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Isotopes of radium

Radium (88Ra) has no stable or nearly stable isotopes, and thus a standard atomic weight cannot be given. The longest lived, and most common, isotope of radium is 226Ra with a half-life of 1600 years. 226Ra occurs in the decay chain of 238U (often referred to as the radium series). Radium has 34 known isotopes from 201Ra to 234Ra.

Isotopes of radium (88Ra)
Main isotopes[1] Decay
abun­dance half-life (t1/2) mode pro­duct
223Ra trace 11.43 d α 219Rn
224Ra trace 3.6319 d α 220Rn
225Ra trace 14.9 d β 225Ac
226Ra trace 1599 y α 222Rn
228Ra trace 5.75 y β 228Ac

In 2013 it was discovered that the nucleus of radium-224 is pear-shaped.[2] This was the first discovery of an asymmetrical nucleus.

List of isotopes Edit

Nuclide
[n 1]
Historic
name
Z N Isotopic mass (Da)
[n 2][n 3]
Half-life
Decay
mode

[n 4]
Daughter
isotope

[n 5]
Spin and
parity
[n 6][n 7]
Isotopic
abundance
Excitation energy[n 7]
201Ra[3] 88 113 8+40
−4
 ms
α 197Rn (3/2−)
201mRa[4] 260(30) keV 1.6+7.7
−0.7
 ms
α 197mRn (13/2+)
202Ra 88 114 202.00989(7) 3.8+1.3
−0.8
 ms
[3]
α 198Rn 0+
203Ra 88 115 203.00927(9) 4(3) ms α 199Rn (3/2−)
β+ (rare) 203Fr
203mRa 220(90) keV 41(17) ms α 199Rn (13/2+)
β+ (rare) 203Fr
204Ra 88 116 204.006500(17) 60(11) ms
[59(+12−9) ms]
α (99.7%) 200Rn 0+
β+ (.3%) 204Fr
205Ra 88 117 205.00627(9) 220(40) ms
[210(+60−40) ms]
α 201Rn (3/2−)
β+ (rare) 205Fr
205mRa 310(110)# keV 180(50) ms
[170(+60−40) ms]
α 201Rn (13/2+)
IT (rare) 205Ra
206Ra 88 118 206.003827(19) 0.24(2) s α 202Rn 0+
207Ra 88 119 207.00380(6) 1.3(2) s α (90%) 203Rn (5/2−, 3/2−)
β+ (10%) 207Fr
207mRa 560(50) keV 57(8) ms IT (85%) 207Ra (13/2+)
α (15%) 203Rn
β+ (.55%) 207Fr
208Ra 88 120 208.001840(17) 1.3(2) s α (95%) 204Rn 0+
β+ (5%) 208Fr
208mRa 1800(200) keV 270 ns (8+)
209Ra 88 121 209.00199(5) 4.6(2) s α (90%) 205Rn 5/2−
β+ (10%) 209Fr
210Ra 88 122 210.000495(16) 3.7(2) s α (96%) 206Rn 0+
β+ (4%) 210Fr
210mRa 1800(200) keV 2.24 μs (8+)
211Ra 88 123 211.000898(28) 13(2) s α (97%) 207Rn 5/2(−)
β+ (3%) 211Fr
212Ra 88 124 211.999794(12) 13.0(2) s α (85%) 208Rn 0+
β+ (15%) 212Fr
212m1Ra 1958.4(5) keV 10.9(4) μs (8)+
212m2Ra 2613.4(5) keV 0.85(13) μs (11)−
213Ra 88 125 213.000384(22) 2.74(6) min α (80%) 209Rn 1/2−
β+ (20%) 213Fr
