Curium (Cm)
actinideSolid
Standard Atomic Weight
[247]Electron configuration
[Rn] 7s2 5f7 6d1Melting point
1344.85 °C (1618 K)Boiling point
3126.85 °C (3400 K)Density
1.351000e+4 kg/m³Oxidation states
+3, +4, +5, +6Electronegativity (Pauling)
1.3Ionization energy (1st)
Discovery year
1944Atomic radius
N/ADetails
Curium is a synthetic transuranium actinide named for Marie and Pierre Curie. It is produced in nuclear reactors by successive neutron capture in plutonium and americium, and all of its isotopes are radioactive. Chemically it is a typical later actinide, dominated by the +3 oxidation state in water and by compounds resembling those of americium and the lanthanides. Its most important practical feature is the intense alpha emission of selected isotopes, especially ²⁴⁴Cm.
Curium does not occur naturally in the Earth’s crust. It was first synthesized in 1944 by Glenn T. Seaborg and his team at the University of California in Berkeley using the reaction 239Pu (4He, n) 242Cm. The element was named after Pierre and Marie Curie, who discovered radium and polonium.
Minute amounts of curium probably exist in natural deposits of uranium, as a result of a sequence of neutron captures and beta decays sustained by the very low flux of neutrons naturally present in uranium ores. The presence of natural curium, however, has never been detected. 242Cm and 244Cm are available in multigram quantities. 248Cm has been produced only in milligram amounts. Curium is similar in some regards to gadolinium, its rare earth homolog, but it has a more complex crystal structure. Curium metal is lustrous, malleable, silver in color, chemically reactive, and is more electropositive than aluminum. Curium metal exist in two crystal forms, a double hexagonal close packed (dhcp) and a high temperature face-centered cubic close packed (fcc) structure. Metallic curium dissolves rapidly in dilute acid to form Cm(III) solutions. Curium metal surfaces rapidly oxidize in air to form a thin film possibly starting out as CmO, Oxidation then progressing to Cm2O3, and eventually to form stable CmO2. Note however that the formation of divalent compounds of curium such as CmO have never been observed in bulk form. Most compounds and solutions of trivalent curium are quite stable and are faintly yellow or yellow-green in color. The stability of the trivalent state for curium is attributed to the half-filled 5f7 electron shell configuration. Curium in the tetravalent state is meta-stable in concentrated fluoride solutions but very stable in the solid state, primarily as the oxides and fluorides. Because curium isotopes are available in macro quantities a number of curium compounds have been prepared and characterized with the majority in the trivalent state.
242Cm generates about three watts of thermal energy per gram. This compares to one-half watt per gram of 238Pu. Both 242Cm and 244Cm have been used as power sources for space and medical uses. 244Cm is now offered for sale at $100/mg. Curium absorbed into the body accumulates in the bones, and is therefore very toxic as its radiation destroys the red-cell forming mechanism. The maximum permissible total body burden of 244Cm (soluble) in a human being is 0.3 microcurie.
This element reviewed and Updated by Dr. David Hobart, 2011
Curium was first produced by Glenn T. Seaborg, Ralph A. James and Albert Ghiorso, working at the University of California, Berkeley, in 1944. They bombarded atoms of plutonium-239, an isotope of plutonium, with alpha particles that had been accelerated in a device called a cyclotron. This produced atoms of curium-242 and one free neutron. Curium-242 has a half-life of about 163 days and decays into plutonium-238 through alpha decay or decays through spontaneous fission. Curium's most stable isotope, curium-247, has a half-life of about 15,600,000 years. It decays into plutonium-243 through alpha decay.
Although curium follows americium in the periodic system, it was actually the third transuranium element to be discovered. It was identified by Seaborg, James, and Ghiorso in 1944 at the wartime metallurgical laboratory at the University of Chicago as a result of helium-ion bombardment of 239Pu in the Berkeley, California, 60-inch cyclotron. Visible amounts (30 µg) of 242Cm, in the form of the hydroxide, were first isolated by Werner and Perlman of the University of California in 1947. In 1950, Crane, Wallmann, and Cunningham found that the magnetic susceptibility of microgram samples of CmF3 was of the same magnitude as that of GdF3. This provided direct experimental evidence for assigning an electronic configuration to Cm+3. In 1951, the same workers prepared curium in its elemental form for the first time. Fourteen isotopes of curium are now known ranging in mass from 237 to 251. The most stable, 247Cm, with a half-life of 16 million years, is so short compared to the earth's age that any primordial curium must have disappeared long ago from the natural scene.
