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Pb 82

Lead (Pb)

post-transition-metal
周期: 6 族: 14 ブロック: p

Solid

標準原子量

207.2 u [206.14, 207.94]

電子配置

[Xe] 6s2 4f14 5d10 6p2

融点

327.46 °C

沸点

1748.85 °C

密度

1.1342e+4 kg/m³

酸化数

−4, −2, −1, 0, +1, +2, +3, +4

電気陰性度(Pauling)

2.33

第1イオン化エネルギー

7.41668 eV

発見年

2021

原子半径

180 pm

詳細

名称の由来 Anglo-Saxon: lead; symbol from Latin: plumbum.
発見者 Known to the ancients.

Lead is a dense, soft post-transition metal with atomic number 82. It is chemically characterized by the +2 oxidation state, with +4 less stable except in selected compounds, a pattern influenced by the inert-pair effect. Lead has been used since antiquity because it is easily smelted and worked, but its toxicity now strongly limits dispersive uses. It remains important where high density, corrosion resistance, low melting point, and radiation attenuation are valuable.

Lead is a bluish-white metal of bright luster. It is very soft, highly malleable, ductile, and a poor conductor of electricity. It is very resistant to corrosion; lead pipes bearing the insignia of Roman emperors, used as drains from the baths, are still in service. It is used in containers for corrosive liquids (such as sulfuric acid) and may be toughened by the addition of a small percentage of antimony or other metals.

The name derives from the Anglo-Saxon lead, which is of unknown origin. The element was known from prehistoric times. The chemical symbol Pb is derived from the Latin plumbum.

<!-- --> <p class="caption">For more information about the natural variations of the atomic weight of lead please read IUPAC Technical Report Variation of lead isotopic composition and atomic weight in terrestrial materials (IUPAC Technical Report) <img src="images/pdf.gif" style="width:auto; margin:0; vertical-align:bottom;"> by Z.-K. Zhu et al Pure Appl. Chem. <strong>93</strong>, 155-166 (2021).

Lead has been known since ancient times. It is sometimes found free in nature, but is usually obtained from the ores galena (PbS), anglesite (PbSO4), cerussite (PbCO3) and minum (Pb3O4). Although lead makes up only about 0.0013% of the earth's crust, it is not considered to be a rare element since it is easily mined and refined. Most lead is obtained by roasting galena in hot air, although nearly one third of the lead used in the United States is obtained through recycling efforts.

Long known, mentioned in Exodus. The alchemists believed lead to be the oldest metal and associated with the planet Saturn. Native lead occurs in nature, but is rare.

画像

性質

物理的性質

原子半径(経験値)
180 pm 全元素の原子半径(経験値)を比較 →
共有結合半径
146 pm 全元素の共有結合半径を比較 →
ファンデルワールス半径
202 pm 全元素のファンデルワールス半径を比較 →
金属半径
150 pm 全元素の金属半径を比較 →
密度
1.1342 × 104 kg/m³ 全元素の密度を比較 →
モル体積
0.0183 L/mol
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
327.46 °C 全元素の融点を比較 →
沸点
1748.85 °C 全元素の沸点を比較 →
熱伝導率
35.3 W/(m·K) 全元素の熱伝導率を比較 →
比熱容量
0.13 J/(g·K) 全元素の比熱容量を比較 →
モル熱容量
26.84 J/(mol·K) 全元素のモル熱容量を比較 →
結晶構造
面心立方構造 全元素の結晶構造を比較 →

化学的性質

電気陰性度(Pauling)
2.33 全元素の電気陰性度(Pauling)を比較 →
電気陰性度(Allen)
1.854
電子親和力
0.364 eV
第1イオン化エネルギー
7.41668 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
15.032551 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
31.93741 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
42.332706 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
68.800237 eV 全元素の第5イオン化エネルギーを比較 →
酸化数
−4, −2, −1, 0, +1, +2, +3, +4 全元素の酸化数を比較 →
価電子
4 全元素の価電子を比較 →
電子配置
[Xe] 6s2 4f14 5d10 6p2

熱力学的性質

融解熱
0.04943774 eV 全元素の融解熱を比較 →
蒸発熱
1.860393 eV 全元素の蒸発熱を比較 →
昇華熱
2.023112 eV
原子化熱
2.023112 eV
原子化エンタルピー
2.023112 eV

原子核

陽子数
82 全元素の陽子数を比較 →
中性子数
126 全元素の中性子数を比較 →
既知の同位体
43 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 →
最も安定な同位体
Pb-208
発見年
2021