213mRa 1769(6) keV 2.1(1) ms IT (99%) 213Ra 17/2−#
α (1%) 209Rn
214Ra 88 126 214.000108(10) 2.46(3) s α (99.94%) 210Rn 0+
β+ (.06%) 214Fr
215Ra 88 127 215.002720(8) 1.55(7) ms α 211Rn (9/2+)#
215m1Ra 1877.8(5) keV 7.1(2) μs (25/2+)
215m2Ra 2246.9(5) keV 1.39(7) μs (29/2−)
215m3Ra 3756.6(6)+X keV 0.555(10) μs (43/2−)
216Ra 88 128 216.003533(9) 182(10) ns α 212Rn 0+
EC (1×10−8%) 216Fr
217Ra 88 129 217.006320(9) 1.63(17) μs α 213Rn (9/2+)
218Ra 88 130 218.007140(12) 25.2(3) μs α 214Rn 0+
219Ra 88 131 219.010085(9) 10(3) ms α 215Rn (7/2)+
220Ra 88 132 220.011028(10) 17.9(14) ms α 216Rn 0+
221Ra 88 133 221.013917(5) 28(2) s α 217Rn 5/2+ Trace[n 8]
CD (1.2×10−10%) 207Pb
14C
222Ra 88 134 222.015375(5) 38.0(5) s α 218Rn 0+
CD (3×10−8%) 208Pb
14C
223Ra[n 9] Actinium X 88 135 223.0185022(27) 11.43(5) d α 219Rn 3/2+ Trace[n 10]
CD (6.4×10−8%) 209Pb
14C
224Ra Thorium X 88 136 224.0202118(24) 3.6319(23) d α 220Rn 0+ Trace[n 11]
CD (4.3×10−9%) 210Pb
14C
225Ra 88 137 225.023612(3) 14.9(2) d β 225Ac 1/2+ Trace[n 12]
226Ra Radium[n 13] 88 138 226.0254098(25) 1600(7) y α 222Rn 0+ Trace[n 14]
CD (2.6×10−9%) 212Pb
14C
227Ra 88 139 227.0291778(25) 42.2(5) min β 227Ac 3/2+
228Ra Mesothorium 1 88 140 228.0310703(26) 5.75(3) y β 228Ac 0+ Trace[n 11]
229Ra 88 141 229.034958(20) 4.0(2) min β 229Ac 5/2(+)
230Ra 88 142 230.037056(13) 93(2) min β 230Ac 0+
231Ra 88 143 231.04122(32)# 103(3) s β 231Ac (5/2+)
231mRa 66.21(9) keV ~53 μs (1/2+)
232Ra 88 144 232.04364(30)# 250(50) s β 232Ac 0+
233Ra 88 145 233.04806(50)# 30(5) s β 233Ac 1/2+#
234Ra 88 146 234.05070(53)# 30(10) s β 234Ac 0+
This table header & footer:
  1. ^ mRa – Excited nuclear isomer.
  2. ^ ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
  3. ^ # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  4. ^ Modes of decay:
  5. ^ Bold symbol as daughter – Daughter product is stable.
  6. ^ ( ) spin value – Indicates spin with weak assignment arguments.
  7. ^ a b # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  8. ^ Intermediate decay product of 237Np
  9. ^ Used for treating bone cancer
  10. ^ Intermediate decay product of 235U
  11. ^ a b Intermediate decay product of 232Th
  12. ^ Intermediate decay product of 237Np
  13. ^ Source of element's name
  14. ^ Intermediate decay product of 238U

