← 周期表に戻る
C 6

Carbon (C)

nonmetal
周期: 2 族: 14 ブロック: p

Solid

標準原子量

12.011 u [12.0096, 12.0116]

電子配置

[He] 2s2 2p2

融点

3549.85 °C

沸点

3824.85 °C

密度

2267 kg/m³

酸化数

−4, −3, −2, −1, 0, +1, +2, +3, +4

電気陰性度(Pauling)

2.55

第1イオン化エネルギー

11.260288 eV

発見年

1797

原子半径

70 pm

詳細

名称の由来 Latin: carbo, (charcoal).
発見者 Known to the ancients

Carbon is a nonmetal in group 14 and the defining element of organic chemistry. Its small atoms form strong covalent bonds with carbon and many other elements, allowing chains, rings, networks, and multiple bonds of great diversity. It occurs naturally as graphite, diamond, amorphous carbon-rich materials, carbonate minerals, fossil carbon, dissolved carbon species, and as a central element in living matter.

Carbon is a member of group 14 of the periodic table. It has three allotropic forms of it, diamonds, graphite and fullerite. Carbon-14 is commonly used in radioactive dating. Carbon occurs in all organic life and is the basis of organic chemistry. Carbon has the interesting chemical property of being able to bond with itself, and a wide variety of other elements.

The name derives from the Latin carbo for "charcoal". It was known in prehistoric times in the form of charcoal and soot. In 1797, the English chemist Smithson Tennant proved that diamond is pure carbon.

Carbon, the sixth most abundant element in the universe, has been known since ancient times. Carbon is most commonly obtained from coal deposits, although it usually must be processed into a form suitable for commercial use. Three naturally occurring allotropes of carbon are known to exist: amorphous, graphite and diamond.

From the Latin word carbo: charcoal. Carbon, an element of prehistoric discovery, is very widely distributed in nature. It is found in abundance in the sun, stars, comets, and atmospheres of most planets. Carbon in the form of microscopic diamonds is found in some meteorites.

Natural diamonds are found in kimberlite of ancient volcanic "pipes," found in South Africa, Arkansas, and elsewhere. Diamonds are now also being recovered from the ocean floor off the Cape of Good Hope. About 30% of all industrial diamonds used in the U.S. are now made synthetically.

The energy of the sun and stars can be attributed at least in part to the well-known carbon-nitrogen cycle.

画像

性質

物理的性質

原子半径(経験値)
70 pm 全元素の原子半径(経験値)を比較 →
共有結合半径
76 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
170 pm 全元素のファンデルワールス半径を比較 →
密度
2267 kg/m³ 全元素の密度を比較 →
モル体積
0.0053 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
3549.85 °C 全元素の融点を比較 →
沸点
3824.85 °C 全元素の沸点を比較 →
熱伝導率
1.59 W/(m·K) 全元素の熱伝導率を比較 →
比熱容量
0.709 J/(g·K) 全元素の比熱容量を比較 →
モル熱容量
8.517 J/(mol·K) 全元素のモル熱容量を比較 →
結晶構造
ダイヤモンド立方構造 全元素の結晶構造を比較 →

化学的性質

電気陰性度(Pauling)
2.55 全元素の電気陰性度(Pauling)を比較 →
電気陰性度(Allen)
2.544
電子親和力
1.2621 eV
第1イオン化エネルギー
11.260288 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
24.383227 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
47.887945 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
64.493742 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
392.09191 eV 全元素の第5イオン化エネルギーを比較 →
酸化数
−4, −3, −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 →
同素体
["graphite"]
電子配置
[He] 2s2 2p2

熱力学的性質

三重点(温度)
4489 °C
三重点(圧力)
1.03e+7 Pa
蒸発熱
7.410478 eV 全元素の蒸発熱を比較 →
昇華熱
7.42789 eV
原子化熱
7.42789 eV
原子化エンタルピー
7.42986 eV

原子核

陽子数
6 全元素の陽子数を比較 →
中性子数
6 全元素の中性子数を比較 →
既知の同位体
16 全元素の既知の同位体を比較 →
安定同位体
2 全元素の安定同位体を比較 →
最も安定な同位体
C-12
発見年
1797

