Rutherfordium (Rf)
transition-metalSolid
Standard Atomic Weight
[263]Electron configuration
[Rn] 7s2 5f14 6d2Melting point
2126.85 °C (2400 K)Boiling point
5526.85 °C (5800 K)Density
2.330000e+4 kg/m³Oxidation states
+3, +4Electronegativity (Pauling)
N/AIonization energy (1st)
Discovery year
1964Atomic radius
150 pmDetails
Rutherfordium is a synthetic transactinide element and the first member of the 6d transition-metal series. All confirmed isotopes are radioactive and short-lived, so its chemistry is studied atom by atom. Chemical experiments show behavior broadly consistent with a group 4 element, analogous to hafnium and zirconium, with the +4 oxidation state dominant in aqueous and halide systems. Relativistic effects and nuclear instability make direct measurements difficult.
Rutherfordium does not occur naturally in the Earth’s crust. Credit for the first synthesis of this element 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. The element is named for Ernest Rutherford (Fig. IUPAC.104.1), who won the Nobel Prize for developing the theory of radioactive transformations [645].
Rutherfordium is of interest in particle physics research, but it has no commercial applications. 261Rf was one of the decay products used to confirm the synthesis of copernicium in a particle accelerator experiment [634].
Rutherfordium named after Ernest Rutherford.
Scientists working at the Joint Institute for Nuclear Research in Dubna, Russia, first reported the production of rutherfordium in 1964. They bombarded atoms of plutonium-242 with ions of neon-22, forming what they believed to be atoms of rutherfordium-260 and four free neutrons. In 1969, a group of scientists working at the Lawrence Radiation Laboratory, now known as the Lawrence Berkeley Laboratory, in Berkeley, California, attempted to confirm the Dubna group's discovery. Lacking the equipment needed to accelerate neon ions, the Berkeley group, led by Albert Ghiorso, bombarded atoms of californium-248 and californium-249 with ions of carbon-12 and carbon-13, producing atoms of rutherfordium-257, rutherfordium-258, rutherfordium-259 and rutherfordium-261. They were, however, unable to produce the same isotope as the Dubna group. Credit for the discovery of rutherfordium is still under debate. Rutherfordium's most stable isotope, rutherfordium-263, has a half-life of about 10 minutes and decays through spontaneous fission.
In 1964, workers at the Joint Nuclear Research Institute at Dubna (U.S.S.R.) bombarded plutonium with accelerated 113 to 115 MeV neon ions. By measuring fission tracks in a special glass with a microscope, they detected an isotope that decays by spontaneous fission. They suggested that this isotope, which had a half-life of 0.3 +/- 0.1 s might be 260-104, produced by the following reaction: 242Pu + 22Ne >260Rf +4n.
Element 104, the first transactinide element, is expected to have chemical properties similar to those of hafnium. It would, for example, form a relatively volatile compound with chlorine (a tetrachloride).
The Soviet scientists have performed experiments aimed at chemical identification, and have attempted to show that the 0.3-s activity is more volatile than that of the relatively nonvolatile actinide trichlorides. This experiment does not fulfill the test of chemically separating the new element from all others, but it provides important evidence for evaluation. Data issued by Soviet scientists reduced the half-life of the isotope they worked with from 0.3 to 0.15 s.
Images
Properties
Physical
Chemical
Thermodynamic
N/A
Nuclear
Abundance
N/A
Reactivity
N/A
Crystal Structure
N/A
Electronic Structure
Identifiers
Electron Configuration Predicted
Rf: 5f¹⁴ 6d² 7s²[Rn] 5f¹⁴ 6d² 7s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹⁴ 6d² 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 |
|---|---|---|---|
| 262 Radioactive | 262.10992 ± 0.00024 | N/A | 250 ms |
| 254 Radioactive | 254.10005 ± 0.0003 | N/A | 22.9 us |
| 260 Radioactive | 260.10644 ± 0.00022 | N/A | 21 ms |
| 253 Radioactive | 253.10044 ± 0.00044 | N/A | 13 ms |
| 258 Radioactive | 258.103428 ± 0.000034 | N/A | 12.5 ms |
Phase / State
Reason: 2101.8 °C below melting point (2126.85 °C)
Schematic, not to scale
Phase transition points
Density
At standard conditions
At standard conditions
Atomic Spectra
Showing 10 of 93 Atomic Spectra. Sorted by ion charge (ascending).
Levels Holdings ?
| Ion | Charge | Levels |
|---|---|---|
| Rf I | 0 | 2 |
| Rf II | +1 | 2 |
| Rf III | +2 | 2 |
| Rf IV | +3 | 2 |
| Rf V | +4 | 2 |
| Rf VI | +5 | 2 |
| Rf VII | +6 | 2 |
| Rf VIII | +7 | 2 |
| Rf IX | +8 | 2 |
| Rf X | +9 | 2 |
Crystal structure data not available
Compounds
Isotopes (5)
In 1969 Ghiorso, Nurmia, Harris, K.A.Y. Eskola, and P.L. Eskola of the University of California at Berkeley reported that they had positively identified two, and possibly three isotopes of Element 104. The group indicated that, after repeated attempts, they produced isotope 260104 reported by the Dubna groups in 1964.
| Mass number | Atomic mass (u) | Natural abundance | Half-life | Decay mode | |
|---|---|---|---|---|---|
| 262 Radioactive | 262.10992 ± 0.00024 | N/A | 250 ms | SF ≈100% | |
| 254 Radioactive | 254.10005 ± 0.0003 | N/A | 22.9 us | SF ≈100%α<1.5% | |
| 260 Radioactive | 260.10644 ± 0.00022 | N/A | 21 ms | SF ≈100%α ?β+ ? | |
| 253 Radioactive | 253.10044 ± 0.00044 | N/A | 13 ms | SF ≈100%α ? | |
| 258 Radioactive | 258.103428 ± 0.000034 | N/A | 12.5 ms | SF =95.1±1.6%α =4.9±1.6% |
Extended Properties
Covalent Radii (Extended)
Numbering Scales
Polarizability & Dispersion
Oxidation State Categories
Advanced Reference Data
Isotope Decay Modes (33)
| Isotope | Mode | Intensity |
|---|---|---|
| 253 | SF | 100% |
| 253 | A | — |
| 254 | SF | 100% |
| 254 | A | 1.5% |
| 255 | A | 52.8% |
| 255 | SF | 47.2% |
| 255 | B+ | 6% |
| 256 | SF | 99.7% |
| 256 | A | 0.3% |
| 257 | A | 89.3% |
Additional Data
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
References (1)
- [5] Rutherfordium https://education.jlab.org/itselemental/ele104.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
References (1)
- [5] Rutherfordium https://education.jlab.org/itselemental/ele104.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 Rutherfordium.
