Darmstadtium (Ds)
transition-metalExpected to be a Solid
Standard Atomic Weight
[281]Electron configuration
[Rn] 7s2 5f14 6d8(predicted)Melting point
N/ABoiling point
N/ADensity
3.480000e+4 kg/m³Oxidation states
0, +2, +4, +6, +8Electronegativity (Pauling)
N/AIonization energy (1st)
Discovery year
1994Atomic radius
132 pmDetails
Darmstadtium is a synthetic transactinide element in group 10, below nickel, palladium, and platinum. It has been produced only atom by atom in heavy-ion fusion experiments and identified from its radioactive decay chains. Its chemistry is largely unmeasured; theoretical work treats it as a very heavy platinum-group metal, with strong relativistic effects expected to influence bonding and volatility.
Darmstadtium does not occur naturally in the Earth’s crust. Darmstadtium was first synthesized by an international team of scientists from the GSI in Darmstadt, Germany, the Joint Institute for Nuclear Research (JINR) in Dubna, Russia, the Comenius University in Bratislava, Slovakia and the University of Jyväskylä, Finland at the GSI Helmholtz Center for Heavy Ion Research in Darmstadt (Fig. IUPAC.110.1), Germany in 1994 using the nuclear reaction 208Pb (62Ni, n) 269Ds. The element was named darmstadtium after the place where the first synthesis was made [656], [657], [658], [659]. Darmstadtium has no known isotopic applications aside from scientific research.
Darmstadtium is named after the city Darmstadt, Germany.
Darmstadtium was first produced by Peter Armbruster, Gottfried Münzenber and their team working at the Gesellschaft für Schwerionenforschung in Darmstadt, Germany on November 9th, 1994. They bombarded atoms of lead with ions of nickel with a device known as a linear accelerator. This produced one atom of darmstadtium-269, an isotope with a half-life of about 0.17 milliseconds (0.00017 seconds), after at least a billion billion (1,000,000,000,000,000,000) nickel ions were fired at the lead target over the course of a week. Darmstadtium's most stable isotope, darmstadtium-281, has a half-life of about 20 seconds. About 15% of the time, it decays into hassium-277 through alpha decay. The remaining 85% of the time, it decays through spontaneous fission.
November 9, 1994 at 4:39 pm, the first atom with atomic number 110 was detected at the Gesellschaft fur Schwerionenforschung (GSI) in Darmstadt, in Germany.
Element 110 was produced by fusing a nickel and lead atom together. This was achieved by accelerating the nickel atoms to a high energy in the heavy ion accelerator."This rare reaction occurs only at a very specific velocity of the nickel projectile. Over a period of many days, many billion billion nickel atoms must be shot at a lead target in order to produce and identify a single atom of element 110. The atoms produced in the nickel-lead collisions are selected by a velocity filter and then captured in a detector system which measures their decay. The energy of the emitted helium nuclei serves to identify the atom" (Press Release). This element was only found to have a lifetime of less than 1/1000th of a second. It is expected that soon a heavier version of element 110 that might be more stable, and that lives slightly longer will be developed.
The name darmstatdium was confirmed by IUPAC in August 2003.
Images
Properties
Physical
Chemical
Thermodynamic
N/A
Nuclear
Abundance
N/A
Reactivity
N/A
Crystal Structure
N/A
Electronic Structure
Identifiers
Electron Configuration Predicted
——Electron configuration data not available for this ion.
Atomic model
Isotopes change neutron count, mass, and stability — not the electron configuration of a neutral atom.
N/A
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 |
|---|---|---|---|
| 278 Radioactive | 278.15704 ± 0.00067 | N/A | 270 ms |
| 273 Radioactive | 273.14856 ± 0.00014 | N/A | 240 us |
| 269 Radioactive | 269.144752 ± 0.000034 | N/A | 230 us |
| 279 Radioactive | 279.1601 ± 0.00064 | N/A | 210 ms |
| 270 Radioactive | 270.144584 ± 0.000052 | N/A | 205 us |
Phase / State
Phase/state data not available
Atomic Spectra
Showing 10 of 94 Atomic Spectra. Sorted by ion charge (ascending).
Levels Holdings ?
| Ion | Charge | Levels |
|---|---|---|
| Ds VI | +5 | 2 |
| Ds VII | +6 | 1 |
| Ds VIII | +7 | 1 |
| Ds IX | +8 | 2 |
| Ds X | +9 | 2 |
| Ds XI | +10 | 2 |
| Ds XII | +11 | 2 |
| Ds XIII | +12 | 2 |
| Ds XIV | +13 | 2 |
| Ds XV | +14 | 2 |
Phase/state data not available
Compounds
Isotopes (5)
| Mass number | Atomic mass (u) | Natural abundance | Half-life | Decay mode | |
|---|---|---|---|---|---|
| 278 Radioactive | 278.15704 ± 0.00067 | N/A | 270 ms | α ?SF ? | |
| 273 Radioactive | 273.14856 ± 0.00014 | N/A | 240 us | α ≈100% | |
| 269 Radioactive | 269.144752 ± 0.000034 | N/A | 230 us | α =100% | |
| 279 Radioactive | 279.1601 ± 0.00064 | N/A | 210 ms | SF =88±0.5%α =12±0.5% | |
| 270 Radioactive | 270.144584 ± 0.000052 | N/A | 205 us | α ≈100%SF ? |
Extended Properties
Covalent Radii (Extended)
Numbering Scales
Polarizability & Dispersion
Oxidation State Categories
Advanced Reference Data
Isotope Decay Modes (30)
| Isotope | Mode | Intensity |
|---|---|---|
| 267 | A | 100% |
| 268 | A | — |
| 269 | A | 100% |
| 270 | A | 100% |
| 270 | SF | — |
| 271 | SF | 75% |
| 271 | A | 25% |
| 272 | SF | — |
| 273 | A | 100% |
| 274 | A | — |
Additional Data
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
References (1)
- [5] Darmstadtium https://education.jlab.org/itselemental/ele110.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
References (1)
- [5] Darmstadtium https://education.jlab.org/itselemental/ele110.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.
This section provides all form of data related to element Darmstadtium.
