Einsteinium (Es)
actinideSolid
Standard Atomic Weight
[252]Electron configuration
[Rn] 7s2 5f11Melting point
859.85 °C (1133 K)Boiling point
N/ADensity
8840 kg/m³Oxidation states
+2, +3, +4Electronegativity (Pauling)
1.3Ionization energy (1st)
Discovery year
1952Atomic radius
N/ADetails
Einsteinium is a synthetic actinide with atomic number 99. It was first identified in debris from a thermonuclear test, and it is now made only in minute amounts by intense neutron irradiation of lighter actinides. Its chemistry is dominated by the +3 oxidation state and resembles that of neighboring trivalent actinides and lanthanides. The element is important mainly as a research material and as a target for producing still heavier elements.
Einsteinium does not occur naturally in the Earth’s crust. It was first identified in December 1952 by American scientists from the Argonne National Laboratory near Chicago, Illinois, the Los Alamos National Laboratory in Los Alamos, New Mexico, and The University of California Laboratory in Berkeley, California in the debris of thermonuclear weapons. The element was named for Albert Einstein (Fig. IUPAC.99.1). 253Es was the first isotope identified; it has a half-life of 20.47 days. The isotope with the longest half-life is 252Es, with a half-life of 472 days [630], [631].
There are no uses for isotopes of einsteinium outside of basic scientific research for the production of higher transuranic elements and studies of actinide science. Due to the radiation and heat given off by einsteinium isotopes, it is difficult to use them in experiments and studies [631].
Tracer studies using 253Es show that einsteinium has chemical properties typical of a heavy trivalent, actinide element. Oxidation states of II and III for einsteinium have been reported and oxidation state IV has been postulated from vapor transport studies but not established unequivocally. Einsteinium is the first divalent metal in the actinide series (two bonding electrons rather than three). The self-irradiation properties of einsteinium make it extremely difficult, for example, to obtain x-ray crystallographic data. The intense gamma and x-rays from einsteinium decay to daughter products over-exposes the x-ray film/detector. This intense self-irradiation can be exploited however to study accelerated aging and radiation damage studies, and for targeted radiation medical treatments. An example of einsteinium chemical studies is the chemical consequences of radioactive decay. With the relatively short half-life of Es-253 (20.47 days) one can study the in-growth of daughter Bk-249 (half-life 330 days) and grand-daughter Cf-249 (half-life 351 years). Evidence suggests that divalent Es might decay into a divalent Bk daughter and subsequently into as of yet unknown divalent Cf. There are no commercial uses for einsteinium however it is the heaviest element for which bulk studies can be performed that allows for fundamental studies of the role of 5-f electrons in actinide systematics.
Further reading:
Richard G. Haire (2006) Chapter 12, The Chemistry of the Actinide and Transactinide Elements, Third Edition, L. R. Morss, J. Fuger, and N. M. Edelstein, Eds, Springer Publishers.
This element reviewed and Updated by Dr. David Hobart, 2011
Einsteinium was discovered by a team of scientists led by Albert Ghiorso in 1952 while studying the radioactive debris produced by the detonation of the first hydrogen bomb. The isotope they discovered, einsteinium-253, has a half-life of about 20 days and was produced by combining 15 neutrons with uranium-238, which then underwent seven beta decays. Today, einsteinium is produced though a lengthy chain of nuclear reactions that involves bombarding each isotope in the chain with neutrons and then allowing the resulting isotope to undergo beta decay. Einsteinium's most stable isotope, einsteinium-252, has a half-life of about 471.7 days. It decays into berkelium-248 through alpha decay or into californium-252 through electron capture.
Einsteinium, the seventh transuranic element of the actinide series to be discovered, was identified by Ghiorso and co-workers at Berkeley in December 1952 in debris from the first large thermonuclear explosion, which took place in the Pacific in November, 1952. The 20-day 253Es isotope was produced. It was named after Albert Einstein.
In 1961, enough einsteinium was produced to separate a macroscopic amount of 253Es. This sample weighted about 0.01µg and was measured using a special magnetic-type balance. 253Es so produced was used to produce mendelevium (Element 101) by neutron bombardment.
About 3 µg of einsteinium has been produced in the High Flux Isotope Reactor (HFIR) at Oak Ridge National Laboratories by:
▸ irradiating kilogram quantities of 239Pu in a reactor for several years to produce 242Pu,
▸ fabricating the 242Pu into pellets of plutonium oxide and aluminum powder,
▸ loading the pellets into target rods for an initial 1-year irradiation at the Savannah River Plant, and,
▸ irradiating the targets for another 4 months in the HFIR.
