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A New Carbon Allotrope with Six-Fold Helical Chains in all-sp2 Bonding Networks

Abstract

Using a recently developed approach to constructing covalent network structures from linear carbyne, we identify by ab initio calculations a new carbon allotrope in () symmetry that comprises six-fold helical chains with alternating sp2-type single and double bonds along the chains that are connected via zigzag benzene rings. This 6-fold carbene is characterized as a three-dimensional three-connected chiral crystalline modification of graphite. Phonon and electronic band calculations indicate that this new structure is dynamically stable and is a semiconductor with a band gap of 0.47 eV, in contrast to the semimetallic nature of graphite. Simulated x-ray diffraction patterns of the 6-fold carbene provide an excellent match to the previously unexplained distinct diffraction peak of a new carbon allotrope found in recent detonation experiments. These results establish a new carbon phase and offer insights into its outstanding structural and electronic properties.

Introduction

Carbon's extremely versatile bonding ability produces a rich variety of structural allotropes, among which graphite and diamond have long been known for their outstanding properties. All carbon atoms in graphite are connected via the sp2 hybridization bonding with a bond length of 0.142 nm and bond angle of 120° and the graphite honeycomb lattice can be viewed as a planar molecule comprising benzene rings or 2-fold polyacetylene-like zigzag chains1. The strong in-plane aromatic π-conjugation makes the two-dimensional three-connected (2D3C) graphite the most stable allotropic form of carbon. In a diamond single crystal, all carbon atoms are connected via the sp3 hybridization bonding with the tetrahedral bond angle of 109.47° and a bond length of 0.154 nm. The average distance between its parallel planes is 0.140 nm, which is much smaller than that in graphite. Single crystal diamond has a dense 3D4C structure comprising four nearest-neighbor polyacetylene-like zigzag chains or two nearest-neighbor twisted graphite layers2. Under static pressure, the highly crystalline varieties of graphite can be transformed to diamond via slipping, buckling and cross-linking of the carbon sheets3,4,5,6,7,8,9 with an sp2sp3 bonding transition. During the last two or three decades, tremendous attention has been focused on synthesizing a variety of new carbon allotropes, including 0D3C fullerenes10, 1D3C nanotubes11 and 2D3C graphene12 in all-sp2 networks. Novel fullerene structures have been discovered in natural coal13, rock14 and detonation soot15.

In addition to these well characterized carbon allotropes, there exist a number of proposed and synthesized carbon structures that require further exploration. Recently, we identified two 3D3C chiral framework structures in all-sp2 bonding networks comprising 3-fold and 4-fold helical chains connected by ethene-type (H2C = CH2) π-conjugation16. These structures contain matching helical chains of complementary chirality with ethene-type planar π-conjugation and they are energetically more favorable than previously proposed structures with helical chains of same chirality (e.g., K417) or zigzag chains (e.g., H-618 and bct-419) with twisted π bonds. This finding suggests a new approach to constructing covalent network structures. In particular, the matching helical chain configuration offers a new strategy for solving structures of yet unidentified carbon phases seen in recent experiments, including carbon blacks, soot, or similar materials20,21,22,23,24,25,26,27,28,29,30.

Here we report by ab initio total-energy and phonon calculations31,32,33,34,35 a new type of 3D3C crystalline carbon in an all-sp2 network that comprises 6-fold helical carbon chains with alternating single and double bonds, which are distinct from the polyyne-like alternating single and triple carbon-carbon bonds in linear sp-carbyne36. This structure can be regarded as twisted graphite in AA stacking consisting of zigzag hexagonal benzene rings connected by an ethene-type planar π-conjugation like as in the 3-fold and 4-fold carbene16. Phonon and electronic band calculations show that this new carbon phase is dynamically stable and is a semiconductor with a band gap of 0.47 eV, in contrast to the semimetallic nature of graphite. Simulated x-ray diffraction (XRD) patterns show an excellent match between this newly identified carbon structure and the condensed carbon phase discovered in detonation soot28,29,30. These results establish a new carbon phase and offer insights into its outstanding structural and electronic properties.

