) ms ฮฑ 218Ra 0+
223Th 90 133 223.0208111(85) 0.60(2) s ฮฑ 219Ra (5/2)+
224Th 90 134 224.021466(10) 1.04(2) s ฮฑ[n 9] 220Ra 0+
225Th 90 135 225.0239510(55) 8.75(4) min ฮฑ (~90%) 221Ra 3/2+
EC (~10%) 225Ac
226Th 90 136 226.0249037(48) 30.70(3) min ฮฑ 222Ra 0+
CD (<3.2ร—10โˆ’12%) 208Pb
18O
227Th Radioactinium 90 137 227.0277025(22) 18.693(4) d ฮฑ 223Ra (1/2+) Trace[n 10]
228Th Radiothorium 90 138 228.0287397(19) 1.9125(7) y ฮฑ 224Ra 0+ Trace[n 11]
CD (1.13ร—10โˆ’11%) 208Pb
20O
229Th 90 139 229.0317614(26) 7916(17) y ฮฑ 225Ra 5/2+ Trace[n 12]
229mTh 8.355733554021(8) eV[6] 7(1) ฮผs[12] IT[n 13] 229Th+ 3/2+
229mTh+ 8.355733554021(8) eV[6] 29(1) min[13] ฮณ[n 13] 229Th+ 3/2+
230Th[n 14] Ionium 90 140 230.0331323(13) 7.54(3)ร—104 y ฮฑ 226Ra 0+ 0.0002(2)[n 15]
CD (5.8ร—10โˆ’11%) 206Hg
24Ne
SF (<4ร—10โˆ’12%) (various)
231Th Uranium Y 90 141 231.0363028(13) 25.52(1) h ฮฒโˆ’ 231Pa 5/2+ Trace[n 10]
232Th[n 16] Thorium 90 142 232.0380536(15) 1.40(1)ร—1010 y ฮฑ[n 17] 228Ra 0+ 0.9998(2)
SF (1.1 ร— 10โˆ’9%) (various)
CD (<2.78ร—10โˆ’10%) 208,206Hg
24,26Ne
233Th 90 143 233.0415801(15) 21.83(4) min ฮฒโˆ’ 233Pa 1/2+ Trace[n 18]
234Th Uranium X1 90 144 234.0435998(28) 24.107(24) d ฮฒโˆ’ 234mPa[14] 0+ Trace[n 15]
235Th 90 145 235.047255(14) 7.2(1) min ฮฒโˆ’ 235Pa 1/2+#
236Th 90 146 236.049657(15) 37.3(15) min ฮฒโˆ’ 236Pa 0+
237Th 90 147 237.053629(17) 4.8(5) min ฮฒโˆ’ 237Pa 5/2+#
238Th 90 148 238.05639(30)# 9.4(20) min ฮฒโˆ’ 238Pa 0+
This table header & footer:
  1. ^ mTh โ€“  Excited nuclear isomer.
  2. ^ ( ) โ€“  Uncertainty (1ฯƒ) is given in concise form in parentheses after the corresponding last digits.
  3. ^ # โ€“  Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  4. ^ Bold half-life โ€“  nearly stable, half-life longer than age of universe.
  5. ^ Modes of decay:
  6. ^ Bold symbol as daughter โ€“  Daughter product is stable.
  7. ^ ( ) spin value โ€“  Indicates spin with weak assignment arguments.
  8. ^ # โ€“  Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  9. ^ Theorized to also undergo ฮฒ+ฮฒ+ decay to 224Ra
  10. ^ a b Intermediate decay product of 235U
  11. ^ Intermediate decay product of 232Th
  12. ^ Intermediate decay product of 237Np
  13. ^ a b Neutral 229mTh decays rapidly by internal conversion, ejecting an electron. There is not enough energy to eject a second electron, so 229mTh+ ions live much longer, decaying by gamma emission. See ยง Thorium-229m.
  14. ^ Used in uraniumโ€“thorium dating
  15. ^ a b Intermediate decay product of 238U

Notable Thorium Isotopes

Thorium-228 (Radiothorium)

228Th is an isotope of thorium with 138 neutrons. It is part of the decay chain of 232Th, historically earning it the name Radiothorium. With a half-life of 1.9125 years, it primarily decays via alpha emission to 224Ra. Unusually, it can also undergo cluster decay, emitting a 20O nucleus and producing stable 208Pb. 228Th is a daughter isotope of 232U and contributes significantly to its radiological hazard. It finds application in alpha particle radiation therapy, often in conjunction with its decay product 224Ra.