存在度

存在度(地殻)
200 mg/kg 全元素の存在度(地殻)を比較 →
存在度(海洋)
28 mg/L 全元素の存在度(海洋)を比較 →

結晶構造

格子定数a
357 pm

電子構造

各電子殻の電子数
2, 4 全元素の各電子殻の電子数を比較 →

識別子

CAS登録番号
7440-44-0 全元素のCAS登録番号を比較 →
項記号
3P0
InChI
InChI=1S/C
InChI Key
OKTJSMMVPCPJKN-UHFFFAOYSA-N

電子配置 測定値

イオンの電荷
陽子 6
電子 6
電荷 中性
電子配置 C: 2s² 2p²
電子配置
測定値
[He] 2s² 2p²
1s² 2s² 2p²
軌道図
1s
2/2
2s
2/2
2p
2/6 2↑
総電子数: 6 不対電子: 2 ?

原子モデル

陽子 6
中性子 6
電子 6
質量数 12
安定性 安定

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 / 50 (50 強度データあり:50本)
測定値
発光 可視光:380–750 nm

同位体分布

1298.9300%131.0700%質量数天然存在比(%)
質量数原子質量(u)天然存在比半減期
12 安定1298.9300%安定
13 安定13.00335483507 ± 0.000000000231.0700%安定
測定値

相/状態

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

理由: 昇華点(3824.85 °C)より3799.8 °C低い

昇華点 3824.85 °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
3824.85 °C
現在の相 計算値
固体

相転移エネルギー

蒸発熱 文献値
7.410478 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
7.42789 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
2267 kg/m³

標準条件下

現在の密度 計算値
2267 kg/m³

標準条件下

詳細

三重点 文献値
4489 °C

原子スペクトル

全11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
C I 0210216162102
12C I 同位体089089
13C I 同位体089089
12C II 同位体+11870187
14C II 同位体+11870187
C II +1160514331605
13C II 同位体+11870187
C III +2882878878
C IV +3259224255
C V +4149146147
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
C I 0435
12C I 同位体033
13C I 同位体033
12C II 同位体+136
14C II 同位体+136
C II +1415
13C II 同位体+136
C III +2201
C IV +3107
C V +4156
NIST準位データの収録状況 →
6 C 12.0106

Carbon — 原子軌道可視化ツール

[He]2s22p2
エネルギー準位 2 4
酸化数 -4, -3, -2, -1, 0, +1, +2, +3, +4
HOMO 2p n=2 · l=1 · m=-1
Carbon — 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
6 C 12.0106

Carbon — 結晶構造可視化ツール

Face-Centered Cubic · ピアソン記号 cF8
実験値
ピアソン記号 cF8
配位数 4
充填率 34.000%
Carbon — 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

電荷配位スピン半径
+44データなし15 pm
+46データなし16 pm

化合物

C
12.011 u

同位体 (2)

Carbon has seven isotopes. In 1961 the International Union of Pure and Applied Chemistry adopted the isotope carbon-12 as the basis for atomic weights. Carbon-14, an isotope with a half-life of 5715 years, has been widely used to date such materials as wood, archaeological specimens, etc.

質量数原子質量(u)天然存在比半減期崩壊形式
12 安定1298.9300% ± 0.0800%安定
stable
13 安定13.00335483507 ± 0.000000000231.0700% ± 0.0800%安定
stable
12 安定
原子質量(u) 12
天然存在比 98.9300% ± 0.0800%
半減期 安定
崩壊形式
stable
13 安定
原子質量(u) 13.00335483507 ± 0.00000000023
天然存在比 1.0700% ± 0.0800%
半減期 安定
崩壊形式
stable