存在度

存在度(地殻)
14 mg/kg 全元素の存在度(地殻)を比較 →
存在度(海洋)
3 × 10−5 mg/L 全元素の存在度(海洋)を比較 →

結晶構造

格子定数a
495 pm

電子構造

各電子殻の電子数
2, 8, 18, 32, 18, 4 全元素の各電子殻の電子数を比較 →

識別子

CAS登録番号
7439-92-1 全元素のCAS登録番号を比較 →
項記号
(1/2,1/2)0
InChI
InChI=1S/Pb
InChI Key
WABPQHHGFIMREM-UHFFFAOYSA-N

電子配置 測定値

イオンの電荷
陽子 82
電子 82
電荷 中性
電子配置 Pb: 4f¹⁴ 5d¹⁰ 6s² 6p²
電子配置
測定値
[Xe] 4f¹⁴ 5d¹⁰ 6s² 6p²
1s² 2s² 2p⁶ 3s² 3p⁶ 3d¹⁰ 4s² 4p⁶ 4d¹⁰ 5s² 5p⁶ 4f¹⁴ 5d¹⁰ 6s² 6p²
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
2/6 2↑
総電子数: 82 不対電子: 2 ?

原子モデル

陽子 82
中性子 102
電子 82
質量数 184
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

25 / 26 (26 強度データあり:26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
183 放射性182.991872 ± 0.00003データなし535 ms
184 放射性183.988136 ± 0.000014データなし490 ms
178 放射性178.003831 ± 0.000026データなし250 us
215 放射性215.00474 ± 0.00011データなし142 秒
204 放射性203.973044 ± 0.00000131.4000%140 Py
測定値

相/状態

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

理由: 融点(327.46 °C)より302.5 °C低い

融点 327.46 °C
沸点 1748.85 °C
融点との差(下) 302.5 °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
液体
気体
融解
沸騰
25°C
固体
液体
気体
現在

相転移点

融点 文献値
327.46 °C
沸点 文献値
1748.85 °C
現在の相 計算値
固体

相転移エネルギー

融解熱 文献値
0.04943774 eV

融点で1 molを融解させるのに必要なエネルギー

蒸発熱 文献値
1.860393 eV

沸点で1 molを蒸発させるのに必要なエネルギー

昇華熱 文献値
2.023112 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
1.1342e+4 kg/m³

標準条件下

現在の密度 計算値
1.1342e+4 kg/m³

標準条件下

原子スペクトル

全82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
Pb I 013528135
Pb II +197312
Pb III +24100
Pb IV +39200
Pb V +49000
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
Pb I 0136
Pb II +195
Pb III +2124
Pb IV +3108
Pb V +445
Pb VI +52
Pb VII +62
Pb VIII +72
Pb IX +82
Pb X +92
NIST準位データの収録状況 →
82 Pb 207.2

Lead — 原子軌道可視化ツール

[Xe]6s24f145d106p2
エネルギー準位 2 8 18 32 18 4
酸化数 -4, -2, -1, 0, +1, +2, +3, +4
HOMO 6p n=6 · l=1 · m=-1
Lead — 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
82 Pb 207.2

Lead — 結晶構造可視化ツール

Face-Centered Cubic · ピアソン記号 cF4
実験値
ピアソン記号 cF4
配位数 12
充填率 74.000%
Lead — 結晶構造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

イオン半径

全12件中10件を表示しています。

電荷配位スピン半径
+24データなし98 pm
+26データなし119 pm
+27データなし123 pm
+28データなし129 pm
+29データなし135 pm
+210データなし140 pm
+211データなし145 pm
+212データなし149 pm
+44データなし65 pm
+45データなし73 pm

化合物

Pb
207.000 u
Pb+2
207.000 u
Pb
209.984 u
Pb
214.000 u
Pb
211.992 u
Pb
205.974 u
Pb
206.976 u
Pb
207.977 u
Pb
203.973 u
Pb
202.973 u
Pb
204.974 u
Pb
208.981 u
Pb
210.989 u
Pb
200.973 u
Pb
199.972 u
Pb
197.972 u
Pb
198.973 u
Pb
201.972 u
Pb
194.975 u
Pb
218.017 u
Pb+2
211.992 u
Pb
193.974 u
Pb
195.973 u
Pb
196.973 u
Pb
212.997 u

同位体 (5)

