Prediction of an ultrasoft graphene allotrope with Dirac cones
Source abstract
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 ↗