Lawrencium (Lr)
actinideSolid
Standard Atomic Weight
[262]Electron configuration
[Rn] 7s2 5f14 6d1Melting point
1626.85 °CBoiling point
N/ADensity
1.56e+4 kg/m³Oxidation states
+3Electronegativity (Pauling)
N/AIonization energy (1st)
4.96 eVDiscovery year
1961Atomic radius
N/ADetails
Lawrencium is a synthetic, highly radioactive actinide and the last element of the actinide series. It has been made only in minute numbers of atoms in nuclear reactions, so its chemistry is known from rapid, atom-at-a-time experiments and theoretical calculations. Its most stable known isotopes are short-lived on ordinary laboratory timescales. In solution it behaves chiefly as a trivalent metal, Lr³⁺, broadly resembling late actinides and some trivalent lanthanides.
Lawrencium does not occur naturally in the Earth’s crust. Credit for the first synthesis of this element in 1971 is given jointly to Albert Ghiorso and his team at the University of California in Berkeley and Georgi Flerov and his team at the Joint Institute for Nuclear Research (JINR) in Dubna, Russia (Fig. IUPAC.103.1). The element is named for Ernest O. Lawrence (Fig. IUPAC.103.2), who developed the cyclotron. The chemical symbol for lawrencium was originally proposed as Lw. At the IUPAC General Assembly in 1963, lawrencium was officially accepted by IUPAC, but the symbol was changed to Lr because the Commission on Inorganic Nomenclature determined that the letter ‘w’ presented a problem in languages other than English [636], [640], [641], [642]. There are no known isotopic applications for lawrencium outside of scientific research.
Lawrencium behaves differently from dipositive nobelium and more like the tripositive elements earlier in the actinide series.
Lawrencium was created by four American scientists, Albert Ghiorso, Torbjørn Sikkeland, Almon E. Larsh and Robert M. Latimer, in March, 1961. Working at the Lawrence Radiation Laboratory in Berkeley, California, the scientists placed three micrograms (0.000003 grams) of californium in the target chamber of a device called a linear accelerator. The scientists used the accelerator to bombard the californium with boron ions. Several different isotopes of lawrencium were created and there is some confusion as to which isotope the group actually detected. Today, the Lawrence Radiation Laboratory is known as the Lawrence Berkeley Laboratory. Lawrencium's most stable isotope, lawrencium-262, has a half-life of about 4 hours. It decays into nobelium-262 through electron capture, mendelevium-258 through alpha decay or through spontaneous fission.
Named after Lawrence, inventor of the cyclotron. This member of the 5f transition elements (actinide series) was discovered in March 1961 by A. Ghiorso, T. Sikkeland, A.E. Larsh, and R.M. Latimer. A 3-Mg californium target, consisting of a mixture of isotopes of mass number 249, 250, 251, and 252, was bombarded with either 10B or 11B. The electrically charged transmutation nuclei recoiled with an atmosphere of helium and were collected on a thin copper conveyor tape which was then moved to place collected atoms in front of a series of solid-state detectors. The isotope of element 103 produced in this way decayed by emitting an 8.6 MeV alpha particle with a half-life of 8 s.
In 1967, Flerov and associates at the Dubna Laboratory reported their inability to detect an alpha emitter with a half-life of 8 s which was assigned by the Berkeley group to 257103. This assignment has been changed to 258Lr or 259Lr.
In 1965, the Dubna workers found a longer-lived lawrencium isotope, 256Lr, with a half-life of 35 s. In 1968, Thiorso and associates at Berkeley used a few atoms of this isotope to study the oxidation behavior of lawrencium. Using solvent extraction techniques and working very rapidly, they extracted lawrencium ions from a buffered aqueous solution into an organic solvent completing each extraction in about 30 s.
No macroscopic sample of lawrencium has been prepared, and its visible appearance has not been observed. The pure metal’s color, texture, density, melting behavior, and other bulk properties are therefore unknown or only theoretically estimated.
Lawrencium has no practical use outside scientific research. Its isotopes are produced to study nuclear structure, heavy-element synthesis, decay chains, and the chemical behavior at the end of the actinide series. Individual atoms have also been used in chromatography and related experiments to test periodic trends, especially the stability and complexing behavior of Lr³⁺. It has no commercial, medical, industrial, or consumer application.
Since only tiny amounts of lawrencium have ever been produced, there are currently no uses for it outside of basic scientific research.
No weighable compound of lawrencium has been isolated. The established chemistry is dominated by the +3 oxidation state in aqueous solution, where Lr³⁺ is the important species. Atom-at-a-time studies have examined its adsorption and complex formation with mineral acids and organic complexants. Simple compounds such as lawrencium trichloride, LrCl₃, or lawrencium oxide, Lr₂O₃, are chemically plausible by analogy, but their bulk structures and properties have not been measured directly. Higher oxidation states are not established under ordinary chemical conditions.
