14
Si
Silicon
Atomic Mass 28.0855
Electron Configuration [Ne]3s23p2
Oxidation States +4, +2, -4
Year Discovered 1854

Identifiers

Element Name Silicon
Element Symbol Si
InChI InChI=1S/Si
InChIKey XUIMIQQOPSSXEZ-UHFFFAOYSA-N

Properties

Atomic Weight

[28.084, 28.086]

28.0855

28.09

[28.084,28.086]

Electron Configuration

[Ne]3s23p2

Atomic Radius

Van der Waals Atomic Radius : 210 pm (Van der Waals)

Empirical Atomic Radius : 110pm (Empirical)

Covalent Atomic Radius : 111(2) pm (Covalent)

Oxidation States

+4, +2, -4

4, 3, 2, 1 -1, -2, -3, -4 ​(an amphoteric oxide)

Ground Level

3P0

Ionization Energy

8.152 eV

8.15168 ± 0.00003 eV

Electronegativity

Pauling Scale Electronegativity : 1.9(Pauling Scale)

Allen Scale Electronegativity : 1.916(Allen Scale)

Electron Affinity

1.385eV

1.36eV

Atomic Spectra

Lines Holdings

Levels Holdings

Physical Description

Solid

Element Classification

Semi-metal

Element Period Number

3

Element Group Number

14

Density

2.3296 grams per cubic centimeter

Melting Point

1687 K (1414°C or 2577°F)

1414°C

Boiling Point

3538 K (3265°C or 5909°F)

3265°C

Estimated Crustal Abundance

2.82×105 milligrams per kilogram

Estimated Oceanic Abundance

2.2 milligrams per liter

History

The name derives from the Latin silex and silicis for "flint". Amorphous silicon was discovered by the Swedish chemist Jöns Jacob Berzelius in 1824. Crystalline silicon was first prepared by the French chemist Henri Sainte-Claire Deville in 1854.

Silicon was discovered by Jöns Jacob Berzelius, a Swedish chemist, in 1824 by heating chips of potassium in a silica container and then carefully washing away the residual by-products. Silicon is the seventh most abundant element in the universe and the second most abundant element in the earth's crust. Today, silicon is produced by heating sand (SiO2) with carbon to temperatures approaching 2200°C.

From the Latin. word silex, silicis, flint. In 1800, Davy thought silica to be a compound and not an element; but in 1811, Gay Lussac and Thenard probably prepared impure amorphous silicon by heating potassium with silicon tetrafluoride.

In 1824 Berzelius, generally credited with the discovery, prepared amorphous silicon by the same general method and purified the product by removing the fluosilicates by repeated washings. Deville in 1854 first prepared crystalline silicon, the second allotropic form of the element.

Historical Atomic Weights

Year Atomic Weight (uncertainty) [u] Reference
2009 [28.084, 28.086] https://doi.org/10.1351/PAC-REP-10-09-14
1975 28.0855(3) https://doi.org/10.1351/pac197647010075
1969 28.086(3) https://doi.org/10.1351/pac197021010091
1961 28.086(1) https://doi.org/10.1021/ja00881a001
1951 28.09 https://doi.org/10.1039/JR9530000001
1925 28.06 https://doi.org/10.1039/CT9252700913
1922 28.1 https://doi.org/10.1021/ja01441a001
1909 28.3 https://doi.org/10.1021/ja01931a001
1902 28.4 https://doi.org/10.1007/BF01370337

Historical Isotopic Abundances

Year Isotope Abundance (uncertainty) Reference
2013 28Si [0.921 91, 0.923 18] https://doi.org/10.1515/pac-2015-0503
2013 29Si [0.046 45, 0.046 99] https://doi.org/10.1515/pac-2015-0503
2013 30Si [0.030 37, 0.031 10] https://doi.org/10.1515/pac-2015-0503
2001 28Si 0.922 23(19) https://doi.org/10.1063/1.1836764
2001 29Si 0.046 85(8) https://doi.org/10.1063/1.1836764
2001 30Si 0.030 92(11) https://doi.org/10.1063/1.1836764
1997 28Si 0.922 297(7) https://doi.org/10.1351/pac199870010217
1997 29Si 0.046 832(5) https://doi.org/10.1351/pac199870010217
1997 30Si 0.030 872(5) https://doi.org/10.1351/pac199870010217
1975 28Si 0.9223 https://doi.org/10.1351/pac197647010075
1975 29Si 0.0467 https://doi.org/10.1351/pac197647010075
1975 30Si 0.031 https://doi.org/10.1351/pac197647010075

Description

Crystalline silicon has a metallic luster and grayish color. Silicon is a relatively inert element, but it is attacked by halogens and dilute alkali. Most acids, except hydrofluoric, do not affect it. Elemental silicon transmits more than 95% of all wavelengths of infrared, from 1.3 to 6.y micro-m.