Actinides vs fission products Edit

Actinides[5] by decay chain Half-life
range (a)
Fission products of 235U by yield[6]
4n 4n + 1 4n + 2 4n + 3 4.5–7% 0.04–1.25% <0.001%
228Ra 4–6 a 155Euþ
244Cmƒ 241Puƒ 250Cf 227Ac 10–29 a 90Sr 85Kr 113mCdþ
232Uƒ 238Puƒ 243Cmƒ 29–97 a 137Cs 151Smþ 121mSn
248Bk[7] 249Cfƒ 242mAmƒ 141–351 a

No fission products have a half-life in the range of 100 a–210 ka ...

241Amƒ 251Cfƒ[8] 430–900 a
226Ra 247Bk 1.3–1.6 ka
240Pu 229Th 246Cmƒ 243Amƒ 4.7–7.4 ka
245Cmƒ 250Cm 8.3–8.5 ka
239Puƒ 24.1 ka
230Th 231Pa 32–76 ka
236Npƒ 233Uƒ 234U 150–250 ka 99Tc 126Sn
248Cm 242Pu 327–375 ka 79Se
1.53 Ma 93Zr
237Npƒ 2.1–6.5 Ma 135Cs 107Pd
236U 247Cmƒ 15–24 Ma 129I
244Pu 80 Ma

... nor beyond 15.7 Ma[9]

232Th 238U 235Uƒ№ 0.7–14.1 Ga

References Edit

  1. ^ Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3): 030001. doi:10.1088/1674-1137/abddae.
  2. ^ "First observations of short-lived pear-shaped atomic nuclei".
  3. ^ a b Kalaninová, Z.; Antalic, S.; Andreyev, A. N.; Heßberger, F. P.; Ackermann, D.; Andel, B.; Bianco, L.; Hofmann, S.; Huyse, M.; Kindler, B.; Lommel, B.; Mann, R.; Page, R. D.; Sapple, P. J.; Thomson, J.; Van Duppen, P.; Venhart, M. (12 May 2014). "Decay of 201–203Ra and 200–202Fr" (PDF). Physical Review C. 89 (5). doi:10.1103/PhysRevC.89.054312. ISSN 0556-2813. Retrieved 11 June 2023.
  4. ^ Uusitalo, J.; Leino, M.; Enqvist, T.; Eskola, K.; Grahn, T.; Greenlees, P. T.; Jones, P.; Julin, R.; Juutinen, S.; Keenan, A.; Kettunen, H.; Koivisto, H.; Kuusiniemi, P.; Leppänen, A.-P.; Nieminen, P.; Pakarinen, J.; Rahkila, P.; Scholey, C. (11 February 2005). "α decay studies of very neutron-deficient francium and radium isotopes". Physical Review C. 71 (2). doi:10.1103/PhysRevC.71.024306. ISSN 0556-2813.
  5. ^ Plus radium (element 88). While actually a sub-actinide, it immediately precedes actinium (89) and follows a three-element gap of instability after polonium (84) where no nuclides have half-lives of at least four years (the longest-lived nuclide in the gap is radon-222 with a half life of less than four days). Radium's longest lived isotope, at 1,600 years, thus merits the element's inclusion here.
  6. ^ Specifically from thermal neutron fission of uranium-235, e.g. in a typical nuclear reactor.
  7. ^ Milsted, J.; Friedman, A. M.; Stevens, C. M. (1965). "The alpha half-life of berkelium-247; a new long-lived isomer of berkelium-248". Nuclear Physics. 71 (2): 299. Bibcode:1965NucPh..71..299M. doi:10.1016/0029-5582(65)90719-4.
    "The isotopic analyses disclosed a species of mass 248 in constant abundance in three samples analysed over a period of about 10 months. This was ascribed to an isomer of Bk248 with a half-life greater than 9 [years]. No growth of Cf248 was detected, and a lower limit for the β half-life can be set at about 104 [years]. No alpha activity attributable to the new isomer has been detected; the alpha half-life is probably greater than 300 [years]."
  8. ^ This is the heaviest nuclide with a half-life of at least four years before the "sea of instability".
  9. ^ Excluding those "classically stable" nuclides with half-lives significantly in excess of 232Th; e.g., while 113mCd has a half-life of only fourteen years, that of 113Cd is nearly eight quadrillion years.
  • Isotope masses from:
    • Audi, Georges; Bersillon, Olivier; Blachot, Jean; Wapstra, Aaldert Hendrik (2003), "The NUBASE evaluation of nuclear and decay properties", Nuclear Physics A, 729: 3–128, Bibcode:2003NuPhA.729....3A, doi:10.1016/j.nuclphysa.2003.11.001
  • Isotopic compositions and standard atomic masses from:
    • de Laeter, John Robert; Böhlke, John Karl; De Bièvre, Paul; Hidaka, Hiroshi; Peiser, H. Steffen; Rosman, Kevin J. R.; Taylor, Philip D. P. (2003). "Atomic weights of the elements. Review 2000 (IUPAC Technical Report)". Pure and Applied Chemistry. 75 (6): 683–800. doi:10.1351/pac200375060683.
    • Wieser, Michael E. (2006). "Atomic weights of the elements 2005 (IUPAC Technical Report)". Pure and Applied Chemistry. 78 (11): 2051–2066. doi:10.1351/pac200678112051.
  • "News & Notices: Standard Atomic Weights Revised". International Union of Pure and Applied Chemistry. 19 October 2005.
  • Half-life, spin, and isomer data selected from the following sources.

