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Lawrencium is an exclusively artificially produced radioactive chemical element that is not known in nature.
With 258Lr, the first lawrencium isotope was discovered in 1961 by the research team led by Albert Ghiorso at the Lawrence Berkeley National Laboratory University of California.
To date, a total of 11 different isotopes have been produced, all of which are extremely short-lived; with a half-life of about 4 hours, Lawrencium-262 is the most stable Lr nuclide. It is expected that heavier lawrencium nuclides may have longer half-lives.
Atoms or atomic nuclei are generally referred to as lawrencium isotopes or lawrencium nuclides, which have element-specific 103 protons and differ in the number of neutrons in the nucleus.
Isotope Nuclide | E | N | Atomic Mass [Nuclear Mass] {Mass Excess} | Spin I (h/2π) | Parent |
---|---|---|---|---|---|
1 | 2 | 3 | 4 | 5 | 6 |
Lawrencium-251 | 251103Lr | 148 | 251 u [250.943505 u] {0 MeV} | ||
Lawrencium-252 | 252103Lr | 149 | 252.09526(25) u [252.038765 u] {88.73412 MeV} | 256Db | |
Lawrencium-253 | 253103Lr | 150 | 253.09509(22) u [253.038595 u] {88.57576 MeV} | (7/2-) | 257Db |
Lawrencium-253m | 253m103Lr | 150 | 253.09509(22) u [253.038595 u] {88.57576 MeV} | (1/2-) | |
Lawrencium-254 | 254103Lr | 151 | 254.09648(32) u [254.039985 u] {89.87054 MeV} | 258Db | |
Lawrencium-255 | 255103Lr | 152 | 255.096562(19) u [255.040067 u] {89.94692 MeV} | (1/2-) | |
Lawrencium-255m1 | 255m1103Lr | 152 | 255.096562(19) u [255.040067 u] {89.94692 MeV} | (7/2-) | |
Lawrencium-256 | 256103Lr | 153 | 256.09849(9) u [256.041995 u] {91.74284 MeV} | 260Db | |
Lawrencium-257 | 257103Lr | 154 | 257.09948(5) u [257.042985 u] {92.66502 MeV} | 9/2+ | 261Db |
Lawrencium-258 | 258103Lr | 155 | 258.10175(11) u [258.045255 u] {94.77951 MeV} | 262Db | |
Lawrencium-259 | 259103Lr | 156 | 259.10290(8) u [259.046405 u] {95.85073 MeV} | (9/2+) | 263Db |
Lawrencium-260 | 260103Lr | 157 | 260.10550(13) u [260.049005 u] {98.27262 MeV} | ||
Lawrencium-261 | 261103Lr | 158 | 261.10688(21) u [261.050385 u] {99.55808 MeV} | ||
Lawrencium-262 | 262103Lr | 159 | 262.10961(21) u [262.053115 u] {102.10106 MeV} | ||
Lawrencium-263 | 263103Lr | 160 | |||
Lawrencium-264 | 264103Lr | 161 | 264 u [263.943505 u] {0 MeV} | ||
Lawrencium-265 | 265103Lr | 162 | |||
Lawrencium-266 | 266103Lr | 163 | 266.11983(63) u [266.063335 u] {111.62093 MeV} |
Isotope | Radioactive Decay | Extern | |||
---|---|---|---|---|---|
Half-life | Decay Mode | Probability | Energy | ||
7 | 8 | 9 | 10 | 11 | 12 |
Lr-251 | α 247Md ε ? | AL | |||
Lr-252 | 0.36 s | EC/β+ → 252No α → 248Md SF div. | ? ? ? | 5.87(24) MeV 9.164(17) MeV | AL |
Lr-253 | 0.57 s | α → 249Md SF div. | 98.7 % 1.3 % | 8.918(20) MeV | AL |
Lr-253m | 1.49 s | α → 249Md SF div. | 92(5) % 8(5) % | AL | |
Lr-254 | 18.1(18) s | EC/β+ → 254No α → 250Md SF div. | 28.3(19) % 71.7(19) % < 0.1 % | 5.15(30) MeV 8.816(12) MeV | AL |
Lr-255 | 31.1(11) s | α → 251Md EC → 255No SF div. | 99.7(1) % < 0.3(1) % < 0.1 % | 8.556(7) MeV 3.140(23) MeV | AL |
Lr-255m1 | 2.54(5) s | Iso → 255Lr α → 251Md | ca. 60 % ca. 40 % | ||
Lr-256 | 27.9 s | EC/β+ → 256No α → 253Md SF div. | 15(10) % 85(10) % < 0.03 % | 3.92(8) MeV 8.81(10) MeV | AL |
Lr-257 | 4 s | α → 253Md EC → 257No SF div. | < 100 % < 15 % < 0.033 % | 9.07(3) MeV 2.42(4) MeV | AL |
Lr-258 | 3.92(33) s | α → 254Md EC → 258No | 97.4(18) % 2.6 (18) | 8.904(19) MeV 3.30(14) MeV | AL |