質量数原子質量(u)天然存在比半減期崩壊形式
183 放射性182.991872 ± 0.00003データなし535 ms
α ≈100%β+ ?
184 放射性183.988136 ± 0.000014データなし490 ms
α =80±1.1%β+ ?
178 放射性178.003831 ± 0.000026データなし250 us
α ≈100%β+ ?
215 放射性215.00474 ± 0.00011データなし142 秒
β- =100%
204 放射性203.973044 ± 0.00000131.4000% ± 0.1000%140 Py
IS =1.4±0.6%α ?
183 放射性
原子質量(u) 182.991872 ± 0.00003
天然存在比 データなし
半減期 535 ms
崩壊形式
α ≈100%β+ ?
184 放射性
原子質量(u) 183.988136 ± 0.000014
天然存在比 データなし
半減期 490 ms
崩壊形式
α =80±1.1%β+ ?
178 放射性
原子質量(u) 178.003831 ± 0.000026
天然存在比 データなし
半減期 250 us
崩壊形式
α ≈100%β+ ?
215 放射性
原子質量(u) 215.00474 ± 0.00011
天然存在比 データなし
半減期 142 秒
崩壊形式
β- =100%
204 放射性
原子質量(u) 203.973044 ± 0.0000013
天然存在比 1.4000% ± 0.1000%
半減期 140 Py
崩壊形式
IS =1.4±0.6%α ?

スペクトル線

波長(nm)強度電離段階種類遷移精度出典
401.96322 nm15000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.(2P*<1/2>).6d 2[5/2]*測定値NIST
405.780659 nm95000Pb Iemission6s2.6p2 (3/2,1/2) → 6s2.6p.7s (1/2,1/2)*測定値NIST
406.213593 nm14000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.(2P*<1/2>).6d 2[3/2]*測定値NIST
415.78144 nm10Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.9s (1/2,1/2)*測定値NIST
416.80327 nm10000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.(2P*<1/2>).6d 2[5/2]*測定値NIST
434.041263 nm200Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.(2P*<1/2>).7d 2[3/2]*測定値NIST
500.54165 nm1000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.7s (3/2,1/2)*測定値NIST
500.65724 nm100Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,3/2)測定値NIST
507.6322 nm10Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,1/2)測定値NIST
508.94835 nm50Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,3/2)測定値NIST
509.00083 nm20Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,3/2)測定値NIST
510.72427 nm10Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.9p (1/2,1/2)測定値NIST
520.14372 nm2000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.8s (1/2,1/2)*測定値NIST
569.23465 nm40Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.(2P*<1/2>).5f 2[5/2]測定値NIST
589.56245 nm200Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,3/2)測定値NIST
600.18624 nm2000Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,3/2)測定値NIST
601.16667 nm500Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,3/2)測定値NIST
605.93556 nm500Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,1/2)測定値NIST
611.05203 nm50Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,1/2)測定値NIST
623.52656 nm100Pb Iemission6s2.6p.7s (1/2,1/2)* → 6s2.6p.8p (1/2,1/2)測定値NIST
689.2117 nm10Pb Iemission6s2.6p.7p (1/2,1/2) → 6s2.6p.(2P*<1/2>).10d 2[5/2]*測定値NIST
712.893 nm5Pb Iemission6s2.6p.7p (1/2,1/2) → 6s2.6p.11s (1/2,1/2)*測定値NIST
722.89658 nm20000Pb Iemission6s2.6p2 (3/2,3/2) → 6s2.6p.7s (1/2,1/2)*測定値NIST
730.46753 nm5Pb Iemission6s2.6p.7p (1/2,1/2) → 6s2.6p.(2P*<1/2>).9d 2[3/2]*測定値NIST
733.0146 nm8Pb Iemission6s2.6p2 (3/2,1/2) → 6s2.6p2 (3/2,3/2)測定値NIST
734.6676 nm10Pb Iemission6s2.6p.7p (1/2,1/2) → 6s2.6p.(2P*<1/2>).9d 2[5/2]*測定値NIST

詳細な性質

共有結合半径(詳細)