isotopes, radium, radium, 88ra, stable, nearly, stable, isotopes, thus, standard, atomic, weight, cannot, given, longest, lived, most, common, isotope, radium, 226ra, with, half, life, 1600, years, 226ra, occurs, decay, chain, 238u, often, referred, radium, se. Radium 88Ra has no stable or nearly stable isotopes and thus a standard atomic weight cannot be given The longest lived and most common isotope of radium is 226Ra with a half life of 1600 years 226Ra occurs in the decay chain of 238U often referred to as the radium series Radium has 34 known isotopes from 201Ra to 234Ra Isotopes of radium 88Ra Main isotopes 1 Decayabun dance half life t1 2 mode pro duct223Ra trace 11 43 d a 219Rn224Ra trace 3 6319 d a 220Rn225Ra trace 14 9 d b 225Ac226Ra trace 1599 y a 222Rn228Ra trace 5 75 y b 228AcviewtalkeditIn 2013 it was discovered that the nucleus of radium 224 is pear shaped 2 This was the first discovery of an asymmetrical nucleus List of isotopes EditNuclide n 1 Historicname Z N Isotopic mass Da n 2 n 3 Half life Decaymode n 4 Daughterisotope n 5 Spin andparity n 6 n 7 IsotopicabundanceExcitation energy n 7 201Ra 3 88 113 8 40 4 ms a 197Rn 3 2 201mRa 4 260 30 keV 1 6 7 7 0 7 ms a 197mRn 13 2 202Ra 88 114 202 00989 7 3 8 1 3 0 8 ms 3 a 198Rn 0 203Ra 88 115 203 00927 9 4 3 ms a 199Rn 3 2 b rare 203Fr203mRa 220 90 keV 41 17 ms a 199Rn 13 2 b rare 203Fr204Ra 88 116 204 006500 17 60 11 ms 59 12 9 ms a 99 7 200Rn 0 b 3 204Fr205Ra 88 117 205 00627 9 220 40 ms 210 60 40 ms a 201Rn 3 2 b rare 205Fr205mRa 310 110 keV 180 50 ms 170 60 40 ms a 201Rn 13 2 IT rare 205Ra206Ra 88 118 206 003827 19 0 24 2 s a 202Rn 0 207Ra 88 119 207 00380 6 1 3 2 s a 90 203Rn 5 2 3 2 b 10 207Fr207mRa 560 50 keV 57 8 ms IT 85 207Ra 13 2 a 15 203Rnb 55 207Fr208Ra 88 120 208 001840 17 1 3 2 s a 95 204Rn 0 b 5 208Fr208mRa 1800 200 keV 270 ns 8 209Ra 88 121 209 00199 5 4 6 2 s a 90 205Rn 5 2 b 10 209Fr210Ra 88 122 210 000495 16 3 7 2 s a 96 206Rn 0 b 4 210Fr210mRa 1800 200 keV 2 24 ms 8 211Ra 88 123 211 000898 28 13 2 s a 97 207Rn 5 2 b 3 211Fr212Ra 88 124 211 999794 12 13 0 2 s a 85 208Rn 0 b 15 212Fr212m1Ra 1958 4 5 keV 10 9 4 ms 8 212m2Ra 2613 4 5 keV 0 85 13 ms 11 213Ra 88 125 213 000384 22 2 74 6 min a 80 209Rn 1 2 b 20 213Fr213mRa 1769 6 keV 2 1 1 ms IT 99 213Ra 17 2 a 1 209Rn214Ra 88 126 214 000108 10 2 46 3 s a 99 94 210Rn 0 b 06 214Fr215Ra 88 127 215 002720 8 1 55 7 ms a 211Rn 9 2 215m1Ra 1877 8 5 keV 7 1 2 ms 25 2 215m2Ra 2246 9 5 keV 1 39 7 ms 29 2 215m3Ra 3756 6 6 X keV 0 555 10 ms 43 2 216Ra 88 128 216 003533 9 182 10 ns a 212Rn 0 EC 1 10 8 216Fr217Ra 88 129 217 006320 9 1 63 17 ms a 213Rn 9 2 218Ra 88 130 218 007140 12 25 2 3 ms a 214Rn 0 219Ra 88 131 219 010085 9 10 3 ms a 215Rn 7 2 220Ra 88 132 220 011028 10 17 9 14 ms a 216Rn 0 221Ra 88 133 221 013917 5 28 2 s a 217Rn 5 2 Trace n 8 CD 1 2 10 10 207Pb14C222Ra 88 134 222 015375 5 38 0 5 s a 218Rn 0 CD 3 10 8 208Pb14C223Ra n 9 Actinium X 88 135 223 0185022 27 11 43 5 d a 219Rn 3 2 Trace n 10 CD 6 4 10 8 209Pb14C224Ra Thorium X 88 136 224 0202118 24 3 6319 23 d a 220Rn 0 Trace n 11 CD 4 3 10 9 210Pb14C225Ra 88 137 225 