Allotropes of carbon

From Wikipedia, the free encyclopedia
  (Redirected from Prismane C8)
Jump to: navigation, search
Eight allotropes of carbon: a) diamond, b) graphite, c) lonsdaleite, d) C60 buckminsterfullerene, e) C540, Fullerite f) C70, g) amorphous carbon, and h) single-walled carbon nanotube.

Carbon is capable of forming many allotropes due to its valency. Well-known forms of carbon include diamond and graphite; in recent decades many more allotropes and forms of carbon have been discovered and researched including ball shapes such as buckminsterfullerene and sheets such as graphene. Larger scale structures of carbon include nanotubes, nanobuds and nanoribbons. Other unusual forms of carbon exist at very high temperatures or extreme pressures, around 500 hypothetical 3-periodic allotropes of carbon are known at the present time according to SACADA[1] database.


Diamond is a well known allotrope of carbon. The hardness and high dispersion of light of diamond make it useful for both industrial applications and jewelry. Diamond is the hardest known natural mineral, this makes it an excellent abrasive and makes it hold polish and luster extremely well. No known naturally occurring substance can cut (or even scratch) a diamond, except another diamond.

The market for industrial-grade diamonds operates much differently from its gem-grade counterpart. Industrial diamonds are valued mostly for their hardness and heat conductivity, making many of the gemological characteristics of diamond, including clarity and color, mostly irrelevant, this helps explain why 80% of mined diamonds (equal to about 100 million carats or 20 tonnes annually) are unsuitable for use as gemstones and known as bort, are destined for industrial use. In addition to mined diamonds, synthetic diamonds found industrial applications almost immediately after their invention in the 1950s; another 400 million carats (80 tonnes) of synthetic diamonds are produced annually for industrial use which is nearly four times the mass of natural diamonds mined over the same period.

The dominant industrial use of diamond is in cutting, drilling (drill bits), grinding (diamond edged cutters), and polishing. Most uses of diamonds in these technologies do not require large diamonds; in fact, most diamonds that are not gem-quality can find an industrial use. Diamonds are embedded in drill tips or saw blades, or ground into a powder for use in grinding and polishing applications (due to its extraordinary hardness). Specialized applications include use in laboratories as containment for high pressure experiments (see diamond anvil), high-performance bearings, and limited use in specialized windows.

With the continuing advances being made in the production of synthetic diamond, future applications are beginning to become feasible. Garnering much excitement is the possible use of diamond as a semiconductor suitable to build microchips from, or the use of diamond as a heat sink in electronics. Significant research efforts in Japan, Europe, and the United States are under way to capitalize on the potential offered by diamond's unique material properties, combined with increased quality and quantity of supply starting to become available from synthetic diamond manufacturers.

Each carbon atom in a diamond is covalently bonded to four other carbons in a tetrahedron, these tetrahedrons together form a 3-dimensional network of six-membered carbon rings (similar to cyclohexane), in the chair conformation, allowing for zero bond angle strain. This stable network of covalent bonds and hexagonal rings, is the reason that diamond is so strong, although graphite is the most stable allotrope of carbon under standard laboratory conditions (273 or 298 K, 1 atm), a recent computational study indicated that under idealized conditions (T = 0, p = 0), diamond is the most stable allotrope by 1.1 kJ/mol compared to graphite.[2]


Graphite, named by Abraham Gottlob Werner in 1789, from the Greek γράφειν (graphein, "to draw/write", for its use in pencils) is one of the most common allotropes of carbon. Unlike diamond, graphite is an electrical conductor. Thus, it can be used in, for instance, electrical arc lamp electrodes. Likewise, under standard conditions, graphite is the most stable form of carbon. Therefore, it is used in thermochemistry as the standard state for defining the heat of formation of carbon compounds.

Graphite conducts electricity, due to delocalization of the pi bond electrons above and below the planes of the carbon atoms. These electrons are free to move, so are able to conduct electricity. However, the electricity is only conducted along the plane of the layers; in diamond, all four outer electrons of each carbon atom are 'localised' between the atoms in covalent bonding. The movement of electrons is restricted and diamond does not conduct an electric current; in graphite, each carbon atom uses only 3 of its 4 outer energy level electrons in covalently bonding to three other carbon atoms in a plane. Each carbon atom contributes one electron to a delocalised system of electrons that is also a part of the chemical bonding, the delocalised electrons are free to move throughout the plane. For this reason, graphite conducts electricity along the planes of carbon atoms, but does not conduct in a direction at right angles to the plane.

