← 周期表に戻る
Fm 100

Fermium (Fm)

actinide
周期: 7 ブロック: f

Solid

標準原子量

[257]

電子配置

[Rn] 5f12 7s2

融点

1526.85 °C

沸点

データなし

密度

9700 kg/m³

酸化数

+2, +3

電気陰性度(Pauling)

1.3

第1イオン化エネルギー

6.5 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 Enrico Fermi.
発見国 United States
発見者 Argonne, Los Alamos, U of Calif

Fermium is a synthetic actinide and the element with atomic number 100. It is produced only in minute amounts in high-neutron-flux reactions and is studied mainly by radiochemical and nuclear methods. Its chemistry is dominated by the +3 oxidation state, broadly resembling that of other late actinides and lanthanides. No macroscopic metallic sample has been prepared, and most measured properties are isotope- or solution-specific.

Fermium 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 (Fig. IUPAC.100.1). The element was named for Enrico Fermi, who built the first man-made nuclear reactor. 255Fm (with a half-life of 20 h) was the first fermium isotope identified. Fermium is the heaviest element that can be formed by neutron bombardment of lighter elements and is thus the heaviest element that can be synthesized in macroscopic quantities [632], [633].

Fermium is of interest in particle physics research, but it has no commercial applications. 253Fm was one of the decay products used to confirm synthesis of copernicium in a particle accelerator experiment [634].

Fermium is the heaviest synthetic element that can be formed by neutron bombardment of lighter elements, and hence the heaviest element that can be prepared in macroscopic quantities. The chemical properties of fermium have been studied solely using tracer amounts and innovative experimental techniques are required. Fermium metal has not been prepared, however measurements have been made on fermium alloys with rare earth metals and a number of predictions have been made. It was deduced that fermium metal prefers a divalent state but with modest compression can form a trivalent state. Other measurements on mixed fermium alloys and compounds include the magnetic moment, inner-shell binding energies, x-ray energies, sublimation enthalpy, etc.

The chemistry of fermium is typical of the late actinides, with a dominance of the +3 oxidation state but also a tendency toward an accessible +2 oxidation state. In the solid state no pure fermium compounds have been prepared, however Fm(III) has been studied by co-crystallization techniques as a trace component in a rare earth matrix with the same charge. Fermium co-precipitates with rare earth fluorides and hydroxides. In aqueous solution, fermium exists in solution as the Fm3+ ion, which has a hydration number of 16.9 and an acid dissociation constant of 1.6 × 10-4 (pKa = 3.8). Fm3+ forms complexes with a wide variety of organic ligands with hard donor atoms such as oxygen, and these complexes are usually more stable than those of the lighter actinides. It also forms complexes with ligands such as chloride or nitrate and, again, these complexes appear to be more stable than those formed by einsteinium or californium. Bonding in the heavier actinides is mostly ionic in character and the ionic radius of the Fm3+ ion is smaller than the preceding An3+ ions because of the actinide contraction. This is the result of a higher effective nuclear charge of fermium, and thus fermium forms shorter and stronger metal–ligand bonds. In the heavier actinides there is an increasing tendency to form a divalent ion that emerges at einsteinium. Fm3+ can be readily reduced to stable Fm2+ using moderately strong reducing agents such as samarium(II) chloride. In aqueous media, the Fm(III)/Fm(III) redox couple has been investigated via radio-electrochemistry and other techniques. The electrode potentials have been estimated to be similar to that of the ytterbium redox couple. The redox potentials for the various fermium couples have been measured and/or estimated by various workers: Fm3+ → Fm2+ (- 1.15 V); Fm2+ → Fm0 (-2.37 V), all versus the Normal Hydrogen Electrode.

Fermium 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, fermium-255, has a half-life of about 20 hours and was produced by combining 17 neutrons with uranium-238, which then underwent eight beta decays. Today, fermium 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. Fermium's most stable isotope, fermium-257, has a half-life of about 100.5 days. It decays into californium-253 through alpha decay or decays through spontaneous fission.

Fermium, element 100, is the eighth transuranium element of the actinide series and is named after the Italian physicist and Nobel Laureate Enrico Fermi. Element 100 was first discovered in 1952 in the fallout from the 10-megaton "Ivy Mike" nuclear test in the south Pacific the first successful test of a hydrogen fusion bomb. Researchers identified a new Pu-244 isotope found on filter papers on drone aircraft flown through the fallout. They determined that it could only have formed by the unexpected absorption of six neutrons by uranium-238 followed by successive beta-decays. At the time, the absorption of neutrons by a heavy nucleus was thought to be a rare process, but the identification of Pu-244 raised the possibility that still more neutrons could have been absorbed by the uranium nuclei leading to additional new elements.