023612 3 14 9 2 d b 225Ac 1 2 Trace n 12 226Ra Radium n 13 88 138 226 0254098 25 1600 7 y a 222Rn 0 Trace n 14 CD 2 6 10 9 212Pb14C227Ra 88 139 227 0291778 25 42 2 5 min b 227Ac 3 2 228Ra Mesothorium 1 88 140 228 0310703 26 5 75 3 y b 228Ac 0 Trace n 11 229Ra 88 141 229 034958 20 4 0 2 min b 229Ac 5 2 230Ra 88 142 230 037056 13 93 2 min b 230Ac 0 231Ra 88 143 231 04122 32 103 3 s b 231Ac 5 2 231mRa 66 21 9 keV 53 ms 1 2 232Ra 88 144 232 04364 30 250 50 s b 232Ac 0 233Ra 88 145 233 04806 50 30 5 s b 233Ac 1 2 234Ra 88 146 234 05070 53 30 10 s b 234Ac 0 This table header amp footer view mRa Excited nuclear isomer Uncertainty 1s is given in concise form in parentheses after the corresponding last digits Atomic mass marked value and uncertainty derived not from purely experimental data but at least partly from trends from the Mass Surface TMS Modes of decay CD Cluster decayEC Electron captureIT Isomeric transition Bold symbol as daughter Daughter product is stable spin value Indicates spin with weak assignment arguments a b Values marked are not purely derived from experimental data but at least partly from trends of neighboring nuclides TNN Intermediate decay product of 237Np Used for treating bone cancer Intermediate decay product of 235U a b Intermediate decay product of 232Th Intermediate decay product of 237Np Source of element s name Intermediate decay product of 238UActinides vs fission products EditActinides and fission products by half life vteActinides 5 by decay chain Half life range a Fission products of 235U by yield 6 4n 4n 1 4n 2 4n 3 4 5 7 0 04 1 25 lt 0 001 228Ra 4 6 a 155Euth244Cmƒ 241Puƒ 250Cf 227Ac 10 29 a 90Sr 85Kr 113mCdth232Uƒ 238Puƒ 243Cmƒ 29 97 a 137Cs 151Smth 121mSn248Bk 7 249Cfƒ 242mAmƒ 141 351 a No fission products have a half life in the range of 100 a 210 ka 241Amƒ 251Cfƒ 8 430 900 a226Ra 247Bk 1 3 1 6 ka240Pu 229Th 246Cmƒ 243Amƒ 4 7 7 4 ka245Cmƒ 250Cm 8 3 8 5 ka239Puƒ 24 1 ka230Th 231Pa 32 76 ka236Npƒ 233Uƒ 234U 150 250 ka 99Tc 126Sn248Cm 242Pu 327 375 ka 79Se 1 53 Ma 93Zr237Npƒ 2 1 6 5 Ma 135Cs 107Pd236U 247Cmƒ 15 24 Ma 129I 244Pu 80 Ma nor beyond 15 7 Ma 9 232Th 238U 235Uƒ 0 7 14 1 Ga has thermal neutron capture cross section in the range of 8 50 barnsƒ fissile primarily a naturally occurring radioactive material NORM th neutron poison thermal neutron capture cross section greater than 3k barns References Edit Kondev F G Wang M Huang W J Naimi S Audi G 2021 The NUBASE2020 evaluation of nuclear properties PDF Chinese Physics C 45 3 030001 doi 10 1088 1674 1137 abddae First observations of short lived pear shaped atomic nuclei a b Kalaninova Z Antalic S Andreyev A N Hessberger F P Ackermann D Andel B Bianco L Hofmann S Huyse M Kindler B Lommel B Mann R Page R D Sapple P J Thomson J Van Duppen P Venhart M 12 May 2014 Decay of 201 203Ra and 200 202Fr PDF Physical Review C 89 5 doi 10 1103 PhysRevC 89 054312 ISSN 0556 2813 Retrieved 11 June 2023 Uusitalo J Leino M Enqvist T Eskola K Grahn T Greenlees P T Jones P Julin R Juutinen S Keenan A Kettunen H Koivisto H Kuusiniemi P Leppanen A P Nieminen P Pakarinen J Rahkila P