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Es 99

Einsteinium (Es)

actinide
周期: 7 ブロック: f

Solid

標準原子量

[252]

電子配置

[Rn] 7s2 5f11

融点

859.85 °C

沸点

データなし

密度

8840 kg/m³

酸化数

+2, +3, +4

電気陰性度(Pauling)

1.3

第1イオン化エネルギー

6.3684 eV

発見年

1952

原子半径

データなし

詳細

名称の由来 Named in honor of the scientist Albert Einstein.
発見国 United States
発見者 Argonne, Los Alamos, U of Calif

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.

画像

性質

物理的性質

ファンデルワールス半径
245 pm 全元素のファンデルワールス半径を比較 →
密度
8840 kg/m³ 全元素の密度を比較 →
標準温度・圧力(STP)での相
固体 全元素の標準温度・圧力(STP)での相を比較 →
融点
859.85 °C 全元素の融点を比較 →

化学的性質

電気陰性度(Pauling)
1.3 全元素の電気陰性度(Pauling)を比較 →
電子親和力
-0.3 eV (負の値—この原子は電子を取り込まないと予測される)
第1イオン化エネルギー
6.3684 eV 全元素の第1イオン化エネルギーを比較 →
第2イオン化エネルギー
12.200042 eV 全元素の第2イオン化エネルギーを比較 →
第3イオン化エネルギー
22.700078 eV 全元素の第3イオン化エネルギーを比較 →
第4イオン化エネルギー
38.800134 eV 全元素の第4イオン化エネルギーを比較 →
第5イオン化エネルギー
54.100186 eV 全元素の第5イオン化エネルギーを比較 →
酸化数
+2, +3, +4 全元素の酸化数を比較 →
価電子
3 全元素の価電子を比較 →
電子配置
[Rn] 7s2 5f11

熱力学的性質

昇華熱
3.990258 eV
原子化熱
3.990258 eV
原子化エンタルピー
1.378453 eV

原子核

陽子数
99 全元素の陽子数を比較 →
中性子数
153 全元素の中性子数を比較 →
既知の同位体
20 全元素の既知の同位体を比較 →
安定同位体
0 全元素の安定同位体を比較 →
質量数(最も安定な同位体)
252
最も安定な同位体
Es-252
発見年
1952

存在度

データなし

結晶構造

データなし

電子構造

各電子殻の電子数
2, 8, 18, 32, 29, 8, 2 全元素の各電子殻の電子数を比較 →

識別子

CAS登録番号
7429-92-7 全元素のCAS登録番号を比較 →
項記号
4I°15/2
InChI
InChI=1S/Es
InChI Key
CKBRQZNRCSJHFT-UHFFFAOYSA-N

電子配置 測定値

イオンの電荷
陽子 99
電子 99
電荷 中性
電子配置 Es: 5f¹¹ 7s²
電子配置
測定値
[Rn] 5f¹¹ 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹¹ 7s²
軌道図
1s
2/2
2s
2/2
2p
6/6
3s
2/2
3p
6/6
4s
2/2
3d
10/10
4p
6/6
5s
2/2
4d
10/10
5p
6/6
6s
2/2
4f
14/14
5d
10/10
6p
6/6
7s
2/2
5f
11/14 3↑
総電子数: 99 不対電子: 3 ?

原子モデル

陽子 99
中性子 153
電子 99
質量数 252
安定性 放射性

同位体によって中性子数、質量、安定性は変わりますが、中性原子の電子配置は変わりません。

模式的な原子モデルです。実際の縮尺とは異なります。

原子の指紋

発光/吸収スペクトル

0 / 0 (0 強度データあり:0本)
測定値
発光 可視光:380–750 nm

同位体分布

安定同位体はありません。

質量数原子質量(u)天然存在比半減期
252 放射性252.08298 ± 0.000054データなし471.7 日
254 放射性254.0880222 ± 0.0000045データなし275.7 日
249 放射性249.076411 ± 0.000032データなし102.2 分
255 放射性255.090275 ± 0.000012データなし39.8 日
244 放射性244.07088 ± 0.0002データなし37 秒
測定値

相/状態

1 atm / 101.325 kPa
固体 25 °C (298.15 K)

理由: 昇華点(859.85 °C)より834.9 °C低い

昇華点 859.85 °C
0 K 現在の温度: 25 °C 6000 K
相変化図

模式図、実際の縮尺とは異なります

固体
気体
昇華
25°C
固体
液体
気体
現在

相転移点

昇華点 文献値
859.85 °C
現在の相 計算値
固体

相転移エネルギー

昇華熱 文献値
3.990258 eV

昇華点で1 molを昇華させるのに必要なエネルギー

密度

基準密度 文献値
8840 kg/m³

標準条件下

現在の密度 計算値
8840 kg/m³

標準条件下

原子スペクトル

全99件中10件を表示しています。 イオンの電荷の昇順で並べています。

スペクトル線データの収録状況 ?