スペクトル線

全993件中50件を表示しています。 初期設定では、強度の測定値があるスペクトル線のみを表示します。

波長(nm)強度電離段階種類遷移精度出典
505.214927 nm160000C Iemission2s2.2p.3s 1P* → 2s2.2p.4p 1D測定値NIST
538.033014 nm120000C Iemission2s2.2p.3s 1P* → 2s2.2p.4p 1P測定値NIST
711.31656 nm110000C Iemission2s2.2p.3p 3D → 2s2.2p.4d 3F*測定値NIST
493.202524 nm73000C Iemission2s2.2p.3s 1P* → 2s2.2p.4p 1S測定値NIST
477.173374 nm69000C Iemission2s2.2p.3s 3P* → 2s2.2p.4p 3P測定値NIST
711.697758 nm45000C Iemission2s2.2p.3p 3D → 2s2.2p.5s 3P*測定値NIST
658.76211 nm40000C Iemission2s2.2p.3p 1P → 2s2.2p.4d 1P*測定値NIST
579.311495 nm38000C Iemission2s.2p3 3D* → 2s2.2p.4p 3P測定値NIST
711.96559 nm37000C Iemission2s2.2p.3p 3D → 2s2.2p.5s 3P*測定値NIST
580.059993 nm35000C Iemission2s.2p3 3D* → 2s2.2p.4p 3P測定値NIST
600.1123 nm35000C Iemission2s2.2p.3p 3D → 2s2.2p.6s 3P*測定値NIST
477.589266 nm34000C Iemission2s2.2p.3s 3P* → 2s2.2p.4p 3P測定値NIST
437.13814 nm33000C Iemission2s2.2p.3s 1P* → 2s2.2p.5p 1P測定値NIST
711.145795 nm32000C Iemission2s2.2p.3p 3D → 2s2.2p.4d 3F*測定値NIST
682.814076 nm27000C Iemission2s2.2p.3p 1P → 2s2.2p.4d 1D*測定値NIST
504.149039 nm25000C Iemission2s.2p3 3D* → 2s2.2p.(2P*<1/2>).4f 2[5/2]測定値NIST
477.002376 nm24000C Iemission2s2.2p.3s 3P* → 2s2.2p.4p 3P測定値NIST
600.6012 nm23000C Iemission2s2.2p.3p 3D → 2s2.2p.5d 3D*測定値NIST
665.55294 nm20000C Iemission2s2.2p.3p 1P → 2s2.2p.5s 1P*測定値NIST
710.011312 nm19000C Iemission2s2.2p.3p 3D → 2s2.2p.5s 3P*測定値NIST
566.894 nm18000C Iemission2s2.2p.3p 1P → 2s2.2p.5d 1P*測定値NIST
596.933151 nm18000C Iemission2s.2p3 3D* → 2s2.2p.4p 3D測定値NIST
708.782188 nm18000C Iemission2s2.2p.3p 3D → 2s2.2p.4d 3D*測定値NIST
402.94119 nm16000C Iemission2s2.2p.3s 3P* → 2s2.2p.5p 3P測定値NIST
601.64487 nm16000C Iemission2s2.2p.3p 3D → 2s2.2p.5d 3F*測定値NIST
473.426281 nm15000C Iemission2s.2p3 3D* → 2s2.2p.5p 3P測定値NIST
481.737213 nm15000C Iemission2s2.2p.3s 3P* → 2s2.2p.4p 3S測定値NIST
579.446608 nm15000C Iemission2s.2p3 3D* → 2s2.2p.4p 3P測定値NIST
748.344451 nm15000C Iemission2s2.2p.3p 3S → 2s2.2p.4d 3P*測定値NIST
406.52425 nm14000C Iemission2s2.2p.3s 3P* → 2s2.2p.5p 3D測定値NIST
580.52017 nm14000C Iemission2s.2p3 3D* → 2s2.2p.4p 3P測定値NIST
601.4833 nm14000C Iemission2s2.2p.3p 3D → 2s2.2p.6s 3P*測定値NIST
710.89263 nm14000C Iemission2s2.2p.3p 3D → 2s2.2p.5s 3P*測定値NIST
400.9928 nm13000C Iemission2s2.2p.3s 1P* → 2s2.2p.6p 1P測定値NIST
422.83269 nm13000C Iemission2s2.2p.3s 1P* → 2s2.2p.5p 1S測定値NIST
447.85821 nm13000C Iemission2s.2p3 3D* → 2s2.2p.(2P*<1/2>).5f 2[5/2]測定値NIST
504.012903 nm12000C Iemission2s.2p3 3D* → 2s2.2p.(2P*<1/2>).4f 2[7/2]測定値NIST
601.0669 nm12000C Iemission2s2.2p.3p 3D → 2s2.2p.6s 3P*測定値NIST
406.4264 nm11000C Iemission2s2.2p.3s 3P* → 2s2.2p.5p 3D測定値NIST
639.7965 nm11000C Iemission2s2.2p.3p 3S → 2s2.2p.6s 3P*測定値NIST
666.3043 nm11000C Iemission2s2.2p.3p 3P → 2s2.2p.5d 3D*測定値NIST
667.1849 nm11000C Iemission2s2.2p.3p 3P → 2s2.2p.6s 3P*測定値NIST
403.180216 nm10000C Iemission2s2.2p.3s 3P* → 2s2.2p.5p 3P測定値NIST
482.679468 nm10000C Iemission2s2.2p.3s 3P* → 2s2.2p.4p 3S測定値NIST
598.903753 nm10000C Iemission2s.2p3 3D* → 2s2.2p.4p 3D測定値NIST
707.649944 nm9900C Iemission2s2.2p.3p 3D → 2s2.2p.4d 3D*測定値NIST
402.284321 nm9700C Iemission2s2.2p.3s 3P* → 2s2.2p.5p 3P測定値NIST
555.1578 nm9600C Iemission2s2.2p.3p 3D → 2s2.2p.7s 3P*測定値NIST
600.7173 nm9600C Iemission2s2.2p.3p 3D → 2s2.2p.6s 3P*測定値NIST
502.492938 nm9400C Iemission2s.2p3 3D* → 2s2.2p.(2P*<3/2>).4f 2[7/2]測定値NIST

