journal article·2016-08

Prediction of an ultrasoft graphene allotrope with Dirac cones

Xiaoming Zhang, Lin Wei, Jie Tan, Mingwen Zhao

Carbon· Volume 105
Publisher page

Abstract

Abstract Searching for the Dirac materials with ultrasoftness is crucial for flexible electronics applications. Based on first-principles calculations, we propose a new carbon allotrope (named as ph-graphene) with a penta-hexagonal framework, which is energetically more favorable than the penta-graphene composing surely of pentagons and some of already-synthesized carbon allotropes. Ph-graphene has an in-plane stiffness of 27.75 GPa·nm, smaller than those of graphene and penta-graphene by one order. The famous isotropic Dirac cones are well preserved in the ultrasoft ph-graphene, exhibiting delocalized feature of p z orbits with the Fermi velocity of 2.8 × 10 5 m/s. Additionally, surface hydrogenation alters drastically the electronic and mechanical properties of ph-graphene, resulting in electronic spin-polarization and anisotropic negative Poisson’s ratios sequentially with the increase of hydrogenation concentrations.
Source: openaire · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Graphene research and applications · Graphene and Nanomaterials Applications · 2D Materials and Applications

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (65)

Show source-provided references
1. Complex evolution of the electronic structure from polycrystalline to monocrystalline graphene: generation of a new Dirac point10.1103/PhysRevB.81.073408 ↗
2. The rise of graphene10.1038/nmat1849 ↗
3. The electronic properties of graphene10.1103/RevModPhys.81.109 ↗
4. The band theory of graphite10.1103/PhysRev.71.622 ↗
5. Electric field effect in atomically thin carbon films10.1126/science.1102896 ↗
6. Creation of graphene allotropes using patterned defects10.1016/j.carbon.2009.04.014 ↗
7. Point defects and self-diffusion in graphite10.1002/pssa.2210470102 ↗
8. Theoretical studies of icosahedral C60 and some related species10.1016/0009-2614(86)80661-3 ↗
9. Graphene nanoengineering and the inverse Stone-Thrower-Wales defect10.1103/PhysRevB.81.155444 ↗
10. Nanoengineering defect structures on graphene10.1103/PhysRevLett.100.175503 ↗
11. Prediction of a pure-carbon planar covalent metal10.1103/PhysRevB.53.R13303 ↗
12. New metallic allotropes of planar and tubular carbon10.1103/PhysRevLett.84.1716 ↗
13. Gap opening in topological-defect lattices in graphene10.1103/PhysRevB.81.193405 ↗
14. Two-dimensional carbon semiconductor: density functional theory calculations10.1103/PhysRevB.82.073410 ↗
15. Gate-induced insulating state in bilayer graphene devices10.1038/nmat2082 ↗
16. Phagraphene: a low-energy graphene allotrope composed of 5-6-7 carbon rings with distorted dirac cones10.1021/acs.nanolett.5b02512 ↗
17. Structure-property predictions for new planar forms of carbon: layered phases containing sp2 and sp atoms10.1063/1.453405 ↗
18. Carbon scaffolding: building acetylenic all-carbon and carbon-rich compounds10.1038/369199a0 ↗
19. Synthesis and properties of annulenic subunits of graphyne and graphdiyne nanoarchitectures10.1351/pac200880030519 ↗
20. Optimized geometries and electronic structures of graphyne and its family10.1103/PhysRevB.58.11009 ↗
21. Competition for graphene: graphynes with direction-dependent Dirac cones10.1103/PhysRevLett.108.086804 ↗
22. Graphene allotropes10.1002/pssb.201046583 ↗
23. Tunable thermal conductivity in carbon allotrope sheets: role of acetylenic linkages10.1063/1.4936111 ↗
24. Highly anisotropic dirac fermions in square graphynes10.1021/acs.jpclett.5b01337 ↗
25. Ab initio vibrational and thermal properties of carbon allotropes: polycyclic and rectangular networks10.1016/j.commatsci.2015.07.007 ↗
26. Penta-graphene: a new carbon allotrope10.1073/pnas.1416591112 ↗