Lr-259 | 6.2(3) s | α → 255Md SF div. | 78(2) % 22(2) % | 8.58(7) | AL |
Lr-260 | 180(30) s | α → 256Md EC → 260No | 80(20) % < 40 % | 8.40(14) MeV 2.66(24) MeV | AL |
Lr-261 | 39(12) min | SF div. | ? | AL | |
Lr-262 | 4 h | SF div. EC/β+ → 262No α → 258Md | < 10 % ? ? | 2.00(41) MeV 7.99(20) MeV | AL |
Lr-263 | gibt es nicht | AL | |||
Lr-264 | 4.9 h | SF div | AL | ||
Lr-265 | unknown | AL | |||
Lr-266 | 11 h | SF div. | 100 % | AL |
Notes (related to the columns):
1 - name of the nuclide, isotope.
2 - E: isotope symbol with mass number (superscript; number of nucleons) and atomic number (subscript; number of protons).
3 - N: number of neutrons.
4 - relative atomic mass of the Lawrencium isotope (isotopic mass including electrons) and the mass of the atomic nucleus in square brackets (nuclear mass, nuclide mass without electrons), each related to 12C = 12.00000 [2]. In addition, the mass excess is given in MeV.
5 - nuclear spin I, unit: h/2π.
6 - source nuclides: Possible, assumed or actual source nuclides (mother nuclides, parent nuclides). If applicable, the corresponding decay modes can be found in the data for the respective starting nuclide.
7 - isotope notation in short form.
8 - decay: half-live of the Lawrencium isotope (a = years; ; d = days; h = hours; min = minutes; s = seconds).
9 - decay mode: type of decay into the respective daughter nuclides with n = neutron emission; p = proton emission; α = alpha decay; β- = beta minus decay with electron emission; EC = electron capture; β+ = positron emission; ε = β+ and/or EC; Iso = isomeric transition; CD = cluster decay; SF = spontaneous decay.
10 - decay probability in percent (%).
11 - decay energy; Particle energy related to decay type.
12 - other information and notes: AL = Adopted Levels (link to external data [1]).
Miscellaneous:
()- Numbers in brackets: uncertainty to represent the spread of the reported value.
~ - Theoretical values or systematic trends.
- unlisted-: Nuclides that have already been mentioned in the literature but for some reason can no longer be found in the current nuclide tables because their discovery e.g. has not confirmed.
Properties of the Lawrencium nucleides
[1] - NuDat: National Nuclear Data Center, Brookhaven National Laboratory, based on ENSDF and the Nuclear Wallet Cards.
[2] - G. Audi et. al.: The NUBASE evaluation of nuclear and decay properties. Nuclear Physics, (2003), DOI 10.1016/j.nuclphysa.2003.11.001.
[3] - Live Chart of Nuclides. Nuclear structure and decay data.
Lawrencium: NMR properties
[4] - N. J. Stone: Table of nuclear magnetic dipole and electric quadrupole moments. Atomic Data and Nuclear Data Tables, (2005), DOI 10.1016/j.adt.2005.04.001.
[5] - Pekka Pyykkö: Year-2008 nuclear quadrupole moments. Molecular Physics, (2008), DOI 10.1080/00268970802018367.
[6] - Pekka Pyykkö: Year-2017 nuclear quadrupole moments. Molecular Physics, (2018), DOI 10.1080/00268976.2018.1426131.
[7] - N. J. Stone: Table of recommended nuclear magnetic dipole moments. IAEA, (2019).
More sources:
[8] - Isotopic abundances, atomic weights and isotopic masses: see respective keyword.
[9] - J. Khuyagbaatar et al.:
48Ca + 249Bk Fusion Reaction Leading to Element Z = 117: Long-Lived α-Decaying 270Db and Discovery of 266Lr.
In: Physical Review Letters, (2014), DOI 10.1103/PhysRevLett.112.172501.
Last update: 2022-11-30
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