Formation mechanism of insensitive tellurium hexanitride with armchair-like cyclo-N6 anions

Abstract

The lower decomposition barriers of cyclo-N6 anions hinder their application as high-energy-density materials. Here, first-principles calculations and molecular dynamics simulations reveal that enhancing the covalent component of the interaction between cyclo-N6 anions and cations can effectively improve the stability of cyclo-N6 anions. Taking tellurium hexanitride as a representative, the exotic armchair-like N6 anions of tellurium hexanitride exhibit resistance towards electronic attack and gain extra stability through the formation of covalent bonds with the surrounding elemental tellurium under high pressures. These covalent bonds effectively improve the chemical barrier and insensitivity of tellurium hexanitride during blasting, which prevents the decomposition of solid cyclo-N6 salts into molecular nitrogen. Furthermore, the high-pressure induced covalent bonds between cyclo-N6 anions and tellurium enable the high bulk modulus, remarkable detonation performance, and high-temperature thermodynamic stability of tellurium hexanitride.

Introduction

High pressure, a typically clean and controllable thermodynamic variable, can be adopted to obtain curious materials that are difficult to synthesize under ambient condition1,2,3. Moreover, the precompression evoked by metal elements can reduce the required external pressure for the synthesis of these materials4. Under high pressure, metal nitrides have attractive physical and chemical characteristics, such as good superconductivity, good magnetism, good hardness, and a particular catalytic performance5,6,7,8. Metallic nitrides are conducive to optoelectronic and defect-tolerance characteristics and have strong metal–nitrogen bonds for structural stability and mechanical stiffness9. Particularly, the compression of N-rich nitrides has been recommend as an alternative method to obtain metallic atomic nitrogen states as high-energy density materials since the laser-heated diamond anvil cell, which is a powerful tool, has been used to synthesize a series of stable monatomic forms of solid nitrogen10,11,12,13. Synthesizing pentazolate or π-aromatic ions is considered one of the best and most efficient methods to obtain metallic poly-nitrogen phases14. However, all π-aromatics are incredibly unstable, difficult to synthesize, and sensitive to electrophilic attack, and they mostly appear nonmetallic15.

Many attempts have been made to synthesize pentazolate anion until cyclo-N5, and the first attempt was first reported in 199816. Later, the pentazolate salt in solid (N5)6(H3O)3(NH4)4Cl was reported with a stable thermal decomposition temperature (390 K) via thermogravimetric experiments17,18. Recently, the controllable and synthetic cyclo-N5 ionic salt CsN5 was reported at 60 GPa with a high-energy density and a relatively assessable pressure19. Compressing CsN3 mixed with N2 cryogenic liquid was also used to achieve cyclo-N5 ionic salt according to a synchrotron X-ray diffraction measurement at 55.4 GPa in a diamond anvil cell. A Raman spectral vibration mode unique to the cyclo-N5 anion was observed in LiN5 salt20. Because of the intrinsic stability of N5 anions, their crystals have considerable kinetic stability that may be sufficient for an ambient pressure recovery. Considering their electronic structures, the effective separation of the σ and π electrons that correspond to the highest occupied molecular orbital (MO) and lowest unoccupied MO can help to stabilize cyclo-N5/N5+ salt21. Likewise, the pursuit of energy-intensive cyclo-N6 salts with higher nitrogen contents than pentazolate anions, which are synthesized at a modest pressure, has never ceased22. However, the cyclo-N6 ionic salt only remains in the theoretical stage. Numerous planar or quasi-planar cyclo-N6 anions are predicted at high pressure in Li, Mg, Cs, Ca, Rb, and Ba nitrides, but they have not been successfully synthesized for unclear reasons6,22,23,24,25.