Thorium-229

229Th is a radioactive isotope of thorium that decays via alpha emission with a half-life of 7916 years. It is generated from the decay of uranium-233 and is crucial for producing medical isotopes like actinium-225 and bismuth-213. A unique characteristic of 229Th is its nuclear isomer, 229mTh, which possesses an exceptionally low excitation energy (around 8.3 eV). This property has spurred research into developing highly accurate nuclear clocks and exploring quantum computing applications, though precise measurements of its transition energy have been a long-standing challenge.

Thorium-230 (Ionium)

230Th is a radioactive isotope of thorium utilized in dating methods such as uranium-thorium dating for corals and determining ocean current flux. Historically known as Ionium (Io), this isotope is produced in the decay chain of uranium-238. The name "Ionium" persists in the ionium-thorium dating technique. Its presence in deep seawater led to the reclassification of thorium as binuclidic.

Thorium-232

232Th is the sole primordial nuclide of thorium, making up virtually all natural thorium. Its alpha decay half-life of 1.40ร—1010 years is longer than the age of the Earth. It initiates the thorium series decay chain, ultimately leading to stable lead-208. The longest-lived intermediates in this chain are radium-228 (5.75 years) and thorium-228 (1.91 years). 232Th is a fertile material, capable of absorbing neutrons to transmute into the fissile nuclide uranium-233, forming the basis of the thorium fuel cycle. Historically used in Thorotrast, a thorium dioxide suspension, as an X-ray contrast medium, it is now classified as carcinogenic.

Applications and Significance

Nuclear Energy

Thorium, particularly the isotope 232Th, is a key component in the proposed thorium fuel cycle. It acts as a fertile material, capable of absorbing neutrons to produce fissile uranium-233. This cycle offers potential advantages in nuclear power generation, including reduced long-lived waste and improved safety characteristics.

Industrial and Scientific Uses

Thorium compounds have found use in various industrial applications. Thorium dioxide (ThO2) was historically employed in gas mantles for lamps, providing intense light upon incandescence. It also served as a cathode material in vacuum tubes due to its thermal stability and low work function for electron emission. Certain specialized lenses, like Kodak's Aero-Ektar, utilized thorium-containing glass for its high refractive index and low dispersion properties, though these lenses exhibit mild radioactivity.

Medical and Research Applications

Specific thorium isotopes, such as 228Th and its decay products, are investigated and used in targeted alpha therapy for cancer treatment. Furthermore, the unique properties of the 229Th nuclear isomer are being explored for the development of highly precise nuclear clocks and potentially for quantum computing applications, representing cutting-edge research in nuclear physics and metrology.

Historical Context

Early Discoveries and Naming

The study of thorium's isotopes has a rich history. The isotope 230Th was initially named "Ionium" before the concept of isotopes was fully understood. Early research into radioactive decay chains, particularly those originating from uranium, revealed the existence and properties of various thorium isotopes. The long half-life of 232Th established it as a primordial nuclide, forming the backbone of the thorium decay series.

Isomeric State Research

Significant scientific effort has been dedicated to understanding the low-lying nuclear isomer of 229Th (229mTh). The precise measurement of its excitation energy and lifetime has been a complex endeavor, involving advanced spectroscopic techniques. Recent breakthroughs in laser spectroscopy have provided highly accurate values for this energy, paving the way for practical applications like nuclear clocks.

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References

References

  1.  mThย โ€“ Excited nuclear isomer.
  2.  (โ€‰)ย โ€“ Uncertainty (1ฯƒ) is given in concise form in parentheses after the corresponding last digits.
  3.  #ย โ€“ Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  4.  Bold half-lifeย โ€“ nearly stable, half-life longer than age of universe.
  5.  #ย โ€“ Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  6.  Intermediate decay product of 235U
  7.  Intermediate decay product of 237Np
  8.  Used in uraniumรขย€ย“thorium dating
  9.  Primordial radionuclide
  10.  Specifically from thermal neutron fission of uranium-235, e.g. in a typical nuclear reactor.
  11.  This is the heaviest nuclide with a half-life of at least four years before the "sea of instability".
A full list of references for this article are available at the Isotopes of thorium Wikipedia page

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Important Disclaimer

Scientific Data and Safety Notice

This content has been generated by an AI model based on publicly available scientific data. While efforts have been made to ensure accuracy and adherence to the source material, it is intended for informational and educational purposes only. Thorium and its isotopes are radioactive materials and may pose health risks. Handling or exposure should only be done under strict safety protocols and expert supervision.

This is not professional advice. The information provided does not substitute for expert consultation in nuclear physics, materials science, or radiation safety. Always consult official documentation and qualified professionals for any practical applications or safety concerns related to radioactive materials.

The creators of this page are not liable for any errors, omissions, or consequences arising from the use of this information.