The targets were then removed for chemical separation of the einsteinium from californium daughter products. About 2 milligrams of einsteinium can be present in special HFIR campaigns.
Images
Properties
Physical
Chemical
Thermodynamic
Nuclear
Abundance
N/A
Reactivity
N/A
Crystal Structure
N/A
Electronic Structure
Identifiers
Electron Configuration Measured
Es: 5f¹¹ 7s²[Rn] 5f¹¹ 7s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹¹ 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 |
|---|---|---|---|
| 252 Radioactive | 252.08298 ± 0.000054 | N/A | 471.7 days |
| 254 Radioactive | 254.0880222 ± 0.0000045 | N/A | 275.7 days |
| 249 Radioactive | 249.076411 ± 0.000032 | N/A | 102.2 minutes |
| 255 Radioactive | 255.090275 ± 0.000012 | N/A | 39.8 days |
| 244 Radioactive | 244.07088 ± 0.0002 | N/A | 37 seconds |
Phase / State
Reason: 834.9 °C below sublimation point (859.85 °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 99 Atomic Spectra. Sorted by ion charge (ascending).
Lines Holdings ?
| Ion | Charge | Total lines | Transition probabilities | Level designations |
|---|---|---|---|---|
| Es I | 0 | 11 | 0 | 0 |
| Es II | +1 | 12 | 0 | 0 |
Levels Holdings ?
| Ion | Charge | Levels |
|---|---|---|
| Es I | 0 | 2 |
| Es II | +1 | 2 |
| Es III | +2 | 2 |
| Es IV | +3 | 2 |
| Es V | +4 | 2 |
| Es VI | +5 | 2 |
| Es VII | +6 | 2 |
| Es VIII | +7 | 2 |
| Es IX | +8 | 2 |
| Es X | +9 | 2 |
Crystal structure data not available
Ionic Radii
| Charge | Coordination | Spin | Radius |
|---|---|---|---|
| +3 | 9 | N/A | 111.6 pm |
Compounds
Isotopes (5)
Sixteen isotopes with three isomers ranging in atomic mass from 241 to 256 are now recognized for einsteinium. 252Es has the longest half-life (472 days) but is only available in minute quantities. The isotopes 253Es and 254Es are the isotopes of choice for physicochemical studies because of their availability and reasonable half-lives. However, usually only a few micrograms of einsteinium isotopes are used in experiments to reduce worker exposure and to minimize the intense self-irradiation effects.
| Mass number | Atomic mass (u) | Natural abundance | Half-life | Decay mode | |
|---|---|---|---|---|---|
| 252 Radioactive | 252.08298 ± 0.000054 | N/A | 471.7 days | α =78±0.2%ε =22±0.2% | |
| 254 Radioactive | 254.0880222 ± 0.0000045 | N/A | 275.7 days | α ≈100%ε ?β- =1.74e-4±0.8% | |
| 249 Radioactive | 249.076411 ± 0.000032 | N/A | 102.2 minutes | β+ ≈100%α =0.57±0.8% | |
| 255 Radioactive | 255.090275 ± 0.000012 | N/A | 39.8 days | β- =92.0±0.4%α =8.0±0.4%SF =0.0041±0.2% | |
| 244 Radioactive | 244.07088 ± 0.0002 | N/A | 37 seconds | β+ =95±0.3%α =5±0.3%β+SF =0.011±0.4% |
Extended Properties
Covalent Radii (Extended)
Van der Waals Radii
Numbering Scales
Electronegativity Scales
Polarizability & Dispersion
Phase Transitions & Allotropes
| Melting point | 1133.15 K |
Oxidation State Categories
Advanced Reference Data
Crystal Radii Detail (1)
| Charge | CN | Spin | rcrystal (pm) | Origin |
|---|---|---|---|---|
| 3 | IX | — | 125.6 |
Isotope Decay Modes (51)
| Isotope | Mode | Intensity |
|---|---|---|
| 239 | A | — |
| 239 | B+ | — |
| 239 | SF | — |
| 240 | A | 70% |
| 240 | B+ | 30% |
| 240 | B+SF | 0.2% |
| 241 | A | 100% |
| 241 | B+ | — |
| 242 | A | 57% |
| 242 | B+ | 43% |
Additional Data
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
References (1)
- [5] Einsteinium https://education.jlab.org/itselemental/ele099.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
References (1)
- [5] Einsteinium https://education.jlab.org/itselemental/ele099.html
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 Einsteinium.
The element property data was retrieved from publications.