These theoretical studies did not pay close attention to the microstructural characteristics of cyclo-N6 anions. It is of note that an in-plane distortion may occur in cyclo-N6 sub-lattices when the neutral π-aromatic switches to a charged anion. For instance, armchair-like N6 rings are predicted in h-W2.4+N62.4− 26. Once a benzene-like molecule forms a cyclo-N66− anion, its symmetry reduces and even decomposes because its antibonding states are fully occupied, which may prevent experimental synthesis. Another reason may be that the decomposition barrier of cyclo-N6 anions is extremely low and they spontaneously decompose to other anions. We propose a strategy to maintain the “non-molecular nitrogen phase”, i.e., to enhance its energy barrier and insensitivity via covalent bonds entrapment between metal/nonmetal and cyclo-N6 ions to keep it from breaking down into the molecular phase. Based on these judgments, armchair-like cyclo-N6 anions may be able to stabilized if their antibonding MOs are not completely occupied and their structures are entrapped by covalent effects. Considering that Te has higher electronegativity and a larger atomic radius than W, it easily forms covalent bonds with nitrogen; thus, we adopt the binary Te–N candidates as prototypes to search for cyclo-N6 ions and study the trap effect by the covalent bond27,28.

In this work, our broad structure searches combined with first-principles simulations identify a TeN6 nitride with armchair-like cyclo-N6 anions, high-pressure–temperature stability and remarkable mechanical properties. Herein, tellurium serves as an electron donor to modulate the electronic distribution and forms covalent bonds with nitrogen atoms, which induces metallic cyclo-N6 anions. Meanwhile, covalent bond entrapment to stabilize the armchair-like cyclo-N6 anions is revealed. More importantly, the covalent bonds effectively improve the chemical barrier and insensitivity to prevent the decomposition of monatomic forms of solid N6 anions into the molecular phase. Moreover, the detonation performance and energy density of the metallic cyclo-N6 anions predicted by our study are higher than those of most previously reported pentazolate and six-membered N6 anions in binary nitrides.

Results and discussion

Phase stability and structural features at high pressure

A neutral cyclo-N6 molecule with inherent benzene-like structure has planar D6h symmetry29. However, the crystalline sub-lattice N6 isolated anions have D3d symmetry in the anti-CdCl2 TeN6 phase (space group R-3m, Supplementary Tabel 1) because of structural mutations, as shown in Fig. 1a and Supplementary Fig. 1. The armchair-like structural configuration of the equivalent bonding in 3D space hints that the nitrogen atoms adopt sp3 hybridization to form σ covalent bonds. The distance between nitrogen atoms is 1.37 Å at million magnitude pressure, which is a prototypical N–N single bond without the resonance effect between alternating π- and σ-bonds. After removing tellurium atoms from the anti-CdCl2 phase, as shown in Fig. 1b, the cyclo-N6 structure transforms into a flat shape with D6h symmetry but remains in the anti-CdCl2 phase. Compared with the anti-CdCl2-TeN6 phase, the volume of planar cyclo-N6 decreases by 20%, which suggests that the structural deformation of cyclo-N6 is related to the interactions with tellurium atoms. Thus, the N–N bond lengths, Bader charge transfer and volumes as functions of pressure are analyzed to gain insight into the interaction between atoms. The volume decreases by 0.20 Å3/GPa almost linearly with pressure, which indicates strong incompressibility, as shown in Supplementary Fig. 2, while the charge transfer amount gradually increases, as shown in Fig. 1c. However, the change in the N–N distances under high pressure is extremely weak, which preserves N–N single bonds. Herein, the decrease in lattice volume under pressure is mainly attributed to the Te–N distance shrinkage, which increases the interaction and stimulates new physicochemical properties.

Fig. 1: Structural properties and enthalpies of TeN6 under high pressures.
figure1

a Stable structures of the anti-CdCl2 phase at 120 GPa. b Planar cyclo-N6 sub-lattice interacted with Te atoms to form armchair-like N6 anions. c N–N bond lengths and Bader charge transfer as a function of pressure in TeN6. d Enthalpy of the anti-CdCl2 phase relative to the mixture of P3121-Te, TeN or TeN3 and the P41212 nitrogen phases.