詳細な性質

共有結合半径(詳細)

共有結合半径(Pyykkö)
75 pm
共有結合半径(Pyykkö、二重結合)
67 pm
共有結合半径(Pyykkö、三重結合)
60 pm
共有結合半径(Bragg)
77 pm

ファンデルワールス半径

Bondi
170 pm
Batsanov
170 pm
Alvarez
177 pm
UFF
385.1 pm
MM3
204 pm
Dreiding
389.83 pm
Rowland–Taylor
177 pm

原子半径と金属半径

原子半径(Rahm)
190 pm
金属半径(C12)
86 pm

番号付けの尺度

Mendeleev
87
Pettifor
95
Glawe
87

電気陰性度の尺度

Ghosh
0
Miedema
6
Gunnarsson–Lundqvist
7
Robles–Bartolotti
6

分極率と分散

双極子分極率
11.3 a.u.
双極子分極率(不確かさ)
0.2 a.u.
C₆
46.6 Ha·Bohr6
C₆ (Gould–Bučko)
47.9 Ha·Bohr6

ミーデマパラメータ

ミーデマモル体積
3.26 cm3/mol
ミーデマ電子密度
6

供給リスクと経済性

生産集中度
46
相対供給リスク
5
埋蔵量の分布
28
政治的安定性(最大生産国)
24
政治的安定性(最大埋蔵国)
57

相転移と同素体

graphite 昇華
沸点4098.15 K
三重点(温度)4762.15 K
三重点(圧力)10300 kPa

酸化数の分類

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

専門参考データ

遮蔽定数 (3)
n軌道σ
1s0.3273
2p2.8642
2s2.7834
結晶半径の詳細 (3)
電荷CNスピンrcrystal (pm)由来
4III6
4IV29Pauling's (1960) crystal radius,
4VI30Ahrens (1952) ionic radius,
同位体の崩壊形式 (27)
同位体モード強度
82p100%
9B+100%
9B+p7.5%
9B+A38.4%
10B+100%
11B+100%
14B-100%
15B-100%
16B-100%
16B-n99%
X線散乱因子 (502)
エネルギー (eV)f₁f₂
10—0.80688
10.1617—0.85152
10.3261—0.89863
10.4931—0.94834
10.6628—1.0008
10.8353—1.05755
11.0106—1.12167
11.1886—1.18968
11.3696—1.26181
11.5535—1.33832

追加データ

Isotopes in Forensic Science and Anthropology

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

Variations in the isotope-amount ratio n(13C)/n(12C) of biological products can be observed using isotope-ratio mass spectrometry (IRMS) to detect adulteration (the addition of inferior ingredients) in honey and other food products.

