Einsteinium (Es)
actinideSolid
Peso atomico standard
[252]Configurazione elettronica
[Rn] 7s2 5f11Punto di fusione
859,85 °CPunto di ebollizione
N/DDensità
8840 kg/m³Stati di ossidazione
+2, +3, +4Elettronegatività (Pauling)
1,3Energia di ionizzazione (1ª)
6,3684 eVAnno della scoperta
1952Raggio atomico
N/DDettagli
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.
Only microgram-scale samples have been isolated, so ordinary bulk appearance is not well established. Metallic einsteinium has not been characterized like common metals; many physical properties are measured with difficulty or inferred from very small samples.
Einsteinium has no commercial use. Its main use is in nuclear and chemical research, especially in studies of heavy-actinide chemistry and radiation effects in solids. ²⁵³Es has been used as a target material for producing mendelevium and other heavier nuclei in accelerator experiments. Because it is scarce, intensely radioactive, and self-heating, its use is limited to specialized laboratories with radiochemical facilities.
Since only small amounts of einsteinium have ever been produced, it currently has no uses outside of basic scientific research.
Einsteinium chemistry is known from tracer and microgram-scale work. The most stable common oxidation state in solution is Es³⁺, which forms salts and coordination complexes broadly similar to those of other trivalent actinides. Reported compounds include einsteinium(III) chloride, EsCl₃, einsteinium(III) bromide, EsBr₃, and einsteinium(III) oxide, Es₂O₃. A divalent state has been observed under reducing conditions in some systems, but +3 remains the principal aqueous and solid-state chemistry.
See more information at the Einsteinium compound page.
All einsteinium isotopes are radioactive, and hazards depend strongly on the isotope and amount. Important risks include external gamma or X-ray exposure from associated decay products, internal alpha exposure if material is inhaled or ingested, and heat generation in concentrated samples. Handling requires shielded, contamination-controlled radiochemical equipment. No biological role is known.
Einsteinium has no meaningful natural environmental cycle. Any natural occurrence would be transient and extraordinarily rare, produced by neutron capture in exceptional nuclear events and quickly lost by radioactive decay. Environmental releases are associated only with nuclear activities or laboratory material, where behavior is governed by actinide chemistry, sorption to minerals, complexation, and isotope-specific decay.
Einsteinium is not a commodity and has no normal market. It is produced in specialized high-flux reactors by prolonged neutron irradiation of plutonium, curium, or other actinide targets, followed by difficult radiochemical separation from neighboring transplutonium elements. Production yields are tiny, and the material decays during and after processing. Supply is therefore episodic, institutionally controlled, and directed almost entirely to research experiments rather than industrial demand.
Made by bombarding uranium with neutrons.
Einsteinium is not a primordial element and has no stable isotopes. In the universe it can be formed only in environments with intense neutron capture, such as nuclear explosions or possibly extreme astrophysical r-process events, but any atoms produced decay on short geological timescales. It is not expected to persist in planets, meteorites, or stellar material except as a transient radionuclide.
- The first einsteinium atoms were found in fallout from the 1952 Ivy Mike thermonuclear test.
- ²⁵³Es is often the most useful isotope for chemistry because it can be made in measurable microgram quantities.
- Self-irradiation damages einsteinium compounds and can alter measurements during an experiment.
- Einsteinium helped enable the first synthesis of mendelevium.
- Separation from californium and other neighboring actinides is one of the main practical difficulties.
Immagini
Proprietà
Fisiche
- Raggio di van der Waals
- 245 pm Confronta Raggio di van der Waals di tutti gli elementi →
- Densità
- 8840 kg/m³ Confronta Densità di tutti gli elementi →
- Fase in condizioni STP
- Solido Confronta Fase in condizioni STP di tutti gli elementi →
- Punto di fusione
- 859,85 °C Confronta Punto di fusione di tutti gli elementi →
Chimiche
- Elettronegatività (Pauling)
- 1,3 Confronta Elettronegatività (Pauling) di tutti gli elementi →
- Affinità elettronica
- -0,3 eV (valore negativo — l'atomo non dovrebbe legare un elettrone extra)
- Energia di ionizzazione (1ª)
- 6,3684 eV Confronta Energia di ionizzazione (1ª) di tutti gli elementi →
- Energia di ionizzazione (2ª)
- 12,200042 eV Confronta Energia di ionizzazione (2ª) di tutti gli elementi →
- Energia di ionizzazione (3ª)
- 22,700078 eV Confronta Energia di ionizzazione (3ª) di tutti gli elementi →
- Energia di ionizzazione (4ª)
- 38,800134 eV Confronta Energia di ionizzazione (4ª) di tutti gli elementi →
- Energia di ionizzazione (5ª)
- 54,100186 eV Confronta Energia di ionizzazione (5ª) di tutti gli elementi →
- Stati di ossidazione
- +2, +3, +4 Confronta Stati di ossidazione di tutti gli elementi →
- Elettroni di valenza
- 3 Confronta Elettroni di valenza di tutti gli elementi →
- Configurazione elettronica
- [Rn] 7s2 5f11
Termodinamiche
- Calore di sublimazione
- 3,990258 eV
- Calore di atomizzazione
- 3,990258 eV
- Entalpia di atomizzazione
- 1,378453 eV
Nucleari
- Protoni
- 99 Confronta Protoni di tutti gli elementi →
- Neutroni
- 153 Confronta Neutroni di tutti gli elementi →
- Isotopi noti
- 20 Confronta Isotopi noti di tutti gli elementi →
- Isotopi stabili
- 0 Confronta Isotopi stabili di tutti gli elementi →
- Numero di massa (isotopo più stabile)
- 252
- Isotopo più stabile
- Es-252
- Anno della scoperta
- 1952
Abbondanza
N/D
Struttura cristallina
N/D
Struttura elettronica
- Elettroni per guscio
- 2, 8, 18, 32, 29, 8, 2 Confronta Elettroni per guscio di tutti gli elementi →
Identificativi
- Numero CAS
- 7429-92-7 Confronta Numero CAS di tutti gli elementi →
- Simbolo di termine
- 4I°15/2
- InChI
- InChI=1S/Es
- Chiave InChI
- CKBRQZNRCSJHFT-UHFFFAOYSA-N
Configurazione elettronica Misurato
Es: 5f¹¹ 7s²[Rn] 5f¹¹ 7s²1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹¹ 7s²Modello atomico
Gli isotopi modificano il numero di neutroni, la massa e la stabilità — non la configurazione elettronica di un atomo neutro.