Results

We first present structural characterization of the new carbon phase, which has a 6-atom rhombohedral primitive unit cell with equilibrium lattice parameters a = 4.1491 Å, α = 112.55°, occupying the 6 h (0.4381, 0.7965, 0.4381) position, thus termed rh6 carbon (or 6-fold carbene). In hexagonal representation, it has an 18 atom hexagonal unit cell (see Fig. 1a and 1b) with lattice parameters a = 6.902 Å, c = 3.470 Å, occupying the 18 h (0.8805, 0.1195, 0.5576) position. It has a polymerized carbyne-like structure containing three 6-fold helical carbon chains; however, instead of having the polyyne-like alternating sp-type single and triple carbon-carbon bonds as those in linear carbyne36, the right-handed (or left-handed) helical chains in rh6 carbon have an alternating sp2-type single and double carbon-carbon bonds (see Fig. 1a). The spsp2 bonding state transition produces a large energy gain of about 0.46 eV per carbon atom (see Fig. 2a). Meanwhile, three right-handed (or left-handed) helical carbon chains bond together forming a zigzag benzene ring. Therefore, rh6 carbon also can be regarded as a twisted graphite in AA stacking consisting of three zigzag hexagonal carbon rings with a (3 × 3 × 1) superlattice of graphite (see Fig. 1c). However, in contrast to the uniform bond length of 1.42 Å in graphite, there are two distinct carbon-carbon bond lengths, a longer bond of 1.483 Å associated with a C(sp2)–C(sp2) single bond in the zigzag benzene rings and a shorter bond of 1.359 Å associated with an ethene-type C(sp2) = C(sp2) double bond16 between the zigzag benzene rings (these bonds are different from that in 3-fold and 4-fold carbene with single bonds along the chains and double bonds between the carbon chains16). Also, there are two different bond angles, 113.45° for in the zigzag benzene rings and 123.16° for out of the zigzag benzene rings. These structural parameters on average are similar to those in graphite, but they are closer to those in 3-fold and 4-fold carbene16, thus rh6 carbon can also be considered a 6-fold chiral carbene.

Figure 1
figure 1

Chiral crystalline modification of carbon in an all-sp2 3D3C bonding network in () symmetry.

Top (a) and side (b) view of rh6 carbon, which comprises three 6- fold helices or three zigzag benzene rings as its building blocks. In hexagonal representation its lattice parameters are a = 6.902 Å, c = 3.470 Å and carbon atoms occupy the 18 h (0.8805, 0.1195, 0.5576) position. Symbols R and 6 represent right-handed helices and closed hexagon, respectively. It topologically corresponds to a (3 × 3 × 1) superlattice of graphite in AA stacking as shown in (c).

Figure 2
figure 2

Energetics and kinetics of selected carbon structures.

(a) Energy versus volume for K4, H-6, bct-4, cR6, cT8 and rh6 in 3D3C bonding networks compared to those of 1D2C carbyne, 2D3C graphite and 3D4C diamond. The energies for fcc C60 fullerene and (5,5) carbon nanotube are also shown for comparison. (b) Enthalpy per atom (relative to that of graphite) for rh6, rh6-II and diamond versus pressure. The insert picture is rh6-II structure.

We have calculated the total energy of rh6 carbon as a function of volume (see Fig. 2a) in comparison with the results for diamond and several other carbon structures that are all in an all-sp2 bonding environment, including K417, H-618, bct-419, cR616, cT816 and graphite. The energies for fcc C60 fullerene37 and (5,5) carbon nanotube are also shown for comparison. Graphite has all its 2pz orbitals perfectly aligned, leading to a strong aromatic π bonding interaction between neighboring carbon atoms, which makes it the most stable carbon crystal. Conversely, all the 2pz orbitals are misaligned in the K4 carbon, making it the most unfavorable crystalline carbon form16. Meanwhile, rh6 carbon has one-third of its bonds with well-aligned 2pz orbitals between the zigzag benzene rings and, as a result, it is less stable than diamond, graphite, C60 fullerene and (5,5) nanotube, but is almost as stable as the 4-fold cT8 carbene and more favorable than 3-fold cR6 carbene with the same symmetry.