The isotope-amount ratio n(13C)/n(12C) can fluctuate between carbon sources, for example C3 plants (found in temperate climates and which use atmospheric carbon dioxide to make a 3-carbon molecule during photosynthesis — examples include rice, potatoes, tomatoes, and sugar beets), C4 plants (found in hot climates and which use atmospheric carbon dioxide to make a 4-carbon molecule during photosynthesis — examples include corn and sugar cane), animal carbon, atmospheric CO2, etc. This commonly makes it possible to detect whether these different carbon sources have been mixed by using isotope or mass balance to distinguish, for example, between beet sugar and cane sugar. Complications in source identification can arise with plants that open stomata at night to collect carbon dioxide to use a third mechanism to fix atmospheric carbon dioxide (CAM or crassulacean acid metabolism). The isotope-amount ratio n(13C)/n(12C) of CAM plants overlaps that of C3 or C4 plants — examples include pineapples and jade plants. The following adulterations are commonly detected using stable carbon isotope IRMS:

–Variations in the isotope-amount ratio n(13C)/n(12C) of honey are used to detect the addition (and potential adulteration) of high fructose corn syrup, corn, or sugar cane [67] C. Cordella, I. Moussa, A. C. Martel, N. Sbirrazzuoli, L. Lizzani-Cuvelier. J. Agric. Food. Chem.50, 1751 (2002)..

–Variations in the isotope-amount ratio n(13C)/n(12C) of fruit juice have been used to detect the addition of a sugar [67] C. Cordella, I. Moussa, A. C. Martel, N. Sbirrazzuoli, L. Lizzani-Cuvelier. J. Agric. Food. Chem.50, 1751 (2002)..

–Variations in the isotope-amount ratio n(13C)/n(12C) of natural vanilla extract have been used to detect the addition of artificial vanillin or p-hydroxybenzaldehyde [67] C. Cordella, I. Moussa, A. C. Martel, N. Sbirrazzuoli, L. Lizzani-Cuvelier. J. Agric. Food. Chem.50, 1751 (2002)..

–Variations in the isotope-amount ratio n(13C)/n(12C) of beer are used to detect C4 carbon, which would indicate that a beer company may have added ingredients that are not traditionally used in brewing beer. Therefore, this ratio is used to detect the misrepresentation of a product as being pure [67] C. Cordella, I. Moussa, A. C. Martel, N. Sbirrazzuoli, L. Lizzani-Cuvelier. J. Agric. Food. Chem.50, 1751 (2002)., [68] J. R. Brooks, N. Buchmann, S. Phillips, B. Ehleringer, R. D. Evans, M. Lott, L. A. Martinelli, W. T. Pockman, D. Sandquist, J. P. Sparks, L. Sperry, D. Williams, J. R. Ehleringer. J. Agric. Food. Chem.50, 6413 (2002)..