Modello atomico schematico, non in scala.
Impronta atomica
Spettro di emissione / assorbimento
Distribuzione isotopica
Nessun isotopo stabile.
| Numero di massa | Massa atomica (u) | Abbondanza naturale | Emivita |
|---|---|---|---|
| 252 Radioattivo | 252,08298 ± 0,000054 | N/D | 471.7 giorni |
| 254 Radioattivo | 254,0880222 ± 0,0000045 | N/D | 275.7 giorni |
| 249 Radioattivo | 249,076411 ± 0,000032 | N/D | 102.2 minuti |
| 255 Radioattivo | 255,090275 ± 0,000012 | N/D | 39.8 giorni |
| 244 Radioattivo | 244,07088 ± 0,0002 | N/D | 37 secondi |
Fase / Stato
Motivo: 834,9 °C sotto il punto di sublimazione (859,85 °C)
Schema non in scala
Punti di transizione di fase
Energie di transizione
Energia necessaria per sublimare 1 mol al punto di sublimazione
Densità
In condizioni standard
In condizioni standard
Spettri atomici
Sono visualizzati 10 di 99. Ordinamento per carica ionica crescente.
Righe disponibili ?
| Ione | Carica | Righe totali | Probabilità di transizione | Designazioni dei livelli |
|---|---|---|---|---|
| Es I | 0 | 11 | 0 | 0 |
| Es II | +1 | 12 | 0 | 0 |
Livelli disponibili ?
| Ione | Carica | Livelli |
|---|---|---|
| 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 |
Dati sulla struttura cristallina non disponibili
Raggi ionici
| Carica | Coordinazione | Spin | Raggio |
|---|---|---|---|
| +3 | 9 | N/D | 111.6 pm |
Composti
Isotopi (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.
| Numero di massa | Massa atomica (u) | Abbondanza naturale | Emivita | Modalità di decadimento | |
|---|---|---|---|---|---|
| 252 Radioattivo | 252,08298 ± 0,000054 | N/D | 471.7 giorni | α =78±0.2%ε =22±0.2% | |
| 254 Radioattivo | 254,0880222 ± 0,0000045 | N/D | 275.7 giorni | α ≈100%ε ?β- =1.74e-4±0.8% | |
| 249 Radioattivo | 249,076411 ± 0,000032 | N/D | 102.2 minuti | β+ ≈100%α =0.57±0.8% | |
| 255 Radioattivo | 255,090275 ± 0,000012 | N/D | 39.8 giorni | β- =92.0±0.4%α =8.0±0.4%SF =0.0041±0.2% | |
| 244 Radioattivo | 244,07088 ± 0,0002 | N/D | 37 secondi | β+ =95±0.3%α =5±0.3%β+SF =0.011±0.4% |
Proprietà estese
Raggi covalenti (dati estesi)
- Raggio covalente (Pyykkö)
- 165 pm
- Raggio covalente (Pyykkö, legame doppio)
- 140 pm
Raggi di van der Waals
- Alvarez
- 270 pm
- UFF
- 329,9 pm
Scale di numerazione
- Mendeleev
- 34
- Pettifor
- 38
- Glawe
- 43
Scale di elettronegatività
- Ghosh
- 0
Polarizzabilità e dispersione
- Polarizzabilità dipolare
- 118 a.u.
- Polarizzabilità dipolare (inc.)
- 20 a.u.
Transizioni di fase e allotropi
| Punto di fusione | 1133,15 K |
Categorie degli stati di ossidazione
Dati di riferimento avanzati
Dettaglio dei raggi cristallini (1)
| Carica | CN | Spin | rcrystal (pm) | Origine |
|---|---|---|---|---|
| 3 | IX | — | 125,6 |
Modalità di decadimento degli isotopi (51)
| Isotopo | Modalità | Intensità |
|---|---|---|
| 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% |
Dati aggiuntivi
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
Not Applicable
Riferimenti (1)
- [5] Einsteinium https://education.jlab.org/itselemental/ele099.html
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
Not Applicable
Riferimenti (1)
- [5] Einsteinium https://education.jlab.org/itselemental/ele099.html
Riferimenti
(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.