Graphite powder is used as a dry lubricant, although it might be thought that this industrially important property is due entirely to the loose interlamellar coupling between sheets in the structure, in fact in a vacuum environment (such as in technologies for use in space), graphite was found to be a very poor lubricant. This fact led to the discovery that graphite's lubricity is due to adsorbed air and water between the layers, unlike other layered dry lubricants such as molybdenum disulfide. Recent studies suggest that an effect called superlubricity can also account for this effect.

When a large number of crystallographic defects bind these planes together, graphite loses its lubrication properties and becomes what is known as pyrolytic carbon, a useful material in blood-contacting implants such as prosthetic heart valves.

Graphite is the most stable allotrope of carbon. Contrary to popular belief, high-purity graphite does not readily burn, even at elevated temperatures,[3] for this reason, it is used in nuclear reactors and for high-temperature crucibles for melting metals.[4] At very high temperatures and pressures (roughly 2000 °C and 5 GPa), it can be transformed into diamond.[citation needed]

Natural and crystalline graphites are not often used in pure form as structural materials due to their shear-planes, brittleness and inconsistent mechanical properties.

In its pure glassy (isotropic) synthetic forms, pyrolytic graphite and carbon fiber graphite are extremely strong, heat-resistant (to 3000 °C) materials, used in reentry shields for missile nosecones, solid rocket engines, high temperature reactors, brake shoes and electric motor brushes.

Intumescent or expandable graphites are used in fire seals, fitted around the perimeter of a fire door, during a fire the graphite intumesces (expands and chars) to resist fire penetration and prevent the spread of fumes. A typical start expansion temperature (SET) is between 150 and 300 °C.

Density: graphite's specific gravity is 2.3, which makes it lighter than diamonds.

Chemical activity: it is slightly more reactive than diamond, this is because the reactants are able to penetrate between the hexagonal layers of carbon atoms in graphite. It is unaffected by ordinary solvents, dilute acids, or fused alkalis. However, chromic acid oxidises it to carbon dioxide.


A single layer of graphite is called graphene and has extraordinary electrical, thermal, and physical properties, it can be produced by epitaxy on an insulating or conducting substrate or by mechanical exfoliation (repeated peeling) from graphite. Its applications may include replacing silicon in high-performance electronic devices.

Amorphous carbon[edit]

Amorphous carbon is the name used for carbon that does not have any crystalline structure. As with all glassy materials, some short-range order can be observed, but there is no long-range pattern of atomic positions. While entirely amorphous carbon can be produced, most amorphous carbon actually contains microscopic crystals of graphite-like,[5] or even diamond-like carbon.[6]

Coal and soot or carbon black are informally called amorphous carbon. However, they are products of pyrolysis (the process of decomposing a substance by the action of heat), which does not produce true amorphous carbon under normal conditions.



The buckminsterfullerenes, or usually just fullerenes or buckyballs for short, were discovered in 1985 by a team of scientists from Rice University and the University of Sussex, three of whom were awarded the 1996 Nobel Prize in Chemistry. They are named for the resemblance of their allotropic structure to the geodesic structures devised by the scientist and architect Richard Buckminster "Bucky" Fuller. Fullerenes are molecules of varying sizes composed entirely of carbon, which take the form of a hollow sphere, ellipsoid, or tube.

As of the early twenty-first century, the chemical and physical properties of fullerenes are still under heavy study, in both pure and applied research labs; in April 2003, fullerenes were under study for potential medicinal use — binding specific antibiotics to the structure to target resistant bacteria and even target certain cancer cells such as melanoma.

Carbon nanotubes[edit]

Carbon nanotubes, also called buckytubes, are cylindrical carbon molecules with novel properties that make them potentially useful in a wide variety of applications (e.g., nano-electronics, optics, materials applications, etc.). They exhibit extraordinary strength, unique electrical properties, and are efficient conductors of heat. Inorganic nanotubes have also been synthesized. A nanotube is a member of the fullerene structural family, which also includes buckyballs. Whereas buckyballs are spherical in shape, a nanotube is cylindrical, with at least one end typically capped with a hemisphere of the buckyball structure, their name is derived from their size, since the diameter of a nanotube is on the order of a few nanometers (approximately 50,000 times smaller than the width of a human hair), while they can be up to several centimeters in length. There are two main types of nanotubes: single-walled nanotubes (SWNTs) and multi-walled nanotubes (MWNTs).