See more information at the Lawrencium compound page.
All known lawrencium isotopes are radioactive, and safety concerns are radiological rather than ordinary chemical exposure hazards. The amounts produced are extremely small, but work with lawrencium occurs in facilities equipped for heavy-ion reactions and actinide radiochemistry. Isotope-specific half-lives and decay modes matter for handling, shielding, contamination control, and waste management. There is no known biological role.
Lawrencium has no confirmed natural environmental cycle. Any atoms produced on Earth are artificial and decay before dispersal could resemble the behavior of stable elements. In the environment, hypothetical lawrencium would be expected to follow trivalent actinide chemistry to some extent, but this has not been observed at environmental concentrations. Its ecological relevance is therefore limited to controlled laboratory production and radioactive waste from experiments.
Lawrencium has no commodity market, no bulk production, and no recycling stream. It is made only for research by bombarding heavy actinide targets, such as isotopes of californium or berkelium, with accelerated ions. Production yields are very low, often only atoms suitable for immediate detection or chemistry. The limiting factors are accelerator access, rare target materials, radiochemical separation speed, and detector capability rather than ordinary raw-material demand.
Produced by bombarding californium with boron ions.
Lawrencium is not expected to have a persistent cosmic abundance. Its known isotopes decay too rapidly to survive from stellar nucleosynthesis or the formation of the Solar System. Very short-lived lawrencium nuclei could in principle be formed in extreme neutron-rich or heavy-ion processes, but no extraterrestrial occurrence has been detected. Any natural presence would be transient and atomically scarce.
- Lawrencium chemistry is performed one atom at a time.
- Its electron configuration is anomalous, with a 7p electron in the neutral atom’s ground state.
- The element helps test where the actinide series ends and how group 3 should be described.
- Lr³⁺ is more chemically relevant than the neutral metal for experiments.
- No lawrencium compound has been isolated in visible quantity.
Images
Properties
Physical
- Van der Waals radius
- 246 pm Compare Van der Waals radius of all elements →
- Density
- 1.56 × 104 kg/m³ Compare Density of all elements →
- Phase at STP
- Solid Compare Phase at STP of all elements →
- Melting point
- 1626.85 °C Compare Melting point of all elements →
Chemical
- Electron affinity
- 0.315 eV
- Ionization energy (1st)
- 4.96 eV Compare Ionization energy (1st) of all elements →
- Ionization energy (2nd)
- 14.54005 eV Compare Ionization energy (2nd) of all elements →
- Ionization energy (3rd)
- 21.800075 eV Compare Ionization energy (3rd) of all elements →
- Ionization energy (4th)
- 43.60015 eV Compare Ionization energy (4th) of all elements →
- Ionization energy (5th)
- 56.000193 eV Compare Ionization energy (5th) of all elements →
- Oxidation states
- +3 Compare Oxidation states of all elements →
- Valence electrons
- 3 Compare Valence electrons of all elements →
- Electron configuration
- [Rn] 7s2 5f14 6d1
Thermodynamic
- Heat of sublimation
- 4.249365 eV
- Heat of atomization
- 4.249365 eV
Nuclear
- Protons
- 103 Compare Protons of all elements →
- Neutrons
- 163 Compare Neutrons of all elements →
- Known isotopes
- 16 Compare Known isotopes of all elements →
- Stable isotopes
- 0 Compare Stable isotopes of all elements →
- Mass number (most stable)
- 262
- Most stable isotope
- Lr-266
- Discovery year
- 1961
Abundance
N/A
Crystal Structure
N/A
Electronic Structure
- Electrons per shell
- 2, 8, 18, 32, 32, 8, 3 Compare Electrons per shell of all elements →
Identifiers
- CAS number
- 22537-19-5 Compare CAS number of all elements →
- Term symbol
- 2P°1/2
- InChI
- InChI=1S/Lr
- InChI Key
- CNQCVBJFEGMYDW-UHFFFAOYSA-N
Electron Configuration Measured
Lr: 5f¹⁴ 7s² 7p¹[Rn] 5f¹⁴ 7s² 7p¹1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 7s² 7p¹Atomic model
Isotopes change neutron count, mass, and stability — not the electron configuration of a neutral atom.
Schematic atomic model, not to scale.
