2018
DOI: 10.1016/j.carbon.2017.10.069
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Protomene: A new carbon allotrope

Abstract: We introduce a new carbon allotrope named protomene. Its crystal structure is hexagonal, with a fully-relaxed primitive cell involving 48 atoms. Of these, 12 atoms have the potential to switch hybridization between sp 2 and sp 3 , forming dimers. By means of DFT simulations, we have identified the equilibrium structure of protomene, and estimate that it is 2% less bound than diamond. We have also estimated the amplitude of its direct band gap to be 3 eV, and predicted the X-ray diffraction pattern and phonon m… Show more

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Cited by 34 publications
(20 citation statements)
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“…The groundbreaking results achieved on graphene in the last decade have stimulated the interest in novel carbon allotropes and nanostructures [1,2,3,4,5]. Amongst all, the infinite carbon monoatomic wire, i.e., carbyne, represents a carbon allotrope based on sp1 hybridization, which joins graphite and diamond based on sp2 and sp3 hybridization, respectively [6].…”
Section: Introductionmentioning
confidence: 99%
“…The groundbreaking results achieved on graphene in the last decade have stimulated the interest in novel carbon allotropes and nanostructures [1,2,3,4,5]. Amongst all, the infinite carbon monoatomic wire, i.e., carbyne, represents a carbon allotrope based on sp1 hybridization, which joins graphite and diamond based on sp2 and sp3 hybridization, respectively [6].…”
Section: Introductionmentioning
confidence: 99%
“…Luminescence spectra in the region of 350-1150 nm with a resolution of 1.5 nm were recorded by a scanning CCD array spectrograph (QE 65000 OCEAN OPTICS), also controlled by P.C. The temperature of a finely dispersed sample deposited from an alcohol suspension in the form of a thin layer (һ ≤ 100 μm) on a heater substrate could be kept constant with an accuracy of ≤1% or quickly (<10 s) be changed using an electronic controller with the heater current (Delodovici et al, 2017). Atomic oxygen with a flux density of up to j O = 10 14 cm -2 s -1 was obtained by O 2 thermolysis according to the procedure (Brennan, 1967) on a current-heated rhodium (Rh) ribbon measuring 0.015120 mm.…”
Section: Methodsmentioning
confidence: 99%
“…To obtain the equilibrium conguration and electronic properties of nanoleite, the well-established density functional theory (DFT) is employed. [9][10][11][12][13][14][20][21][22][23][24] Density functionals including the general gradient approximation (GGA) 25 and hybrid functional (HSE06) are used in the Perdew-Burke-Ernzerhof (PBE) formulation, 26 with the norm-conserving PseudoDojo 27 pseudopotential as implemented in the quantum simulation package QuantumATK. 28 The wave functions are expanded on a plain-waves basis with a wave function cut-off of 35 hartree for both of GGA and HSE06, which guarantees the convergence of the total energy of nanoleite structure within 10 À5 hartree.…”
Section: Structure Propertiesmentioning
confidence: 99%
“…Zero-dimensional fullerene, 1 one-dimensional carbon nanotubes (CNTs), 2 and two-dimensional graphene 3 are some of the most common and widely studied allotropic forms of carbon, and have found applications in solar cells, eld-effect transistors, sensors, electromagnetic interference shielding, batteries and supercapacitors. [4][5][6][7][8] Other emerging forms of carbon allotropes, such as D-carbon, 9 T-carbon, 10 penta-graphene, 11 protomene, 12 novamene, 13 and zayedene 14 have been predicted by theorists and some have been conrmed by the experimentalists. Some of the reported carbon allotropes have extraordinary properties, such as ultra-high hardness, 15 direct bandgap, 10 ferromagnetic, 16 and so on, which makes them highly prominent for various applications.…”
Section: Introductionmentioning
confidence: 99%