Carbon nanobuds[edit]

Computer models of stable nanobud structures

Carbon nanobuds are a newly discovered allotrope of carbon in which fullerene like "buds" are covalently attached to the outer sidewalls of the carbon nanotubes. This hybrid material has useful properties of both fullerenes and carbon nanotubes, for instance, they have been found to be exceptionally good field emitters.

Glassy carbon[edit]

A large sample of glassy carbon.

Glassy carbon or vitreous carbon is a class of non-graphitizing carbon widely used as an electrode material in electrochemistry, as well as for high-temperature crucibles and as a component of some prosthetic devices.

It was first produced by Bernard Redfern in the mid-1950s at the laboratories of The Carborundum Company, Manchester, UK, he had set out to develop a polymer matrix to mirror a diamond structure and discovered a resole (phenolic) resin that would, with special preparation, set without a catalyst. Using this resin the first glassy carbon was produced.

The preparation of glassy carbon involves subjecting the organic precursors to a series of heat treatments at temperatures up to 3000 °C. Unlike many non-graphitizing carbons, they are impermeable to gases and are chemically extremely inert, especially those prepared at very high temperatures, it has been demonstrated that the rates of oxidation of certain glassy carbons in oxygen, carbon dioxide or water vapour are lower than those of any other carbon. They are also highly resistant to attack by acids. Thus, while normal graphite is reduced to a powder by a mixture of concentrated sulfuric and nitric acids at room temperature, glassy carbon is unaffected by such treatment, even after several months.

Atomic and diatomic carbon[edit]

Under certain conditions, carbon can be found in its atomic form, it is formed by passing large electric currents through carbon under very low pressures. It is extremely unstable, but it is an intermittent product used in the creation of carbenes.[7]

Diatomic carbon can also be found under certain conditions. It is often detected via spectroscopy in extraterrestrial bodies, including comets and certain stars.[8][9]

Carbon nanofoam[edit]

Carbon nanofoam is the fifth known allotrope of carbon, discovered in 1997 by Andrei V. Rode and co-workers at the Australian National University in Canberra. It consists of a low-density cluster-assembly of carbon atoms strung together in a loose three-dimensional web.

Each cluster is about 6 nanometers wide and consists of about 4000 carbon atoms linked in graphite-like sheets that are given negative curvature by the inclusion of heptagons among the regular hexagonal pattern. This is the opposite of what happens in the case of buckminsterfullerenes, in which carbon sheets are given positive curvature by the inclusion of pentagons.

The large-scale structure of carbon nanofoam is similar to that of an aerogel, but with 1% of the density of previously produced carbon aerogels – only a few times the density of air at sea level. Unlike carbon aerogels, carbon nanofoam is a poor electrical conductor.

Carbide-derived carbon[edit]

Carbide-derived carbon (CDC) is a family of carbon materials with different surface geometries and carbon ordering that are produced via selective removal of metals from metal carbide precursors, such as TiC, SiC, Ti3AlC2, Mo2C, etc. This synthesis is accomplished using chlorine treatment, hydrothermal synthesis, or high-temperature selective metal desorption under vacuum. Depending on the synthesis method, carbide precursor, and reaction parameters, multiple carbon allotropes can be achieved, including endohedral particles composed of predominantly amorphous carbon, carbon nanotubes, epitaxial graphene, nanocrystalline diamond, onion-like carbon, and graphitic ribbons, barrels, and horns, these structures exhibit high porosity and specific surface areas, with highly tunable pore diameters, making them promising materials for supercapacitor-based energy storage, water filtration and capacitive desalinization, catalyst support, and cytokine removal.[10]

Lonsdaleite (hexagonal diamond)[edit]

Lonsdaleite is a hexagonal allotrope of the carbon allotrope diamond, believed to form from graphite present in meteorites upon their impact to Earth. The great heat and stress of the impact transforms the graphite into diamond, but retains graphite's hexagonal crystal lattice. Hexagonal diamond has also been synthesized in the laboratory, by compressing and heating graphite either in a static press or using explosives, it can also be produced by the thermal decomposition of a polymer, poly(hydridocarbyne), at atmospheric pressure, under inert gas atmosphere (e.g. argon, nitrogen), starting at temperature 110 °C (230 °F).[11][12][13]

Linear acetylenic carbon (LAC)[edit]

A one-dimensional carbon polymer with the structure -(C:::C)n-.