Atomic Fingerprint
Emission / Absorption Spectrum
Isotope Distribution
No stable isotopes.
| Mass number | Atomic mass (u) | Natural abundance | Half-life |
|---|---|---|---|
| 253 Radioactive | 253.09509 ± 0.00022 | N/A | 632 ms |
| 252 Radioactive | 252.09526 ± 0.00026 | N/A | 369 ms |
| 251 Radioactive | 251.09418 ± 0.00032 | N/A | 300 us |
| 261 Radioactive | 261.10688 ± 0.00022 | N/A | 39 minutes |
| 255 Radioactive | 255.096562 ± 0.000019 | N/A | 31.1 seconds |
Phase / State
Reason: 1601.8 °C below sublimation point (1626.85 °C)
Schematic, not to scale
Phase transition points
Transition energies
Energy required to sublime 1 mol at sublimation point
Density
At standard conditions
At standard conditions
Atomic Spectra
Showing 10 of 103. Sorted by ion charge (ascending).
Levels Holdings ?
| Ion | Charge | Levels |
|---|---|---|
| Lr I | 0 | 2 |
| Lr II | +1 | 2 |
| Lr III | +2 | 2 |
| Lr IV | +3 | 2 |
| Lr V | +4 | 2 |
| Lr VI | +5 | 2 |
| Lr VII | +6 | 2 |
| Lr VIII | +7 | 2 |
| Lr IX | +8 | 2 |
| Lr X | +9 | 2 |
Crystal structure data not available
Ionic Radii
| Charge | Coordination | Spin | Radius |
|---|---|---|---|
| +3 | 9 | N/A | 107.4 pm |
Compounds
Isotopes (5)
| Mass number | Atomic mass (u) | Natural abundance | Half-life | Decay mode | |
|---|---|---|---|---|---|
| 253 Radioactive | 253.09509 ± 0.00022 | N/A | 632 ms | α =90±1%SF =1.0±0.6%β+ ? | |
| 252 Radioactive | 252.09526 ± 0.00026 | N/A | 369 ms | α ≈98%SF ≈2%β+ ? | |
| 251 Radioactive | 251.09418 ± 0.00032 | N/A | 300 us | β+ ?α ? | |
| 261 Radioactive | 261.10688 ± 0.00022 | N/A | 39 minutes | SF ≈100%α ? | |
| 255 Radioactive | 255.096562 ± 0.000019 | N/A | 31.1 seconds | α =99.7±0.1%β+ =0.3±0.1%SF ? |
Extended Properties
Covalent Radii (Extended)
- Covalent radius (Pyykkö)
- 161 pm
- Covalent radius (Pyykkö, double)
- 141 pm
Van der Waals Radii
- UFF
- 323.6 pm
Numbering Scales
- Mendeleev
- 42
- Pettifor
- 34
- Glawe
- 47
Electronegativity Scales
- Ghosh
- 0
Polarizability & Dispersion
- Dipole polarizability
- 320 a.u.
- Dipole polarizability (unc.)
- 20 a.u.
Phase Transitions & Allotropes
| Melting point | 1900.15 K |
Oxidation State Categories
Advanced Reference Data
Crystal Radii Detail (1)
| Charge | CN | Spin | rcrystal (pm) | Origin |
|---|---|---|---|---|
| 3 | IX | — | 121.4 |
Isotope Decay Modes (38)
| Isotope | Mode | Intensity |
|---|---|---|
| 251 | B+ | — |
| 251 | A | — |
| 252 | A | 98% |
| 252 | SF | 2% |
| 252 | B+ | — |
| 253 | A | 90% |
| 253 | SF | 1% |
| 253 | B+ | — |
| 254 | A | 71.7% |
| 254 | B+ | 28.3% |
Additional Data
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
References (1)
- [5] Lawrencium https://education.jlab.org/itselemental/ele103.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
References (1)
- [5] Lawrencium https://education.jlab.org/itselemental/ele103.html
References
(8)
Data deposited in or computed by PubChem
The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.
Element data are cited from the Atomic weights of the elements (an IUPAC Technical Report). The IUPAC periodic table of elements can be found at https://iupac.org/what-we-do/periodic-table-of-elements/. Additional information can be found within IUPAC publication doi:10.1515/pac-2015-0703 Copyright © 2020 International Union of Pure and Applied Chemistry.
The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.
Thomas Jefferson National Accelerator Facility (Jefferson Lab) is one of 17 national laboratories funded by the U.S. Department of Energy. The lab's primary mission is to conduct basic research of the atom's nucleus using the lab's unique particle accelerator, known as the Continuous Electron Beam Accelerator Facility (CEBAF). For more information visit https://www.jlab.org/
The periodic table at the LANL (Los Alamos National Laboratory) contains basic element information together with the history, source, properties, use, handling and more. The provenance data may be found from the link under the source name.
The periodic table contains NIST's critically-evaluated data on atomic properties of the elements. The provenance data that include data for atomic spectroscopy, X-ray and gamma ray, radiation dosimetry, nuclear physics, and condensed matter physics may be found from the link under the source name. Ref: https://www.nist.gov/pml/atomic-spectra-database
This section provides all form of data related to element Lawrencium.