Images
Properties
Physical
Chemical
Thermodynamic
Nuclear
Abundance
N/A
Reactivity
N/A
Crystal Structure
N/A
Electronic Structure
Identifiers
Electron Configuration Measured
Cm: 5f⁷ 6d¹ 7s²[Rn] 5f⁷ 6d¹ 7s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f⁷ 6d¹ 7s²Atomic 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 |
|---|---|---|---|
| 250 Radioactive | 250.078358 ± 0.000012 | N/A | 8300 years |
| 248 Radioactive | 248.0723499 ± 0.0000056 | N/A | 348 ky |
| 242 Radioactive | 242.058836 ± 0.0000019 | N/A | 162.8 days |
| 249 Radioactive | 249.0759548 ± 0.0000056 | N/A | 64.15 minutes |
| 234 Radioactive | 234.05016 ± 0.00002 | N/A | 52 seconds |
Phase / State
Reason: 3101.8 °C below sublimation point (3126.85 °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 96 Atomic Spectra. Sorted by ion charge (ascending).
Lines Holdings ?
| Ion | Charge | Total lines | Transition probabilities | Level designations |
|---|---|---|---|---|
| Cm I | 0 | 140 | 0 | 0 |
| Cm II | +1 | 32 | 0 | 0 |
Levels Holdings ?
| Ion | Charge | Levels |
|---|---|---|
| Cm I | 0 | 2 |
| Cm II | +1 | 2 |
| Cm III | +2 | 2 |
| Cm IV | +3 | 2 |
| Cm V | +4 | 2 |
| Cm VI | +5 | 2 |
| Cm VII | +6 | 2 |
| Cm VIII | +7 | 2 |
| Cm IX | +8 | 2 |
| Cm X | +9 | 2 |
Crystal structure data not available
Ionic Radii
| Charge | Coordination | Spin | Radius |
|---|---|---|---|
| +3 | 6 | N/A | 97 pm |
| +3 | 9 | N/A | 114.7 pm |
| +4 | 6 | N/A | 85 pm |
| +4 | 8 | N/A | 95 pm |
Compounds
Isotopes (5)
| Mass number | Atomic mass (u) | Natural abundance | Half-life | Decay mode | |
|---|---|---|---|---|---|
| 250 Radioactive | 250.078358 ± 0.000012 | N/A | 8300 years | SF ≈74%α ?β- ? | |
| 248 Radioactive | 248.0723499 ± 0.0000056 | N/A | 348 ky | α =91.61±1.6%SF =8.39±1.6%2β- ? | |
| 242 Radioactive | 242.058836 ± 0.0000019 | N/A | 162.8 days | α =100%SF =6.2e-6±0.3%34Si =1.1e-14±0.4% | |
| 249 Radioactive | 249.0759548 ± 0.0000056 | N/A | 64.15 minutes | β- =100% | |
| 234 Radioactive | 234.05016 ± 0.00002 | N/A | 52 seconds | β+ ≈71%α ≈27%SF ≈2% |
Extended Properties
Covalent Radii (Extended)
Van der Waals Radii
Atomic & Metallic Radii
Numbering Scales
Electronegativity Scales
Polarizability & Dispersion
Phase Transitions & Allotropes
| Melting point | 1618.15 K |
Oxidation State Categories
Advanced Reference Data
Crystal Radii Detail (4)
| Charge | CN | Spin | rcrystal (pm) | Origin |
|---|---|---|---|---|
| 3 | VI | 111 | from r^3 vs V plots, | |
| 4 | VI | 99 | from r^3 vs V plots, | |
| 4 | VIII | 109 | from r^3 vs V plots, | |
| 3 | IX | — | 128.7 |
Isotope Decay Modes (50)
| Isotope | Mode | Intensity |
|---|---|---|
| 231 | B+ | — |
| 231 | A | — |
| 232 | B+ | — |
| 232 | A | — |
| 233 | A | 20% |
| 233 | B+ | 80% |
| 234 | B+ | 71% |
| 234 | A | 27% |
| 234 | SF | 2% |
| 235 | B+ | — |
Additional Data
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
References (1)
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
References (1)
References
(9)
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 Curium.
The element property data was retrieved from publications.