Other possible forms[edit]

Crystal structure of C8 cubic carbon
  • Chaoite is a mineral believed to have been formed in meteorite impacts. It has been described as slightly harder than graphite with a reflection colour of grey to white. However, the existence of carbyne phases is disputed – see the entry on chaoite for details.
  • Metallic carbon: Theoretical studies have shown that there are regions in the phase diagram, at extremely high pressures, where carbon has metallic character.[14]
  • bcc-carbon: At ultrahigh pressures of above 1000 GPa, diamond is predicted to transform into the so-called C8 structure, a body-centered cubic structure with 8 atoms in the unit cell. This cubic carbon phase might have importance in astrophysics, its structure is known in one of the metastable phases of silicon and is similar to cubane.[15] Superdense and superhard material resembling this phase has been synthesized and published in 1979 [16] and 2008,[17][18] the structure of this phase was proposed in 2012 as carbon sodalite.[19]
  • bct-carbon: Body-centered tetragonal carbon proposed by theorists in 2010[20][21]
  • M-carbon: Monoclinic C-centered carbon was first thought to have been created in 1963 by compressing graphite at room temperature. Its structure was theorized in 2006,[22] then in 2009 it was related[23] to those experimental observations. Many structural candidates, including bct-carbon, were proposed to be equally compatible with experimental data available at the time, until in 2012 it was theoretically proven that this structure is kinetically likeliest to form from graphite.[24][25] High-resolution data appeared shortly after, demonstrating that among all structure candidates only M-carbon is compatible with experiment.[26][27]
  • Q-carbon: Ferromagnetic carbon discovered in 2015.[28]
  • T-carbon: Every carbon atom in diamond is replaced with a carbon tetrahedron (hence 'T-carbon'). This was proposed by theorists in 2011.[29]
  • There is an evidence that white dwarf stars have a core of crystallized carbon and oxygen nuclei. The largest of these found in the universe so far, BPM 37093, is located 50 light-years (4.7×1014 km) away in the constellation Centaurus. A news release from the Harvard-Smithsonian Center for Astrophysics described the 2,500-mile (4,000 km)-wide stellar core as a diamond,[30] and it was named as Lucy, after the Beatles' song "Lucy in the Sky With Diamonds";[31] however, it is more likely an exotic form of carbon.
The K4 crystal
  • The Laves graph or K4 crystal is a theoretically-predicted three-dimensional crystalline metastable carbon structure in which each carbon atom is bonded to three others, at 120° angles (like graphite), but where the bond planes of adjacent layers lie at an angle of 70.5°, rather than coinciding[33][34]
  • Penta-graphene
  • Haeckelites Ordered arrangements of pentagons, hexagons, and heptagons which can either be flat or tubular.
  • Phagraphene Graphene allotrope with distorted Dirac cones.

Variability of carbon[edit]

Diamond and graphite are two allotropes of carbon: pure forms of the same element that differ in structure.

The system of carbon allotropes spans an astounding range of extremes, considering that they are all merely structural formations of the same element.

Between diamond and graphite:

  • Diamond crystallizes in the cubic system but graphite crystallizes in the hexagonal system.
  • Diamond is clear and transparent, but graphite is black and opaque.
  • Diamond is the hardest mineral known (10 on the Mohs scale), but graphite is one of the softest (1–2 on Mohs scale).
  • Diamond is the ultimate abrasive, but graphite is soft and is a very good lubricant.
  • Diamond is an excellent electrical insulator, but graphene is an excellent conductor.
  • Diamond is an excellent thermal conductor, but some forms of graphite are used for thermal insulation (for example heat shields and firebreaks).
  • At standard temperature and pressure, graphite is the thermodynamically stable form. Thus diamonds do not exist forever, the conversion from diamond to graphite, however, has a very high activation energy and is therefore extremely slow.