Scholey C 11 February 2005 a decay studies of very neutron deficient francium and radium isotopes Physical Review C 71 2 doi 10 1103 PhysRevC 71 024306 ISSN 0556 2813 Plus radium element 88 While actually a sub actinide it immediately precedes actinium 89 and follows a three element gap of instability after polonium 84 where no nuclides have half lives of at least four years the longest lived nuclide in the gap is radon 222 with a half life of less than four days Radium s longest lived isotope at 1 600 years thus merits the element s inclusion here Specifically from thermal neutron fission of uranium 235 e g in a typical nuclear reactor Milsted J Friedman A M Stevens C M 1965 The alpha half life of berkelium 247 a new long lived isomer of berkelium 248 Nuclear Physics 71 2 299 Bibcode 1965NucPh 71 299M doi 10 1016 0029 5582 65 90719 4 The isotopic analyses disclosed a species of mass 248 in constant abundance in three samples analysed over a period of about 10 months This was ascribed to an isomer of Bk248 with a half life greater than 9 years No growth of Cf248 was detected and a lower limit for the b half life can be set at about 104 years No alpha activity attributable to the new isomer has been detected the alpha half life is probably greater than 300 years This is the heaviest nuclide with a half life of at least four years before the sea of instability Excluding those classically stable nuclides with half lives significantly in excess of 232Th e g while 113mCd has a half life of only fourteen years that of 113Cd is nearly eight quadrillion years Isotope masses from Audi Georges Bersillon Olivier Blachot Jean Wapstra Aaldert Hendrik 2003 The NUBASE evaluation of nuclear and decay properties Nuclear Physics A 729 3 128 Bibcode 2003NuPhA 729 3A doi 10 1016 j nuclphysa 2003 11 001 Isotopic compositions and standard atomic masses from de Laeter John Robert Bohlke John Karl De Bievre Paul Hidaka Hiroshi Peiser H Steffen Rosman Kevin J R Taylor Philip D P 2003 Atomic weights of the elements Review 2000 IUPAC Technical Report Pure and Applied Chemistry 75 6 683 800 doi 10 1351 pac200375060683 Wieser Michael E 2006 Atomic weights of the elements 2005 IUPAC Technical Report Pure and Applied Chemistry 78 11 2051 2066 doi 10 1351 pac200678112051 News amp Notices Standard Atomic Weights Revised International Union of Pure and Applied Chemistry 19 October 2005 Half life spin and isomer data selected from the following sources Audi Georges Bersillon Olivier Blachot Jean Wapstra Aaldert Hendrik 2003 The NUBASE evaluation of nuclear and decay properties Nuclear Physics A 729 3 128 Bibcode 2003NuPhA 729 3A doi 10 1016 j nuclphysa 2003 11 001 National Nuclear Data Center NuDat 2 x database Brookhaven National Laboratory Holden Norman E 2004 11 Table of the Isotopes In Lide David R ed CRC Handbook of Chemistry and Physics 85th ed Boca Raton Florida CRC Press ISBN 978 0 8493 0485 9 Retrieved from https en wikipedia org w index php title Isotopes of radium amp oldid 1159771670 Radium 226, wikipedia, wiki, book, 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