イオン電荷スペクトル線の総数遷移確率準位の表記
Es I 01100
Es II +11200
NISTスペクトル線データの収録状況 →

準位データの収録状況 ?

イオン電荷準位
Es I 02
Es II +12
Es III +22
Es IV +32
Es V +42
Es VI +52
Es VII +62
Es VIII +72
Es IX +82
Es X +92
NIST準位データの収録状況 →
99 Es 252

Einsteinium — 原子軌道可視化ツール

[Rn]7s25f11
エネルギー準位 2 8 18 32 29 8 2
酸化数 +2, +3, +4
HOMO 5f n=5 · l=3 · m=-3
Einsteinium — 原子軌道可視化ツールのプレビュー
Three.jsは必要な場合にのみ読み込まれます
99 Es 252

Einsteinium — 結晶構造可視化ツール

結晶構造のデータはありません

イオン半径

電荷配位スピン半径
+39データなし111.6 pm

化合物

Es
252.083 u
Es
254.088 u
Es
253.085 u
Es
250.079 u
Es
251.080 u

同位体 (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.

質量数原子質量(u)天然存在比半減期崩壊形式
252 放射性252.08298 ± 0.000054データなし471.7 日
α =78±0.2%ε =22±0.2%
254 放射性254.0880222 ± 0.0000045データなし275.7 日
α ≈100%ε ?β- =1.74e-4±0.8%
249 放射性249.076411 ± 0.000032データなし102.2 分
β+ ≈100%α =0.57±0.8%
255 放射性255.090275 ± 0.000012データなし39.8 日
β- =92.0±0.4%α =8.0±0.4%SF =0.0041±0.2%
244 放射性244.07088 ± 0.0002データなし37 秒
β+ =95±0.3%α =5±0.3%β+SF =0.011±0.4%
252 放射性
原子質量(u) 252.08298 ± 0.000054
天然存在比 データなし
半減期 471.7 日
崩壊形式
α =78±0.2%ε =22±0.2%
254 放射性
原子質量(u) 254.0880222 ± 0.0000045
天然存在比 データなし
半減期 275.7 日
崩壊形式
α ≈100%ε ? +2
249 放射性
原子質量(u) 249.076411 ± 0.000032
天然存在比 データなし
半減期 102.2 分
崩壊形式
β+ ≈100%α =0.57±0.8%
255 放射性
原子質量(u) 255.090275 ± 0.000012
天然存在比 データなし
半減期 39.8 日
崩壊形式
β- =92.0±0.4%α =8.0±0.4% +1
244 放射性
原子質量(u) 244.07088 ± 0.0002
天然存在比 データなし
半減期 37 秒
崩壊形式
β+ =95±0.3%α =5±0.3% +1

詳細な性質

共有結合半径(詳細)

共有結合半径(Pyykkö)
165 pm
共有結合半径(Pyykkö、二重結合)
140 pm

ファンデルワールス半径

Alvarez
270 pm
UFF
329.9 pm

番号付けの尺度

Mendeleev
34
Pettifor
38
Glawe
43

電気陰性度の尺度

Ghosh
0

分極率と分散

双極子分極率
118 a.u.
双極子分極率(不確かさ)
20 a.u.

相転移と同素体

融点1133.15 K

酸化数の分類

+3 main
+4 extended
+2 extended

専門参考データ

結晶半径の詳細 (1)
電荷CNスピンrcrystal (pm)由来
3IX—125.6
同位体の崩壊形式 (51)
同位体モード強度
239A—
239B+—
239SF—
240A70%
240B+30%
240B+SF0.2%
241A100%
241B+—
242A57%
242B+43%

追加データ

参考文献

(9)
2 Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
Es

The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.

3 IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)
Einsteinium

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.

4 IUPAC Periodic Table of the Elements and Isotopes (IPTEI)

The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.

ライセンスに関する注記: Copyright (c) 2020 International Union of Pure and Applied Chemistry. The International Union of Pure and Applied Chemistry (IUPAC) contribution within Pubchem is provided under a CC-BY-NC-ND 4.0 license, unless otherwise stated.
5 Jefferson Lab, U.S. Department of Energy
Einsteinium

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/

ライセンスに関する注記: Please see citation and linking information: https://education.jlab.org/faq/index.html
6 Los Alamos National Laboratory, U.S. Department of Energy
Einsteinium

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.

7 NIST Physical Measurement Laboratory
Einsteinium

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

8 PubChem Elements
Einsteinium

This section provides all form of data related to element Einsteinium.

9 PubChem Elements
Einsteinium

The element property data was retrieved from publications.

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