共有結合半径(Pyykkö)
144 pm
共有結合半径(Pyykkö、二重結合)
135 pm
共有結合半径(Pyykkö、三重結合)
137 pm

ファンデルワールス半径

Bondi
202 pm
Batsanov
230 pm
Alvarez
260 pm
UFF
429.7 pm
MM3
274 pm

原子半径と金属半径

原子半径(Rahm)
249 pm
金属半径(C12)
170 pm

番号付けの尺度

Mendeleev
91
Pettifor
82
Glawe
82

電気陰性度の尺度

Ghosh
0
Miedema
4
Gunnarsson–Lundqvist
4
Robles–Bartolotti
4

分極率と分散

双極子分極率
47 a.u.
双極子分極率(不確かさ)
3 a.u.
C₆ (Gould–Bučko)
534 Ha·Bohr6

ミーデマパラメータ

ミーデマモル体積
18.28 cm3/mol
ミーデマ電子密度
2

供給リスクと経済性

生産集中度
44
相対供給リスク
6
埋蔵量の分布
34
政治的安定性(最大生産国)
24
政治的安定性(最大埋蔵国)
75

相転移と同素体

融点600.61 K
沸点2022.15 K

酸化数の分類

+4 main
+2 main
0 extended
−2 extended
+1 extended
−1 extended
−4 extended
+3 extended

専門参考データ

遮蔽定数 (15)
n軌道σ
1s1.5805
2p4.5234
2s21.57
3d13.4533
3p22.8505
3s23.8477
4d37.6804
4f38.0312
4p35.9664
4s35.1072
結晶半径の詳細 (12)
電荷CNスピンrcrystal (pm)由来
2IVPY112calculated,
2VI133
2VII137calculated,
2VIII143calculated,
2IX149calculated,
2X154calculated,
2XI159calculated,
2XII163
4IV79estimated,
4V87estimated,
同位体の崩壊形式 (59)
同位体モード強度
178A100%
178B+—
179A100%
180A100%
181A100%
181B+—
182A100%
182B+—
183A100%
183B+—
X線散乱因子 (516)
エネルギー (eV)f₁f₂
10—4.6699
10.1617—4.72735
10.3261—4.78551
10.4931—4.84439
10.6628—4.83957
10.8353—4.83203
11.0106—4.82451
11.1886—4.817
11.3696—4.7889
11.5535—4.7596

追加データ

Sources

Sources of this element.

Lead is obtained chiefly from galena (PbS) by a roasting process. Anglesite, cerussite, and minim are other common lead minerals.

参考文献 (1)

Isotopes in Forensic Science and Anthropology

Information on the use of this element's isotopes in forensic science and anthropology.

Different geographic regions may have characteristic terrestrial lead isotopic compositions because of variations in the ages and chemical composition of the rocks and minerals in the local environment. Therefore, lead produced at a particular location can have a unique lead isotopic composition and it is possible to trace the history and origins of pollutants by measuring the relative amounts of the four stable isotopes of lead (208Pb, 207Pb, 206Pb, and 204Pb) (Fig. IUPAC.82.2) [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000)., [548] T. J. Chow, J. L. Earl. Science169, 577 (1970).. Using isotopic abundance data, the source of this toxic metal can be identified as it moves through air and water and eventually to living systems [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000)., [549] M. K. Reuer, D. J. Weiss. Math. Phys. Eng. Sci.360, 2889 (2002).. Scientists have analyzed lead in air pollution in California and found that it originated from Asia. Airborne particles from China have relatively higher amounts of 208Pb, which distinguishes the lead isotopic signature between airborne particles from Asia and North America. This knowledge could have implications in understanding the mixing of particles in the atmosphere and how pollutants are transported over vast distances [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000)., [549] M. K. Reuer, D. J. Weiss. Math. Phys. Eng. Sci.360, 2889 (2002)., [550] S. A. Ewing, J. N. Christensen, S. T. Brown, R. A. Vancuren, S. S. Cliff, D. J. Depaolo. Environ. Sci. Technol.44, 8911 (2010)., [551] D. Krotz. Lead Isotopes Yield Clues to How Asian Air Pollution Reaches California, Lawrence Berkeley National Laboratory News Center (2014), Feb. 25; http://newscenter.lbl.gov/feature-stories/2010/12/01/lead-isotopes-air-pollution/.. Mapping the distribution of lead pollution by studying 204Pb, 206Pb, 207Pb and 208Pb also allows the identification of those human activities that contribute the highest amounts of lead to the environment [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000)., [549] M. K. Reuer, D. J. Weiss. Math. Phys. Eng. Sci.360, 2889 (2002)., [552] D. Cicchella, B. De Vivo, A. Lima, S. Albanese, R. A. R. McGill, R. R. Parrish. Geochem. Explor. Environ. Anal.8, 103 (2008)..