Element 99, einsteinium was discovered almost immediately on other filter papers by Albert Ghiorso and co-workers at the Lawrence Berkeley Laboratory in collaboration with Argonne and Los Alamos National Laboratories, demonstrating that 15 neutrons were captured by U-238! The subsequent discovery of fermium required more material, as the yield of element 100 was expected to be at least an order of magnitude lower than that of einsteinium. So, contaminated coral from ground zero on Eniwetok atoll was shipped to Berkeley for processing and analysis. About two months after the Ivy-Mike test, a new activity was isolated emitting high-energy α-particles (7.1 MeV) with a half-life of about 1 day. It was the β- decay daughter of an isotope of einsteinium, and it had to be an isotope of element 100. : It was identified as 255Fm (half-life 20.07 hours). The discovery of the new elements, and the new data on neutron capture, was kept secret on the orders of the U.S. Military until 1955 due to Cold War tensions. Later the Berkeley team was able to prepare elements 99 and 100 in the lab by neutron bombardment of Pu-239 in a cyclotron. They published this work in 1954, with the disclaimer that these were not the first studies that had been carried out on the element. The 'Ivy Mike' studies were later declassified and published in 1955. Meanwhile, a group at the Nobel Institute for Physics in Stockholm independently claimed discovery of element 100 by producing an isotope with a 30-minute half-life and published their work in May 1954. Nevertheless, the historical precedence of the Berkeley team was generally recognized, and with it the prerogative to name the new element in honor of the recently deceased Enrico Fermi, the developer of the first artificial self-sustained nuclear reactor.

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
9700 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
1526.85 °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
0.339 eV
第1イオン化エネルギー
6.5 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
12.400043 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
23.20008 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
39.300135 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
55.000189 eV 全元素の第5イオン化エネルギーを比較 →
酸化数
+2, +3 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] 5f12 7s2

熱力学的性質

昇華熱
4.145722 eV
原子化熱
4.145722 eV

原子核

陽子数
100 全元素の陽子数を比較 →
中性子数
157 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)
257
最も安定な同位体
Fm-257
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, 30, 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
7440-72-4 全元素のCAS登録番号を比較 →
項記号
3H6
InChI
InChI=1S/Fm
InChI Key
MIORUQGGZCBUGO-UHFFFAOYSA-N

電子配置 測定値

イオンの電荷
陽子 100
電子 100
電荷 中性
電子配置 Fm: 5f¹² 7s²
電子配置
測定値
[Rn] 5f¹² 7s²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p⁶ 5f¹² 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
12/14 2↑
総電子数: 100 不対電子: 2 ?

原子モデル

陽子 100
中性子 143
電子 100
質量数 243
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
242 放射性242.07343 ± 0.00043データなし800 us
241 放射性241.07421 ± 0.00032データなし730 us
258 放射性258.09708 ± 0.00022データなし370 us
243 放射性243.07446 ± 0.00023データなし231 ms
256 放射性256.0917745 ± 0.0000078データなし157.1 分
測定値

相/状態

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

理由: 昇華点(1526.85 °C)より1501.8 °C低い

昇華点 1526.85 °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
1526.85 °C
現在の相 計算値
固体

相転移エネルギー

昇華熱 文献値
4.145722 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
9700 kg/m³

標準条件下

現在の密度 計算値
9700 kg/m³

標準条件下

原子スペクトル

全100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。

準位データの収録状況 ?

イオン電荷準位
Fm I 02
Fm II +12
Fm III +22
Fm IV +32
Fm V +42
Fm VI +52
Fm VII +62
Fm VIII +72
Fm IX +82
Fm X +92
NIST準位データの収録状況 →
100 Fm 257

Fermium — 原子軌道可視化ツール

[Rn] 5f12 7s2
エネルギー準位 2 8 18 32 30 8 2
酸化数 +2, +3
HOMO 5f n=5 · l=3 · m=-3
Fermium — 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
100 Fm 257

Fermium — 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110.5 pm

化合物

Fm
257.095 u
Fm
255.090 u
Fm
254.087 u
Fm
257.095 u
Fm
252.082 u
Fm
253.085 u

同位体 (5)

A total of 21 known isotopes of fermium exist with atomic weights from 242 to 260, including 2 that are metastable. Fermium-257 is the longest-lived with a half-life of 100.5 days. Other relatively long-lived isotopes include Fm-253 (3 days), Fm-252 (25.4 hours) and Fm-255 (~20 hours). Fm-250, with a half-life of 30 minutes, was shown to be a decay product of nobelium, element 102 and the chemical identification of the isotope 250Fm confirmed the production and discovery of element 102. All the remaining isotopes of fermium have half-lives ranging from 30 minutes to less than a millisecond. The neutron-capture product of fermium-257, 258Fm, undergoes spontaneous fission with a half-life of just 370 microseconds; 259Fm and 260Fm are also unstable with respect to spontaneous fission (t½ = 1.5 s and 4 ms respectively). This means that the neutron capture production chain essentially terminates at mass number 257 because of the very short spontaneous fission half-lives of the heavier isotopes.