Despite the hardness of diamonds, the chemical bonds that hold the carbon atoms in diamonds together are actually weaker than those that hold together graphite, the difference is that in diamond, the bonds form an inflexible three-dimensional lattice. In graphite, the atoms are tightly bonded into sheets, but the sheets can slide easily over each other, making graphite soft.[35]

See also[edit]


  1. ^ Hoffmann, R.; Kabanov, A.; Golov, A.; Proserpio, D. (2016). "Homo Citans and Carbon Allotropes: For an Ethics of Citation". Angewandte Chemie. 55: 10962–10976. doi:10.1002/anie.201600655. 
  2. ^ Grochala, Wojciech (2014-04-01). "Diamond: Electronic Ground State of Carbon at Temperatures Approaching 0 K". Angewandte Chemie International Edition. 53 (14): 3680–3683. ISSN 1521-3773. PMID 24615828. doi:10.1002/anie.201400131. 
  3. ^ Glowing nuclear reactor graphite 2. YouTube (2007-11-07). Retrieved on 2015-10-22.
  4. ^ Crucibles, Artisan Foundry Shop. Retrieved on 2015-10-22.
  5. ^ Randall L. Vander Wal (1996). "Soot Precursor Material: Spatial Location via Simultaneous LIF-LII Imaging and Characterization via TEM: NASA Contractor Report 198469". 
  6. ^ "IUPAC Compendium of Chemical Terminology 2nd Edition (1997) diamond-like carbon films". 
  7. ^ Reactions of Atomic Carbon with Acid Chlorides. None. Retrieved on 2011-11-23.
  8. ^ Martin Harwit (1998). Astrophysical concepts. Springer. ISBN 978-0-387-94943-7. Retrieved 24 November 2011. 
  9. ^ Green Comet Approaches Earth. (2009-02-24). Retrieved on 2011-11-23.
  10. ^ Presser, Volker; Heon, Min; Gogotsi, Yury (2011). "Carbide-Derived Carbons – From Porous Networks to Nanotubes and Graphene". Advanced Functional Materials. 21 (5): 810–833. doi:10.1002/adfm.201002094. 
  11. ^ Bianconi P, et al. (2004). "Diamond and Diamond-like Carbon from a Preceramic Polymer". Journal of the American Chemical Society. 126 (10): 3191–3202. PMID 15012149. doi:10.1021/ja039254l. 
  12. ^ Nur, Yusuf; Pitcher, Michael; Seyyidoğlu, Semih; Toppare, Levent (2008). "Facile Synthesis of Poly(hydridocarbyne): A Precursor to Diamond and Diamond-like Ceramics". Journal of Macromolecular Science Part A. 45 (5): 358. doi:10.1080/10601320801946108. 
  13. ^ Nur, Yusuf; Cengiz, Halime M.; Pitcher, Michael W.; Toppare, Levent K. (2009). "Electrochemical polymerizatıon of hexachloroethane to form poly(hydridocarbyne): a pre-ceramic polymer for diamond production". Journal of Materials Science. 44 (11): 2774. Bibcode:2009JMatS..44.2774N. doi:10.1007/s10853-009-3364-4. 
  14. ^ Correa, Aa; Bonev, Sa; Galli, G (Jan 2006). "Carbon under extreme conditions: phase boundaries and electronic properties from first-principles theory". Proceedings of the National Academy of Sciences of the United States of America. 103 (5): 1204–8. Bibcode:2006PNAS..103.1204C. ISSN 0027-8424. PMC 1345714Freely accessible. PMID 16432191. doi:10.1073/pnas.0510489103. 
  15. ^ Johnston, Roy L.; Hoffmann, Roald (1989). "Superdense carbon, C8: supercubane or analog of .gamma.-silicon?". Journal of the American Chemical Society. 111 (3): 810. doi:10.1021/ja00185a004. 
  16. ^ Matyushenko N.N.; Strel'nitsky V.E. (1979). "JETP Letters: issues online". p. 199. 
  17. ^ Liu, P.; Cui, H.; Yang, G. W. (2008). "Synthesis of Body-Centered Cubic Carbon Nanocrystals". Crystal Growth & Design. 8 (2): 581. doi:10.1021/cg7006777. 