27. Translation symmetry breakdown in low-dimensional lattices of pentagonal rings10.1021/acs.jpclett.5b02309 ↗
28. Electronic and optical properties of novel carbon allotropes10.1016/j.carbon.2016.01.078 ↗
29. Thermal conductivity of penta-graphene from molecular dynamics study10.1063/1.4933311 ↗
30. Hydrogen-induced stabilization and tunable electronic structures of penta-silicene: a computational study10.1039/C5TC02504D ↗
31. Stable Si-based pentagonal monolayers: high carrier mobilities and applications in photocatalytic water splitting10.1039/C5TA05770A ↗
32. σ-π-Band inversion in a novel two-dimensional material10.1021/acs.jpcc.5b04726 ↗
33. Flexible structural and electronic properties of a pentagonal B2C monolayer via external strain: a computational investigation10.1039/C5CP03885E ↗
34. Pentagonal monolayer crystals of carbon, boron nitride, and silver azide10.1063/1.4930086 ↗
35. Two-dimensional pentagonal crystals and possible spin-polarized Dirac dispersion relations10.1063/1.4868679 ↗
36. When is 6 less than 5? Penta- to hexa-graphene transition10.1016/j.carbon.2015.09.092 ↗
37. C36, a new carbon solid10.1038/31668 ↗
38. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set10.1103/PhysRevB.54.11169 ↗
39. Ab initio molecular dynamics for open-shell transition metals10.1103/PhysRevB.48.13115 ↗
40. Generalized gradient approximation made simple10.1103/PhysRevLett.77.3865 ↗
41. From ultrasoft pseudopotentials to the projector augmented-wave method10.1103/PhysRevB.59.1758 ↗
42. First-principles calculations of the ferroelastic transition between rutile-type and CaCl2-type SiO2 at high pressures10.1103/PhysRevB.78.134106 ↗
43. Structure and stability of solid C3610.1103/PhysRevB.60.13322 ↗
44. Solid C36 as hexaclathrate form of carbon10.1103/PhysRevB.62.15420 ↗
45. Fullerenes: C60’s smallest cousin10.1038/31579 ↗
46. Scanning tunneling spectroscopy of C3610.1103/PhysRevLett.82.165 ↗
47. Electron-phonon interactions in solid C3610.1103/PhysRevLett.81.697 ↗
48. Stabilities and electronic properties of two-dimensional C36 crystals10.1021/jp013623n ↗
49. Growth of C36-films on diamond surface through molecular dynamics simulation10.1142/S021797920201467X ↗
50. Two-dimensional nanocrystals produced by exfoliation of Ti3AlC210.1002/adma.201102306 ↗
51. Exfoliation of hexagonal boron nitride by molten hydroxides10.1002/adma.201204031 ↗
52. Two-dimensional carbon topological insulators superior to graphene10.1038/srep03532 ↗
53. Production of defects in supported carbon nanotubes under ion irradiation10.1103/PhysRevB.65.165423 ↗
54. Electron irradiation effects in single wall carbon nanotubes10.1063/1.1383020 ↗
55. Reversible defect engineering of single-walled carbon nanotubes using scanning tunneling microscopy10.1021/nl071845c ↗
56. Two-dimensional topological insulators with binary honeycomb lattices: SiC3 siligraphene and its analogs10.1103/PhysRevB.89.195427 ↗
57. Monolayer honeycomb structures of group-IV elements and III-V binary compounds: first-principles calculations10.1103/PhysRevB.80.155453 ↗
58. The response of mechanical and electronic properties of graphane to the elastic strain10.1063/1.3353968 ↗
59. Strain-induced phase transition and electron spin-polarization in graphene spirals10.1038/srep05699 ↗
60. Electronic strengthening of graphene by charge doping10.1103/PhysRevLett.109.226802 ↗
61. Failure mechanisms of graphene under tension10.1103/PhysRevLett.105.245502 ↗
62. Isoelectronic doping of graphdiyne with boron and nitrogen: stable configurations and band gap modification10.1021/jp300107d ↗
63. Ferromagnetism in semihydrogenated graphene sheet10.1021/nl9020733 ↗
64. Graphane: a two-dimensional hydrocarbon10.1103/PhysRevB.75.153401 ↗
65. Covalent-adsorption induced magnetism in graphene10.1039/b908949g ↗