質量数原子質量(u)天然存在比半減期崩壊形式
242 放射性242.07343 ± 0.00043データなし800 us
SF ≈100%α ?
241 放射性241.07421 ± 0.00032データなし730 us
SF =?α<14% β+<12%
258 放射性258.09708 ± 0.00022データなし370 us
SF ≈100%α ?
243 放射性243.07446 ± 0.00023データなし231 ms
α =91±0.3%SF =9±0.3%β+ ?
256 放射性256.0917745 ± 0.0000078データなし157.1 分
SF =91.9±0.3%α =8.1±0.3%
242 放射性
原子質量(u) 242.07343 ± 0.00043
天然存在比 データなし
半減期 800 us
崩壊形式
SF ≈100%α ?
241 放射性
原子質量(u) 241.07421 ± 0.00032
天然存在比 データなし
半減期 730 us
崩壊形式
SF =?α<14% +1
258 放射性
原子質量(u) 258.09708 ± 0.00022
天然存在比 データなし
半減期 370 us
崩壊形式
SF ≈100%α ?
243 放射性
原子質量(u) 243.07446 ± 0.00023
天然存在比 データなし
半減期 231 ms
崩壊形式
α =91±0.3%SF =9±0.3% +1
256 放射性
原子質量(u) 256.0917745 ± 0.0000078
天然存在比 データなし
半減期 157.1 分
崩壊形式
SF =91.9±0.3%α =8.1±0.3%

詳細な性質

共有結合半径(詳細)

共有結合半径(Pyykkö)
167 pm

ファンデルワールス半径

UFF
328.6 pm

番号付けの尺度

Mendeleev
36
Pettifor
37
Glawe
44

電気陰性度の尺度

Ghosh
0

分極率と分散

双極子分極率
113 a.u.
双極子分極率(不確かさ)
20 a.u.

相転移と同素体

融点1800.15 K

酸化数の分類

+2 extended
+3 main

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—124.5
同位体の崩壊形式 (46)
同位体モード強度
241SF—
241A14%
241B+12%
242SF100%
242A—
243A91%
243SF9%
243B+—
244SF97%
244B+2%

追加データ

Production

Production of this element (from raw materials or other compounds containing the element).

Because of the short half-life of all fermium isotopes, all that may have been present on the Earth during its formation has long since decayed away. Einsteinium and fermium did occur in the natural nuclear fission reactor at Oklo, but no longer exist. Fermium is produced as the result of multiple neutron captures in lighter elements, such as uranium and curium, followed by successive beta decays. The probability of such events increases with increased neutron flux, and nuclear explosions are the most powerful neutron sources on Earth. Fermium is also produced by the bombardment of lighter actinides with neutrons in nuclear reactors or accelerators. Fermium-257 is the heaviest isotope that is obtained via neutron capture, and can only be produced in nanogram quantities. The major source is the 85 MW High Flux Isotope Reactor (HFIR) at the Oak Ridge National Laboratory in Tennessee, USA. In a HFIR "campaign", tens of grams of curium are irradiated to produce heavier actinides and picogram quantities of fermium. The quantities of fermium produced in 20–200 kiloton thermonuclear explosions are believed to be of the order of milligrams, although it is mixed in with a huge quantity of debris. Forty picograms of 257Fm were recovered from 10 kilograms of debris from the 'Hutch' nuclear test in 1969. After production, fermium must be separated from debris and a host of other actinides and lanthanide fission products by solvent extraction, ion exchange, etc.). The annual reactor production of fermium-257 is in the picogram range. However, pure 255Fm (half-life 20 hours) can be easily isolated by "milking" the beta-decay daughter of pure 255Es (half-life 39.8 days).

参考文献 (1)

参考文献

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

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)
Fermium

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
Fermium

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
Fermium

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
Fermium

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
Fermium

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

9 PubChem Elements
Fermium

The element property data was retrieved from publications.

最終更新:

データ検証済み:

内容は最新の科学データと照合して確認されています。