It should be noted that there is a dense form of rh6 (named rh6-II as shown in Fig. 2) with lattice parameters a = 7.012 Å, c = 2.509 Å, occupying the 18 h (0.7495, 0.1252, 0.4582) position. The rh6-II phase can be obtained from rh6 phase via local bond rotation (Fig. S1 in Supplementary Information) and stabilized under pressure above 12 GPa (see Fig. 2b). It is even more stable than graphite above 70 GPa due to the sp3-like bonding nature in rh6-II state. However, this structural transformation rh6 → rh6-II is reversible (Fig. S2 in Supplementary Information) and upon decompression rh6 phase is recovered. The calculated equilibrium structural parameters, total energy, bulk modulus and electronic band gap for rh6, rh6-II, cR6 and cT8 are listed in Table I, compared to available experimental data38.

Table 1 Calculated equilibrium structural parameters (space group, volume V0, lattice parameters a and c, bond lengths dCC), total energy Etot, bulk modulus B0 and electronic band gap Eg for cR6 carbon, cT8 carbon, rh6 carbon, graphite and diamond at zero pressure, compared to available experimental data38

To understand the mechanical stability of rh6 carbon, the corresponding elastic constants C11, C33, C44, C12 and C13 are estimated to be 630, 90, 128, 288 and 139 GPa, respectively. It clearly meets the mechanical stability criteria given by C44 > 0, C11 > |C12| and for hexagonal phase39. We further examined dynamic stability of rh6 carbon by calculating the phonon dispersion curves. No imaginary frequencies were observed throughout the entire Brillioun zone (results at 0 GPa are shown in Fig. 3a), confirming the dynamic stability of rh6 carbon. The highest phonon frequency 1611 cm−1 for rh6 carbon is almost equal to the highest phonon frequency of 1610 cm−1 for graphite40, which reflects the graphite-like structural bonding character of rh6 carbon.

Figure 3
figure 3

Phonon and electronic band structures.

(a) Calculated phonon band structure of rh6 carbon at zero GPa. (b) Calculated electronic band structure of rh6 carbon at zero GPa.

The increased bonding connectivity in the 3D3C rh6 carbon is expected to open an electronic band gap in contrast to the semimetallic state in the 2D3C graphite structure. A hybrid density functional method based on the Heyd-Scuseria-Ernzerhof scheme (HSE06)34 has been used to calculate electronic properties. It is seen that the calculated HSE06 band gap (5.36 eV) for diamond is very close to the experimental data38 of 5.47 eV, suggesting the validity of HSE06 method in predicting band gaps for diamond. Our calculated electronic band structure of rh6 carbon (see Fig. 3b) indeed shows a band gap of 0.47 eV with the conduction band bottom and valence band top located along the Γ-A and A-H direction, respectively. This moderate band gap makes rh6 carbon highly desirable for a wide range of applications in electronic, optical and energy conversion devices.

We now establish the experimental connection of rh6 carbon. Several experiments in recent years have discovered a new carbon structure in detonation soot or similar materials20,21,22,23,24,25,26,27,28,29,30, but have not been able to identify its structural features that hold the key to further understanding and exploration of this new carbon phase. Experimental x-ray diffraction (XRD) of a TNT/dissel oil detonation soot28 (see Fig. 4b) revealed the presence of a considerable amount of amorphous carbon and several crystalline phases: the strongest peak around 26° comes from the graphite (002) diffraction; a weak peak around 43.6° is attributed to the diamond (111) diffraction; a prominent sharp diffraction peak at 30°, however, cannot be assigned to any known carbon phase such as graphite, diamond or fullerenes25,26,27. A similar sharp diffraction peak at 30° was also found in the chimney soot29 and the trinitrotoluene/cyclomethylenetrinitramine detonation nanoparticles30. The high intensity and sharpness of this unexplained XRD peak suggests that a new carbon phase has been consistently produced in these experiments. In Fig. 4a, we show simulated XRD patterns for graphite, diamond, rh6 carbon, cT8, cR6, H-6, bct-4, K4 and fcc C60 described in Fig. 2a and compare with the experimental XRD pattern28 (see Fig. 4b). Our simulated XRD patterns for graphite and diamond are consistent with the corresponding experimental XRD peaks. Most importantly, the main peak for rh6 carbon matches almost perfectly the XRD peak at 30° for the newly identified carbon phase. Beside of rh6 carbon, it is shown that the main peak of 30.8° for K4 carbon is also close to 30°; however, the K4 carbon is dynamically unstable41. These results suggest that the new rh6 carbon is among the likely candidates for the unidentified carbon phases found in recent detonation experiments28.