Users

Two allotropes of silicon exist at room temperature: amorphous and crystalline. Amorphous appears as a brown powder while crystalline silicon has a metallic luster and a grayish color. Single crystals of crystalline silicon can be grown with a process known as the Czochralski process. These crystals, when doped with elements such as boron, gallium, germanium, phosphorus or arsenic, are used in the manufacture of solid-state electronic devices, such as transistors, solar cells, rectifiers and microchips.

Silicon dioxide (SiO2), silicon's most common compound, is the most abundant compound in the earth's crust. It commonly takes the form of ordinary sand, but also exists as quartz, rock crystal, amethyst, agate, flint, jasper and opal. Silicon dioxide is extensively used in the manufacture of glass and bricks. Silica gel, a colloidal form of silicon dioxide, easily absorbs moisture and is used as a desiccant.

Silicon forms other useful compounds. Silicon carbide (SiC) is nearly as hard as diamond and is used as an abrasive. Sodium silicate (Na2SiO3), also known as water glass, is used in the production of soaps, adhesives and as an egg preservative. Silicon tetrachloride (SiCl4) is used to create smoke screens. Silicon is also an important ingredient in silicone, a class of material that is used for such things as lubricants, polishing agents, electrical insulators and medical implants.

Silicon is one of man's most useful elements. In the form of sand and clay it is used to make concrete and brick; it is a useful refractory material for high-temperature work, and in the form of silicates it is used in making enamels, pottery, etc. Silica, as sand, is a principal ingredient of glass, one of the most inexpensive of materials with excellent mechanical, optical, thermal, and electrical properties. Glass can be made in a very great variety of shapes, and is used as containers, window glass, insulators, and thousands of other uses. Silicon tetrachloride can be used as iridize glass.

Hyperpure silicon can be doped with boron, gallium, phosphorus, or arsenic to produce silicon for use in transistors, solar cells, rectifiers, and other solid-state devices which are used extensively in the electronics and space-age industries.

Hydrogenated amorphous silicon has shown promise in producing economical cells for converting solar energy into electricity.

Silicon is important to plant and animal life. Diatoms in both fresh and salt water extract Silica from the water to build their cell walls. Silica is present in the ashes of plants and in the human skeleton. Silicon is an important ingredient in steel; silicon carbide is one of the most important abrasives and has been used in lasers to produce coherent light of 4560 A.

Silcones are important products of silicon. They may be prepared by hydrolyzing a silicon organic chloride, such as dimethyl silicon chloride. Hydrolysis and condensation of various substituted chlorosilanes can be used to produce a very great number of polymeric products, or silicones, ranging from liquids to hard, glasslike solids with many useful properties.

Sources

Silicon is present in the sun and stars and is a principal component of a class of meteorites known as aerolites. It is also a component of tektites, a natural glass of uncertain origin.

Silicon makes up 25.7% of the earth's crust, by weight, and is the second most abundant element, being exceeded only by oxygen. Silicon is not found free in nature, but occurs chiefly as the oxide and as silicates. Sand, quartz, rock crystal, amethyst, agate, flint, jasper, and opal are some of the forms in which the oxide appears. Granite, hornblende, asbestos, feldspar, clay, mica, etc. are but a few of the numerous silicate minerals.

Silicon is prepared commercially by heating silica and carbon in an electric furnace, using carbon electrodes. Several other methods can be used for preparing the element. Amorphous silicon can be prepared as a brown powder, which can be easily melted or vaporized. The Czochralski process is commonly used to produce single crystals of silicon used for solid-state or semiconductor devices. Hyperpure silicon can be prepared by the thermal decomposition of ultra-pure trichlorosilane in a hydrogen atmosphere, and by a vacuum float zone process.

Compounds

See more information at the Silicon compound page.

Element Forms

CID Name Formula SMILES Molecular Weight
5461123 silicon Si [Si] 28.085
4082203 silicon(4+) Si+4 [Si+4] 28.085
16048636 silicon-28 Si [28Si] 27.976926534
6337619 silicon-31 Si [31Si] 30.9753632
9898792 silicon-29 Si [29Si] 28.976494664
16019983 silicon(1+) Si+ [Si+] 28.085
16048635 silicon-30 Si [30Si] 29.9737701
6335897 silicon-32 Si [32Si] 31.974152
6336987 silicon(1-) Si- [Si-] 28.085
16207196 silicon(2+) Si+2 [Si+2] 28.085
22138154 silicon(3+) Si+3 [Si+3] 28.085

Handling And Storage

Miners, stonecutters, and others engaged in work where siliceous dust is breathed into large quantities often develop a serious lung disease known as silicosis.

