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Graphyne-n varieties, where n indicates the number of carbon-carbon triple bonds in a link between two adjacent hexagons. Graphyne is graphyne-1; graphdiyne is graphyne-2.

Graphyne is an allotrope of carbon. Its structure is one-atom-thick planar sheets of sp and sp2-bonded carbon atoms arranged in crystal lattice. It can be seen as a lattice of benzene rings connected by acetylene bonds. Depending on the content of acetylene groups, graphyne can be considered a mixed hybridization, spn, where 1 < n < 2,[1][2] and thus differs from the hybridization of graphene (considered pure sp2) and diamond (pure sp3).

The existence of graphyne was conjectured before 1960,[3] and attracted attention after the discovery of fullerenes.

Although not yet synthesized, periodic graphyne structures and their boron nitride analogues were shown to be stable on the basis of first-principles calculations using phonon dispersion curves and ab-initio finite temperature, quantum mechanical molecular dynamics simulations.[4]


Graphyne has yet to be synthesized in significant quantities for study but through the use of computer models scientists have been able to predict several properties of the substance on assumed geometries of the lattice. The proposed structures of graphyne are derived from inserting acetylene bonds in place of carbon-carbon single bonds in a graphene lattice.[5] Graphyne is theorized to exist in several different geometries. This variety is due to the multiple arrangements of sp and sp2 hybridized carbon. The proposed geometries include a hexagonal lattice structure and a rectangular lattice structure.[6] It has been hypothesized as preferable to graphene for specific applications due to the potential of direction-dependent Dirac cones.[7][8] Out of the theorized structures the rectangular lattice of 6,6,12-graphyne may hold the most potential for future applications.


The models for graphyne show that it has the potential for Dirac cones on its double and triple bonded carbon atoms. Due to the Dirac cones, there is a single point in the Fermi level where the conduction and valence bands meet in a linear fashion. The advantage of this scheme is that electrons behave as if they have no mass, resulting in energies that are proportional to the momentum of the electrons. Like in graphene, hexagonal graphyne has electric properties that are direction independent. However, due to the symmetry of the proposed rectangular 6,6,12-graphyne the electric properties would change along different directions in the plane of the material.[6] This unique feature of its symmetry allows graphyne to self-dope meaning that it has two different Dirac cones lying slightly above and below the Fermi level.[6] The self-doping effect of 6,6,12-graphyne can be effectively tuned by applying in-plane external strain.[9] Graphyne samples synthesized to date have shown a melting point of 250-300 °C, low reactivity in decomposition reactions with oxygen, heat and light.[5]

Potential applications[edit]

The directional dependency of 6,6,12-graphyne could allow for electrical grating on the nanoscale.[10] This could lead to the development of faster transistors and nanoscale electronic devices.[6][11][12]


The synthesis of graphdiyne was reported as a 1 mm film on a copper surface.[13] Graphdiyne was predicted to exhibit a nanoweb-like structure, characterized by triangular and regularly distributed pores, thus forming a nanoporous membrane. Due to the effective size of its pores, which almost matches the van der Waals radius of the helium atom, graphdiyne could behave as an ideal two-dimensional membrane for helium chemical and isotopic separation.[14] The application of a graphdiyne based membrane as an efficient two-dimensional sieve for water filtration and purification technologies has been proposed.[15]


  1. ^ Heimann, R.B.; Evsvukov, S.E.; Koga, Y. (1997). "Carbon allotropes: a suggested classification scheme based on valence orbital hybridization". Carbon. 35 (10–11): 1654–1658. doi:10.1016/S0008-6223(97)82794-7.
  2. ^ Enyashin, Andrey N.; Ivanovskii, Alexander L. (2011). "Graphene Allotropes". Physica Status Solidi B. 248 (8): 1879–1883. Bibcode:2011PSSBR.248.1879E. doi:10.1002/pssb.201046583.
  3. ^ Balaban, AT; Rentia, CC; Ciupitu, E. (1968). Rev. Roum. Chim. 13: 231
  4. ^ Özçelik, V. Ongun; Ciraci, S. (January 10, 2013). "Size Dependence in the Stabilities and Electronic Properties of α-Graphyne and Its Boron Nitride Analogue". The Journal of Physical Chemistry C. 117 (5): 2175–2182. arXiv:1301.2593. doi:10.1021/jp3111869.
  5. ^ a b Kim, Bog G.; Choi, Hyoung Joon (2012). "Graphyne: Hexagonal network of carbon with versatile Dirac cones". Physical Review B. 86 (11): 115435. arXiv:1112.2932. Bibcode:2012PhRvB..86k5435K. doi:10.1103/PhysRevB.86.115435.
  6. ^ a b c d Dumé, Belle (1 March 2012). "Could graphynes be better than graphene?". Physics World. Institute of Physics.
  7. ^ Malko, Daniel; Neiss, Christian; Viñes, Francesc; Görling, Andreas (24 February 2012). "Competition for Graphene: Graphynes with Direction-Dependent Dirac Cones" (PDF). Phys. Rev. Lett. 108 (8): 086804. Bibcode:2012PhRvL.108h6804M. doi:10.1103/PhysRevLett.108.086804. hdl:2445/65316. PMID 22463556.
  8. ^ Schirber, Michael (24 February 2012). "Focus: Graphyne May Be Better than Graphene". Physics. 5 (24): 24. Bibcode:2012PhyOJ...5...24S. doi:10.1103/Physics.5.24.
  9. ^ Wang, Gaoxue; Si, Mingsu; Kumar, Ashok; Pandey, Ravindra (May 26, 2014). "Strain engineering of Dirac cones in graphyne". Applied Physics Letters. 104 (21): 213107. Bibcode:2014ApPhL.104u3107W. doi:10.1063/1.4880635.
  10. ^ Bardhan, Debjyoti (2 March 2012). "Novel new material graphyne can be a serious competitor to graphene".
  11. ^ Cartwright, J. (1 March 2012). "Graphyne could be better than graphene". Archived from the original on 2 October 2012.
  12. ^ "Graphyne Better Than Graphene?". Materials Today. 5 March 2012.
  13. ^ Li, Guoxing; Li, Yuliang; Liu, Huibiao; Guo, Yanbing; Li, Yongjun; Zhu, Daoben (2010). "Architecture of graphdiyne nanoscale films". Chemical Communications. 46 (19): 3256–3258. doi:10.1039/B922733D. PMID 20442882.
  14. ^ Bartolomei, Massimiliano; Carmona-Novillo, Estela; Hernández, Marta I.; Campos-Martínez, José; Pirani, Fernando; Giorgi, Giacomo (2014). "Graphdiyne Pores: "Ad Hoc" Openings for Helium Separation Applications". Journal of Physical Chemistry C. 118 (51): 29966–29972. arXiv:1409.4286. doi:10.1021/jp510124e.
  15. ^ Bartolomei, Massimiliano; Carmona-Novillo, Estela; Hernández, Marta I.; Campos-Martínez, José; Pirani, Fernando; Giorgi, Giacomo; Yamashita, Koichi (2014). "Penetration Barrier of Water through Graphynes' Pores: First-Principles Predictions and Force Field Optimization". Journal of Physical Chemistry Letters. 5 (4): 751–755. arXiv:1312.3179. doi:10.1021/jz4026563.