Aggregated diamond nanorod

Aggregated diamond nanorods, or ADNRs, are a nanocrystalline form of diamond, also known as nanodiamond or hyperdiamond.

"hyperdiamond" redirects here. For 4-polytope, see 24-cell.
Natural nanodiamond aggregates from the Popigai impact structure, Siberia, Russia.[1]
Internal structure of the Popigai nanodiamonds.[1]
Internal structure of synthetic nanodiamonds.[1]

Discovery

Nanodiamond or hyperdiamond was produced by compression of graphite in 2003 by a group of researchers in Japan and in the same work, published in Nature, it was shown to be much harder than bulk diamond.[2] Later, it was also produced by compression of fullerene and confirmed to be the hardest and least compressible known material, with an isothermal bulk modulus of 491 gigapascals (GPa), while a conventional diamond has a modulus of 442–446 GPa; these results were inferred from X-ray diffraction data, which also indicated that ADNRs are 0.3% denser than regular diamond.[3] The same group later described ADNRs as "having a hardness and Young's modulus comparable to that of natural diamond, but with 'superior wear resistance'".[4]

Hardness

A <111> surface (normal to the largest diagonal of a cube) of pure diamond has a hardness value of 167±6 GPa when scratched with a nanodiamond tip, while the nanodiamond sample itself has a value of 310 GPa when tested with a nanodiamond tip. However, the test only works properly with a tip made of harder material than the sample being tested due to cracking. This means that the true value for nanodiamond is likely lower than 310 GPa.[5] Due to its hardness, a hyperdiamond could possibly exceed 10 on the Mohs scale of mineral hardness.

Synthesis

ADNRs (hyperdiamonds/nanodiamonds) are produced by compressing fullerite powder—a solid form of allotropic carbon fullerene—by either of two somewhat similar methods. One uses a diamond anvil cell and applied pressure ~37 GPa without heating the cell.[6] In another method, fullerite is compressed to lower pressures (2–20 GPa) and then heated to a temperature in the range of 300 to 2,500 K (27 to 2,227 °C).[7][8][9][10] Extreme hardness of what now appears likely to have been nanodiamonds was reported by researchers in the 1990s.[5][6] The material is a series of interconnected diamond nanorods, with diameters of between 5 and 20 nanometres and lengths of around 1 micrometre each.

Nanodiamond aggregates ca. 1 mm in size also form in nature, from graphite upon meteoritic impact, such as that of the Popigai impact structure in Siberia, Russia.[1]

See also
  • Adamant – Mythological hardest substance
  • Carbon nanotube – Allotropes of carbon with a cylindrical nanostructure
  • Diamond – Form of carbon
  • Fullerite – Allotrope of carbons
  • Lonsdaleite – Hexagonal lattice allotrope of carbon
  • Mohs scale of mineral hardness – Qualitative scale characterizing scratch resistance
  • Rhenium diboride – chemical compound
  • Superhard material – Material with Vickers hardness exceeding 40 gigapascals

References
  1. Ohfuji, Hiroaki; Irifune, Tetsuo; Litasov, Konstantin D.; Yamashita, Tomoharu; Isobe, Futoshi; Afanasiev, Valentin P.; Pokhilenko, Nikolai P. (2015). "Natural occurrence of pure nano-polycrystalline diamond from impact crater". Scientific Reports. 5: 14702. Bibcode:2015NatSR...514702O. doi:10.1038/srep14702. PMC 4589680. PMID 26424384.
  2. Irifune, Tetsuo; Kurio, Ayako; Sakamoto, Shizue; Inoue, Toru; Sumiya, Hitoshi (2003). "Materials: Ultrahard polycrystalline diamond from graphite". Nature. 421 (6923): 599–600. Bibcode:2003Natur.421..599I. doi:10.1038/421599b. PMID 12571587. S2CID 52856300.
  3. Dubrovinskaia, Natalia; Dubrovinsky, Leonid; Crichton, Wilson; Langenhorst, Falko; Richter, Asta (2005). "Aggregated diamond nanorods, the densest and least compressible form of carbon". Applied Physics Letters. 87 (8): 083106. Bibcode:2005ApPhL..87h3106D. doi:10.1063/1.2034101.
  4. Dubrovinskaia, Natalia; Dub, Sergey; Dubrovinsky, Leonid (2006). "Superior Wear Resistance of Aggregated Diamond Nanorods". Nano Letters. 6 (4): 824–6. Bibcode:2006NanoL...6..824D. doi:10.1021/nl0602084. PMID 16608291.
  5. Blank, V (1998). "Ultrahard and superhard phases of fullerite C60: Comparison with diamond on hardness and wear" (PDF). Diamond and Related Materials. 7 (2–5): 427–431. Bibcode:1998DRM.....7..427B. CiteSeerX 10.1.1.520.7265. doi:10.1016/S0925-9635(97)00232-X. Archived from the original (PDF) on 2011-07-21.
  6. Blank, V; Popov, M; Buga, S; Davydov, V; Denisov, V; Ivlev, A; Marvin, B; Agafonov, V; et al. (1994). "Is C60 fullerite harder than diamond?". Physics Letters A. 188 (3): 281. Bibcode:1994PhLA..188..281B. doi:10.1016/0375-9601(94)90451-0.
  7. Kozlov, M (1995). "Superhard form of carbon obtained from C60 at moderate pressure". Synthetic Metals. 70 (1–3): 1411–1412. doi:10.1016/0379-6779(94)02900-J.
  8. Blank, V (1995). "Ultrahard and superhard carbon phases produced from C60 by heating at high pressure: structural and Raman studies". Physics Letters A. 205 (2–3): 208–216. Bibcode:1995PhLA..205..208B. doi:10.1016/0375-9601(95)00564-J.
  9. Szwarc, H; Davydov, V; Plotianskaya, S; Kashevarova, L; Agafonov, V; Ceolin, R (1996). "Chemical modifications of C under the influence of pressure and temperature: from cubic C to diamond". Synthetic Metals. 77 (1–3): 265–272. doi:10.1016/0379-6779(96)80100-7.
  10. Blank, V (1996). "Phase transformations in solid C60 at high-pressure-high-temperature treatment and the structure of 3D polymerized fullerites". Physics Letters A. 220 (1–3): 149–157. Bibcode:1996PhLA..220..149B. doi:10.1016/0375-9601(96)00483-5.
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