The possible routes and pressures for synthesizing anti-CdCl2 phase are summarized and displayed in Fig. 1d. The N–N single bonds endowed TeN6 with superior energy storage properties, which reached 4.79 kJ/g after decomposing into pollution-free nitrogen and the P3121-Te phase. The average N–N displacements of the anti-CdCl2 phase at 500 and 1000 K after the 50 Ps first-principles molecular dynamics (AIMD) simulations shown in Fig. 2a are still 1.37 Å, which suggests that the structural framework remains basically unchanged and thermodynamically stable. The radial distribution function g(r) (Fig. 2b) confirms that the covalent N–N single bonds retained in an isolated peak in cyclo-N6 anions were not broken, and the long-range order naturally persists to crystallize even at temperatures up to 1000 K30. The phonon dispersion calculation demonstrates mechanical stability as shown in Supplementary Fig. 3. The mechanical natures are identified in Supplementary Table 3. Especially, the bulk modulus of the anti-CdCl2 phase is 505 GPa higher than that of diamond 431 GPa31, which implies a larger volume compression resistance and covalent bonds equipment. An evidently high value of C33 (929 GPa) is attached to the crystal, which identifies its remarkable high stiffness along the c-axis. The remarkable mechanical properties enable metallic TeN6 to better resist external force destruction under extreme conditions.

Fig. 2: N–N displacements and radial distribution function.
figure2

a N–N bond lengths as a function of time and b radial distribution function g(r) at 500 and 1000 K under a constant pressure (120 GPa) according to AIMD simulations. The blue arrow denotes the N–N single bond distance according to the previous report.

Electronic structure and bonding properties

Compared with the neutral planar cyclo-N6 sub-lattices in the R-3m-N6 phase, the structural deformation induced by tellurium atoms is subject to the Jahn–Teller effect in the anti-CdCl2 TeN6 phase. A typical symmetry breakage occurs because its geometries with high symmetry produce real or approximate degenerate states. In Fig. 3b, the degeneracy of the p_x and p_y orbits in the R-3m-N6 phase is obvious near the Fermi level. However, along the K-Г, Г-M, M-L, and L-H directions, the corresponding MOs (red lines) are nondegenerated in the anti-CdCl2 TeN6 phase and extend in the direction of lower energy. Then, structural distortion inevitably cause changes in the physical properties. The anti-CdCl2 TeN6 exhibiting metallic property is a sharp contrast to the insulator properties in the R-3m-N6 phase. The dispersion of the N_p orbits increases with the strong interaction with tellurium atoms, and a Van Hove singularity is formed near the Fermi level, as shown in Fig. 3a. The consistency of the Te- and N-p orbital profiles shown in Supplementary Fig. 4 confirms the sp3 hybridization. In general, the nonplanar cyclo-N6 can inhibit the delocalization effect of π electrons, which should be a nonmetallic state32. Thus, tellurium atoms play critical roles in bonding and metallic properties for cyclo-N6 anions except for causing structural deformation. Consequently, we perform Crystal orbital Hamilton population (COHP) quantitative analysis, as shown in Fig. 4a, to identify the role of tellurium atoms in the bonding interaction with cyclo-N6. Intriguingly, the tellurium atom serves as an excellent reductant in ionic crystals and forms an unusual covalent bond with the adjacent cyclo-N6 since the integral COHP (ICOHP) value (N1−Te1a, nearest neighbor distance) reaches −0.64 eV and the sub-adjacent (N1-Te1b, second nearest neighbor distance) is −0.35 eV, which implies an overlap of their electron clouds. Meanwhile, this finding proves that Te atoms (in a formula unit, f.u.) do not completely transfer all the valence electrons (6 e) into the antibonding ψ* (N-p_z) MOs, as shown in Fig. 4b. This result is also confirmed by the Bader charge analysis, which reveals that the charge from one Te atom to one N6 ring is approximately 2.4 e. Then, we analyze the metallization process in detail from the perspectives of cyclo-N6 and Te MOs. The cyclo-N6 unit inherently has six π MOs (P_z) and π electrons: three bonding ψ1-3 and three antibonding ψ*4-6 MOs. Assuming that no electron transfer occurs, three bonding ψ1-3 MOs are occupied, while the higher-energy antibonding MOs ψ4* remains vacant and exhibit nonmetallic properties. Considering the interactions with the Te atoms, each ψ MO produces a scattered π band along Г-A and K-M in the Brillouin region and induces the band overlap and metallic phenomenon. Meanwhile, the Te 5p electron, as shown in Supplementary Fig. 4, is completely delocalized in this phase, so it has a strong influence on the electronic structures of TeN6 except for lowering the Fermi level and plays a relatively significant role in the conducting behavior, which is in strong contrast to Heusler semiconductors33.