  18. ^ Liu, P; Cao, Yl; Wang, Cx; Chen, Xy; Yang, Gw (Aug 2008). "Micro- and nanocubes of carbon with C8-like and blue luminescence". Nano letters. 8 (8): 2570–5. Bibcode:2008NanoL...8.2570L. ISSN 1530-6984. PMID 18651780. doi:10.1021/nl801392v. 
  19. ^ Pokropivny, Alex; Volz, Sebastian (2012-09-01). "‘C8 phase’: Supercubane, tetrahedral, BC-8 or carbon sodalite?". physica status solidi (b). 249 (9): 1704–1708. Bibcode:2012PSSBR.249.1704P. ISSN 1521-3951. doi:10.1002/pssb.201248185. 
  20. ^ Wolfram Demonstrations Project. Retrieved on 2011-11-23.
  21. ^ Edwards, Lin (November 8, 2010) Structure of new form of super-hard carbon identified. Retrieved on 2011-11-23.
  22. ^ Oganov A. R.; Glass C. W. (2006). "Crystal structure prediction using ab initio evolutionary techniques: principles and applications". J. Chem. Phys. 124 (3): 244704. Bibcode:2006JChPh.124c4704K. doi:10.1063/1.2155529. 
  23. ^ Li, Q.; Ma, Y.; Oganov, A.R.; Wang, H.B.; Wang, H.; Xu, Y.; Cui, T.; Mao, H.-K.; Zou, G. (2009). "Superhard monoclinic polymorph of carbon". Phys. Rev. Lett. 102 (17): 175506. Bibcode:2009PhRvL.102q5506L. PMID 19518796. doi:10.1103/PhysRevLett.102.175506. 
  24. ^ Boulfelfel S.E.; Oganov A.R.; Leoni S. (2012). "Understanding the nature of "superhard graphite"". Scientific Reports. 2: 471. Bibcode:2012NatSR...2E.471B. PMC 3384968Freely accessible. PMID 22745897. arXiv:1204.4750Freely accessible. doi:10.1038/srep00471. 
  25. ^ Oganov, Artem R. (27 June 2012). "Researchers establish structure of a new superhard form of carbon". Retrieved 23 July 2012. 
  26. ^ Wang Y.; Panzik J.E.; Kiefer B.; Lee K.K.M. (2012). "Crystal structure of graphite under room-temperature compression and decompression". Scientific Reports. 2: 520. Bibcode:2012NatSR...2E.520W. PMC 3400081Freely accessible. PMID 22816043. doi:10.1038/srep00520. 
  27. ^ Lee, Kanani K. M. (20 July 2012). "Diamond in the rough: Half-century puzzle solved". Retrieved 23 July 2012. 
  28. ^ Narayan, Jagdish; Bhaumik, Anagh (2 December 2015). "Novel phase of carbon, ferromagnetism, and conversion into diamond". Journal of Applied Physics. J. Appl. Phys. 118 (215303): 215303. Bibcode:2015JAP...118u5303N. doi:10.1063/1.4936595. Retrieved 2 December 2015. 
  29. ^ Zyga, Lisa (April 22, 2011) New carbon allotrope could have a variety of applications. Retrieved on 2012-08-09.
  30. ^ "This Valentine's Day, Give The Woman Who Has Everything The Galaxy's Largest Diamond". Center for Astrophysics. Retrieved 2009-05-05. 
  31. ^ Cauchi, S. (2004-02-18). "Biggest Diamond Out of This World". The Age. Archived from the original on 4 November 2007. Retrieved 2007-11-11. 
  32. ^ Openov, Leonid A.; Elesin, Vladimir F. (1998). "Prismane C8: A new form of carbon?". JETP Letters. 68 (9): 726. Bibcode:1998JETPL..68..726O. arXiv:physics/9811023Freely accessible. doi:10.1134/1.567936. 
  33. ^ Itoh, Masahiro; Kotani, Motoko; Naito, Hisashi; Sunada, Toshikazu; Kawazoe, Yoshiyuki; Adschiri, Tadafumi (2009), "New metallic carbon crystal", Physical Review Letters, 102 (5): 055703, Bibcode:2009PhRvL.102e5703I, doi:10.1103/PhysRevLett.102.055703 
  34. ^ Tagami, Makoto; Liang, Yunye; Naito, Hisashi; Kawazoe, Yoshiyuki; Kotani, Motoko (2014), "Negatively curved cubic carbon crystals with octahedral symmetry", Carbon, 76: 266–274, doi:10.1016/j.carbon.2014.04.077 
  35. ^ Gray, Theodore (September 2009). "Gone in a Flash". Popular Science: 70. 

External links[edit]