Isotopes

Stable Isotope Count 3

Isotopes in Earth/Planetary Science

Because molecules, atoms, and ions of the stable isotopes of silicon possess slightly different physical and chemical properties, they commonly will be fractionated during physical, chemical, and biological processes, giving rise to variations in isotopic abundances and in atomic weights. There are substantial variations in the isotopic abundances of silicon in natural terrestrial materials (Fig. IUPAC.14.1). These variations are useful in investigating the origin of substances and studying environmental, hydrological, and geological processes [13], [17]. Diatoms, a major group of algae, need silicon to build up their opaline shells and prefer 28Si while taking up Si(OH)4, which is the biologically available form of silicon in the marine environment. This progressively enriches surface waters with 29Si and 30Si [123]. 32Si-labeled silicic acid of high specific radioactivity is used to measure uptake rates of Si and estimate marine sedimentation of biogenic (created by living organisms) silica (by diatoms and sea shells). By performing uptake kinetic experiments, the 32Si activity can be measured as 32P using counting of Cherenkov radiation (radiation produced by charged particles passing through a medium at a speed greater than that of light through the same medium — after Soviet physicist Pavel A. Cherenkov) with a liquid scintillation analyzer (measuring ionizing radiation using the interaction of radiation on a material and counting the resulting photon emissions).

Fig. IUPAC.14.1 : Variation in atomic weight with isotopic composition of selected silicon-bearing materials (modified from [13], [17]).

[13] M. W. Wieser, T. B. Coplen. Pure Appl Chem.83, 359 (2011).
[17] T. B. Coplen, J. A. Hopple, J. K. Böhlke, H. S. Peiser, S. E. Rieder, H. R. Krouse, K. J. R. Rosman, T. Ding, R. D. Vocke, K. Revesz, A. Lamberty, P. D. P. Taylor, P. D. Bièvre. United States Geological Survey Water-Resources Investigations Report, 01-4222, (2002).
[123] S. Kristiansen, T. Farbrot, L. J. Naustvoll. Limnol. Oceanogr.45, 472 (2000).

Isotopes in Geochronology

Cosmogenic 32Si has a half-life of about 150 years and is produced by cosmic-ray spallation of argon in the stratosphere and troposphere [124]. 32Si in dust is precipitated in snow, making it possible to date dust in snow and glacial ice (Fig. IUPAC.14.2). Glaciers are archives for global climate history because they contain a variety of proxies (imprints of past environmental conditions used to interpret paleoclimate) for climate forcing and climate response. Cosmogenic 32Si that is stored in glaciers and ice-core samples can be analyzed using accelerator mass spectrometry to date when sections of glaciers formed [125], [126].

Fig. IUPAC.14.2: ³²Si activity concentrations in three snow samples from Jungfraujoch, a glacial pass in the Bernese Alps at an elevation of approximately 3.5 km above sea level (modified from [127]). Sample Jungfraujoch 2 contains Saharan dust and has a substantially higher concentration of ³²Si than snow samples not containing Saharan dust.

[124] C. Schnabel, J. Beer, H. B. Clausen. Geophys. Res. Abstr.11, (2009).
[125] SAHRA – Sustainability of Semi-Arid Hydrology and Riparian Areas. Silicon, SAHRA – Sustainability of Semi-Arid Hydrology and Riparian Areas (2014), Feb. 24; http://web.sahra.arizona.edu/programs/isotopes/silicon.html.
[126] GNS Science. Climate Change Studies & Ice Core Research, GNS Science (2014), Feb. 24; http://www.gns.cri.nz/Home/Services/Laboratories-Facilities/Tritium-and-Water-Dating-Laboratory/Research-Programmes/Climate-change-studies-ice-core-research.
[127] U. Morgenstern, C. B. Taylor, Y. Parrat, H. W. Gäggeler, B. Eichler. Earth Planet. Sci. Lett.144, 289 (1996).

Isotopes in Industry

At Keio University in Japan, the Itoh Research Group has developed a method that utilizes 29Si to store and process information. The Itoh Research Group focused on manipulating the nanostructure of materials at an atomic level, especially with semiconductors such as silicon. Their manipulations and observations demonstrate that differences in the nuclear spin and mass of an isotope affects the ease of further manipulation of the isotope [128], [129].

Silicon crystals enriched to higher than 99.99 percent purity of 28Si are being used in the Avogadro Project. This project is intended to remeasure the Avogadro constant (NA), which is the proportionality factor between the amount of substance and number of elementary entities [130].

[128] Kohei ITOH research group at Keio University, Japan. Itoh Group at Keio University, Japan, Kohei ITOH research group at Keio University, Japan (2014), Feb. 24; http://www.appi.keio.ac.jp/Itoh_group/research/.
[129] T. Itahashi, H. Hayashi, M. R. Rahman, K. M. Itoh, L. S. Vlasenko, M. P. Vlasenko, D. S. Poloskin. Phys. Rev. B87, 075201-1 (2013).
[130] R. Marquardt, J. Meija, Z. Mester, M. Towns, R. Weir, R. Davis, J. Stohner. Pure Appl. Chem.90, 175 (2018).