Stable carbon IRMS has been used to determine if the botanical origin of an alcoholic spirit has been mislabeled and if chaptalization (the process of adding sugar to increase the alcoholic content) of wine has occurred [67] C. Cordella, I. Moussa, A. C. Martel, N. Sbirrazzuoli, L. Lizzani-Cuvelier. J. Agric. Food. Chem.50, 1751 (2002)., [68] J. R. Brooks, N. Buchmann, S. Phillips, B. Ehleringer, R. D. Evans, M. Lott, L. A. Martinelli, W. T. Pockman, D. Sandquist, J. P. Sparks, L. Sperry, D. Williams, J. R. Ehleringer. J. Agric. Food. Chem.50, 6413 (2002).. 14C scintillation counting has been used to determine the age of wine and alcoholic spirits [67] C. Cordella, I. Moussa, A. C. Martel, N. Sbirrazzuoli, L. Lizzani-Cuvelier. J. Agric. Food. Chem.50, 1751 (2002)., [68] J. R. Brooks, N. Buchmann, S. Phillips, B. Ehleringer, R. D. Evans, M. Lott, L. A. Martinelli, W. T. Pockman, D. Sandquist, J. P. Sparks, L. Sperry, D. Williams, J. R. Ehleringer. J. Agric. Food. Chem.50, 6413 (2002).. Variations in the isotope-amount ratio n(13C)/n(12C) of urine has been used to determine if steroids in urine are natural or of synthetic origin. These measurements enable anti-doping laboratories to perfect their methods for detecting steroid doping in athletes [69] B. D. Ahrens, A. W. Butch. Drug Test Anal.5, 534 (2013)., [70] E. Bulska, D. Gorczyca, I. Zalewska, A. Pokrywka, D. Kwiatkowska. J. Pharm. Biomed. Anal.106, 159 (2015)., [71] A. Casilli, T. Piper, F. A. de Oliveira, M. Costa Padilha, H. Marcelo Pereira, M. Thevis, F. R. de Aquino Neto. Drug Test Anal.8, 1204 (2016).. Variations in the isotope-amount ratio n(13C)/n(12C) of marijuana can provide information to determine if the plants were grown “inside” a building or greenhouse or were “open grown” (Fig. IUPAC.6.4). Plant carbon isotopic compositions are controlled by atmospheric CO2 and the supply and demand of CO2 in photosynthesis (the process used by plants to convert light energy from the sun into chemical energy). “Open grown” plants are grown in an area that is well ventilated and receives natural CO2. In contrast, plants grown “inside” receive supplemented CO2 and the photosynthesis process is more confined. Additionally, CO2 from a tank of compressed gas used to augment atmospheric CO2 to increase the growth of marijuana plants is commonly highly depleted in 13C as a refinery by-product. These differences change the carbon isotope ratios of the plants and the ratios vary enough to enable the determination of the growing and cultivation process of marijuana [72] E. K. Shibuya, J. E. Souza Sarkis, O. N. Neto, M. Z. Moreira, R. L. Victoria. Forensic Sci. Int.160, 35 (2006)., [73] J. B. West, J. M. Hurley, J. R. Ehleringer. J Forensic Sci.54, 84 (2009)..

参考文献 (9)
  • [67] C. Cordella, I. Moussa, A. C. Martel, N. Sbirrazzuoli, L. Lizzani-Cuvelier. J. Agric. Food. Chem.50, 1751 (2002).
  • [68] J. R. Brooks, N. Buchmann, S. Phillips, B. Ehleringer, R. D. Evans, M. Lott, L. A. Martinelli, W. T. Pockman, D. Sandquist, J. P. Sparks, L. Sperry, D. Williams, J. R. Ehleringer. J. Agric. Food. Chem.50, 6413 (2002).
  • [69] B. D. Ahrens, A. W. Butch. Drug Test Anal.5, 534 (2013).
  • [70] E. Bulska, D. Gorczyca, I. Zalewska, A. Pokrywka, D. Kwiatkowska. J. Pharm. Biomed. Anal.106, 159 (2015).
  • [71] A. Casilli, T. Piper, F. A. de Oliveira, M. Costa Padilha, H. Marcelo Pereira, M. Thevis, F. R. de Aquino Neto. Drug Test Anal.8, 1204 (2016).
  • [72] E. K. Shibuya, J. E. Souza Sarkis, O. N. Neto, M. Z. Moreira, R. L. Victoria. Forensic Sci. Int.160, 35 (2006).
  • [73] J. B. West, J. M. Hurley, J. R. Ehleringer. J Forensic Sci.54, 84 (2009).
  • [74] United States Drug Enforcement Administration. Marijuana-Indoor Marijuana Grow, United States Department of Justice (2014), Feb. 22; http://www.justice.gov/dea/pr/multimedia-library/image-gallery/images_marijuana.shtml.
  • [4] IUPAC Periodic Table of the Elements and Isotopes (IPTEI) https://doi.org/10.1515/pac-2015-0703

参考文献

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

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)
Carbon

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
Carbon

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
Carbon

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
Carbon

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
Carbon

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

9 PubChem Elements
Carbon

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。