The measurement of the isotopic composition of lead in blood can help to determine the source of this toxic element in the body [553] R. H. Gwiazda, D. R. Smith. Environ. Health Perspect.108, 1091 (2000).. Lead is stored in bones and teeth. If a person moves to a different geographical region, the isotopic composition of the lead in the teeth is maintained, recording their place of origin. Bone can store lead for long periods of time (about 20 years), and some skeletal lead may be older and have a different isotopic composition than other skeletal lead. These differences reflect exposure to lead of different origins. By studying the isotope-amount ratio n(206Pb)/n(204Pb) and n(207Pb)/n(206Pb) in bone and teeth, it is possible to determine someone’s place of origin. For example, isotopes of lead were analyzed in the teeth and bones of a human mummy, known as the “Iceman”, to help determine his place of origin [554] B. L. Gulson, B. R. Gillings. Environ. Health Perspect.105, 820 (1997)., [555] W. Müller, H. Fricke, A. N. Halliday, M. T. McCulloch, J. A. Wartho. Science302, 862 (2003)..

210Pb is a relatively short-lived radioactive isotope of lead that is constantly produced by the decay of 222Rn in the atmosphere. While living, humans naturally incorporate 210Pb from the environment into bones and tissues. The amount of 210Pb in the body reaches equilibrium such that the 210Pb ingested is in equilibrium with the 210Pb that decays. When a person dies, this incorporation of 210Pb ceases and the relative amount of this isotope in the body decreases. Therefore, measurement of the 210Pb activity in a corpse can help determine time of death [556] D. R. Smith, J. D. Osterloh, A. R. Flegal. Environ. Health Perspect.104, 60 (1996)., [557] P. Rincon. “Isotopes could improve forensics”, in BBC News Online..

Lead isotope-amount ratios n(206Pb)/n(204Pb), n(207Pb)/n(204Pb), and n(208Pb)/n(204Pb)) along with isotope-amount ratio of silver, n(107Ag)/n(109Ag), and isotope-amount ratio of copper n(65Cu)/n(63Cu) have been used to determine the origin of European coins and to investigate the flow of goods in the world market over time [237] A. M. Desaulty, P. Telouk, E. Albalat, F. Albarede. Proc. Natl. Acad. Sci.108, 9002 (2011).. Metals from Peru and Mexico and those from European mining have distinct isotopic signatures that enable the origin of the metal to be determined by examining the isotopic compositions of silver, copper, and lead in the coins. Abundant silver sources mined in Mexico and Peru in the 16 th century were used to mint coins, but were not a major influence in the European coin market until the 18 th century [237] A. M. Desaulty, P. Telouk, E. Albalat, F. Albarede. Proc. Natl. Acad. Sci.108, 9002 (2011)..

参考文献 (13)
  • [237] A. M. Desaulty, P. Telouk, E. Albalat, F. Albarede. Proc. Natl. Acad. Sci.108, 9002 (2011).
  • [547] I. Renberg, M. L. Brännvall, R. Bindler, O. Emteryd. Ambio29, 150 (2000).
  • [548] T. J. Chow, J. L. Earl. Science169, 577 (1970).
  • [549] M. K. Reuer, D. J. Weiss. Math. Phys. Eng. Sci.360, 2889 (2002).
  • [550] S. A. Ewing, J. N. Christensen, S. T. Brown, R. A. Vancuren, S. S. Cliff, D. J. Depaolo. Environ. Sci. Technol.44, 8911 (2010).
  • [551] D. Krotz. Lead Isotopes Yield Clues to How Asian Air Pollution Reaches California, Lawrence Berkeley National Laboratory News Center (2014), Feb. 25; http://newscenter.lbl.gov/feature-stories/2010/12/01/lead-isotopes-air-pollution/.
  • [552] D. Cicchella, B. De Vivo, A. Lima, S. Albanese, R. A. R. McGill, R. R. Parrish. Geochem. Explor. Environ. Anal.8, 103 (2008).
  • [553] R. H. Gwiazda, D. R. Smith. Environ. Health Perspect.108, 1091 (2000).
  • [554] B. L. Gulson, B. R. Gillings. Environ. Health Perspect.105, 820 (1997).
  • [555] W. Müller, H. Fricke, A. N. Halliday, M. T. McCulloch, J. A. Wartho. Science302, 862 (2003).
  • [556] D. R. Smith, J. D. Osterloh, A. R. Flegal. Environ. Health Perspect.104, 60 (1996).
  • [557] P. Rincon. “Isotopes could improve forensics”, in BBC News Online.
  • [4] IUPAC Periodic Table of the Elements and Isotopes (IPTEI) https://doi.org/10.1515/pac-2015-0703

参考文献

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

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)
Lead

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
Lead

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
Lead

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
Lead

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
Lead

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

9 PubChem Elements
Lead

The element property data was retrieved from publications.

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