Figure 4
figure 4

X-ray diffraction (XRD) patterns.

(a) Simulated XRD patterns for graphite, diamond, rh6 carbon and the other structures cT8, cR6, H-6, bct-4, K4 and fcc C60. (b) Experimental XRD patterns for TNT/diesel oil detonation soot28. X-ray wavelength is 1.5406 Å with a copper source.

It is well-known that Raman spectroscopy is also an appropriate method to study the characteristics of new phases of carbon. To provide more information and characters for possible experimental observation, we also simulated the Raman spectra of rh6 carbon and compared the results with different sp2 carbon structures (see Fig. S3 in Supplementary Information). We find that the Raman spectrum of rh6 carbon presents a main peak A1g at 1605 cm−1 and a weaker shoulder peak Eg at 1580 cm−1 instead of the E2g mode at 1585 cm−1 in graphite42. These features may be helpful for identifying the new carbon phases in experiments43.

Discussion

In summary, we have identified a new type of 3D3C crystalline carbon in an all-sp2 network in () symmetry. It consists of three 6-fold carbon helices connected by three zigzag hexagonal carbon rings in hexagonal representation and can be regarded as a chiral crystalline modification of graphite. Phonon and electronic band calculations indicate that this new carbon phase is dynamically stable and is a semiconductor with a band gap of 0.47 eV. Simulated XRD patterns provide an excellent match between this rh6 carbon phase and the previously unexplained carbon structure discovered in recent detonation experiments28,29,30. These results suggest that the possible presence of rh6 phase in soot carbon as well as the ultrafine diamond, graphite and amorphous28.

Recently, a one-step, gas-phase, catalyst-free detonation of hydrocarbon (C2H2) method was developed to produce gram quantities of pristine graphene nanosheets44. It suggests an effective approach to synthesizing rh6 carbon via thermal decomposition or detonation of carbonaceous materials such as aromatic and polymeric hydrocarbon molecules. Successful production of rh6 carbon in large quantity is expected to lead to greatly increased research interest and activity, a situation reminiscent of the early days of the discovery and ensuing study of fullerenes.

Methods

Calculations were carried out using the density functional theory as implemented in the Vienna ab initio simulation package (VASP)31. The generalized gradient approximation (GGA) developed by Armiento-Mattsson (AM05)32 were adopted for the exchange-correlation potential. The all-electron projector augmented wave (PAW) method33 was adopted with 2s22p2 treated as valence electrons. A plane-wave basis set with a large energy cutoff of 800 eV was used. Forces on the ions are calculated through the Hellmann-Feynman theorem allowing a full geometry optimization. The energy minimization is done over the atomic and electronic degrees of freedom using the conjugate gradient iterative technique. Convergence criteria employed for both the electronic self-consistent relaxation and the ionic relaxation were set to 10−8 eV and 0.01 eV/Å for energy and force, respectively. A hybrid density functional method based on the Heyd-Scuseria-Ernzerhof scheme (HSE06)34 has been used to calculate electronic properties. Phonon dispersion curves and Raman spectrum are calculated using the package MedeA35 with the forces calculated from VASP. The phase conversion barrier was calculated using a generalized solid-state nudged elastic band method45,46 with the cell and atomic position optimization.

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Acknowledgements

This study was supported by the NSFC of China (Grants Nos. 11274356, 11274012 and 91021007), the Ministry of Environmental Protection of China (Grant No. 201109037) and CAS (Grant No. KJCX2-YW-W22). C.F.C. acknowledges support by DOE under Cooperative Agreement DENA0001982. Y.K. acknowledges support by the CREST project headed by Professor M. Kotani. We are thankful to the crew of the Center for Computational Materials Science at IMR, Tohoku University for their support at the SR16000 supercomputing facilities.

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J.T.W., C.F.C. and E.G.W. designed the study and wrote the paper; J.T.W. and Y.K. carried out ab initio simulations; all authors discussed the results and contributed to the manuscript.

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Wang, JT., Chen, C., Wang, E. et al. A New Carbon Allotrope with Six-Fold Helical Chains in all-sp2 Bonding Networks. Sci Rep 4, 4339 (2014). https://doi.org/10.1038/srep04339

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