Isotope Mass and Abundance

Isotope Atomic Mass (uncertainty) [u] Abundance (uncertainty)
28Si 27.976 926 535(3) [0.921 91, 0.923 18]
29Si 28.976 494 665(4) [0.046 45, 0.046 99]
30Si 29.973 7701(2) [0.030 37, 0.031 10]
Isotope Atomic Mass (uncertainty) [u] Abundance (uncertainty)
28Si 27.97692653465(44) 0.92223(19)
29Si 28.97649466490(52) 0.04685(8)
30Si 29.973770136(23) 0.03092(11)

Atomic Mass, Half Life, and Decay

Nuclide Atomic Mass and Uncertainty [u] Half Life and Uncertainty Discovery Year Decay Modes, Intensities and Uncertainties [%]
22Si 22.036114 ± 0.000537 [Estimated] 28.7 ms ± 1.1 1987 β+=100%; β+p=62±0.5%; β+2p=0.7±0.3%
23Si 23.025711 ± 0.000537 [Estimated] 42.3 ms ± 0.4 1986 β+=100%; β+p≈88%; β+2p=3.6±0.3%
24Si 24.011535430 ± 0.000020904 143.2 ms ± 2.1 1979 β+=100%; β+p=34.5±1.4%
25Si 25.004108798 ± 0.000010735 220.6 ms ± 1.0 1963 β+=100%; β+p=35±0.2%
26Si 25.992333818 ± 0.000000115 2.2453 s ± 0.0007 1960 β+=100%
27Si 26.986704687 ± 0.000000115 4.117 s ± 0.014 1939 β+=100%
28Si 27.97692653442 ± 0.00000000055 Stable 1920 IS=92.2545±3.7%
28Sir 27.97692653442 ± 0.00000000055 Not-specified
29Si 28.97649466434 ± 0.0000000006 Stable 1920 IS=4.672±1.6%
30Si 29.973770137 ± 0.000000023 Stable 1924 IS=3.0735±2.1%
31Si 30.975363196 ± 0.000000046 157.16 m ± 0.20 1934 β-=100%
32Si 31.974151538 ± 0.00000032 157 y ± 7 1953 β-=100%
33Si 32.977976964 ± 0.00000075 6.18 s ± 0.18 1971 β-=100%
34Si 33.978538045 ± 0.00000086 2.77 s ± 0.20 1971 β-=100%
34Sim 33.978538045 ± 0.00000086 <210 ns 1989 IT=100%
35Si 34.984550111 ± 0.000038494 780 ms ± 120 1971 β-=100%; β-n<5%
36Si 35.986649271 ± 0.000077077 503 ms ± 2 1971 β-=100%; β-n=12±0.5%
37Si 36.992945191 ± 0.000122179 141.0 ms ± 3.5 1979 β-=100%; β-n=17±1.3%; β-2n ?
38Si 37.995523000 ± 0.0001125 63 ms ± 8 1979 β-=100%[Estimated]; β-n=25±1%
39Si 39.002491000 ± 0.0001455 41.2 ms ± 4.1 1979 β-=100%; β-n=33±0.3%; β-2n ?
40Si 40.006083641 ± 0.000130962 31.2 ms ± 2.6 1989 β-=100%; β-n=38±0.5%; β-2n ?
41Si 41.014171 ± 0.000322 [Estimated] 20.0 ms ± 2.5 1989 β-=100%; β-n>55%; β-2n ?
42Si 42.018078 ± 0.000322 [Estimated] 12.5 ms ± 3.5 1990 β-=100%; β-n ?; β-2n ?
43Si 43.026119 ± 0.000429 [Estimated] 30 ms >260ns [Estimated] 2002 β- ?; β-n ?; β-2n ?
44Si 44.031466 ± 0.000537 [Estimated] 4 ms >360ns [Estimated] 2007 β- ?; β-n ?; β-2n ?
45Si 45.039818 ± 0.000644 [Estimated] 4 ms [Estimated] β- ?; β-n ?; β-2n ?

Information Sources

  1. 1.  PubChem
  2. 2.  Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
  3. 3.  IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)
  4. 4.  Jefferson Lab, U.S. Department of Energy
    LICENSE
    Please see citation and linking information https https://www.jlab.org/privacy-and-security-notice
  5. 5.  Los Alamos National Laboratory, U.S. Department of Energy
  6. 6.  NIST Physical Measurement Laboratory
  7. 7.  IUPAC Periodic Table of the Elements and Isotopes (IPTEI)
    LICENSE
    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.
    https://creativecommons.org/licenses/by-nc-nd/4.0/
  8. 8.  PubChem Elements
    Silicon

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