Fig. 3: Electronic structure and differential charge density analysis.
figure3

a Electronic band structures and projected density of states (PDOS) with TeN6. b Planar six-membered N6 optimized after removing Te atoms at 120 GPa and its schematic molecular orbital diagram for N atoms. c Differential charge density of TeN6 projected on the (−0.5 0.6 0.7) plane. d Selected high symmetry point and path in the reciprocal lattice space to calculate the energy bands.

Fig. 4: Bonding characteristics under high pressure.
figure4

a Plot of COHP and ICOHP for anti-CdCl2-type TeN6 at 120 GPa. b Simplified correlation diagram of the p_z orbitals of cyclo-N6 and the schematic orbital overlap of N62.4− MOs, which form because of tellurium. c Gradient paths and critical points derived from a QTAIM analysis in the (001) plane. The heavy, dotted, and solid thin lines correspond to the zero, positive, and negative isovalues of Laplacian, respectively. d Electron localization functions in the (001) plane and bonding features marked by the VSEPR notation.

We further investigated the covalent bond effect of cyclo-N6 anions. Through the topological analysis of the coupling electron charge density with Laplacian, the bond critical points (BCPs) derived from a QTAIM34 were adopted to further confirm the bonding behavior, as shown in Fig. 4c. In the (001) plane, the solid isovalues of Laplace for its electron density at BCP are negative, which indicates strong covalent interactions. N atoms connect to the nearest neighbors and form bond paths. The nearest Te and N atoms also have negative isovalues of Laplacian; the actual effect between them is due to polar covalent bonds but not entirely of the closed-shell interaction category35. Each Te covalently bonds with six N6 units, while each N in sp3 hybridization forms three covalent bonds (one Te and two N atoms), which implies that Te can form abundant delocalized chemical bonds. The three-dimensional structure formed by the effective covalent bonds endows metallic TeN6 with higher hardness (HV, 24 GPa), as shown in Supplementary Table 3. Meanwhile, the bonding configuration of cyclo-N6 changes from AX2E2 in isolated N6 ions to AX3E1 (Fig. 4d and Supplementary Fig. 5), which effectively restrains the damage caused by the interactions of nonbonding pairs to the system’s stability36. In addition to the electrostatic interaction between Te2.4+ and N62.4− ions, which reduces the energy by forming strong ionic bonds, the existence of weak covalent bonds leads to the same function since the COHP integral of Te–N leads to a drop of approximately −1 eV/f.u. of the MO energy.

Chemical insensitivity and detonation performance

Nitrides are unstable energy-intensive materials and are expected to be highly insensitive, which allows their use in detonation applications15. The discovered Te–N covalent bonds led us to investigate their energy barrier. According to the ICOHP calculation of the Te–N bonds, the potential barrier induced by the covalent bond is 96.49 kJ/mol per f.u., as shown in Fig. 5, which accounts for most of the tellurium mixing energy barriers (129.80 kJ/mol), and plays an important role in improving the chemical barrier and insensitivity property. Moreover, the study of the stability of arylpentazoles indicates that the potential barriers of their various compounds are 78–100 kJ/mol, which are lower than the predicted potential barriers of cyclo-N6 in our report37. As is known, a large pressure is required to overcome the energy barrier (~82.98 kJ/mol) of dinitrogen N2 to shape the poly-nitrogen phase during synthesis. A higher barrier induced by covalent bonds can resist the spontaneous decomposition of cyclo-N6. In contrast, for the known quasi-planar cyclo-N62− anions in the C2/m-CsN3 phase (Supplementary Fig. 6 and Supplementary Table 1), covalent interactions did not occur between cesium and cyclo-N6 anions since all the ICOHP values presented in Supplementary Table 2 are greater than 0. However, the armchair-like cyclo-N6 in h-WN6 has covalent bond characteristics, which shows that armchair-like N6 anions have extra stability and prevent the decomposition of the monatomic forms of solid cyclo-N6 ions into molecular phases.

Fig. 5: Stabilization of the cyclo-N6 anion by covalent bonds entrapment.
figure5

Tellurium mixing enhances the insensitivity of the cyclo-N6 anion by improving the energy barriers by 129.80 kJ/mol per f.u.; the potential barrier induced by the covalent bond is 96.49 kJ/mol per f.u. relative to the isolated cyclo-N6 in the stability effect.

The detonation performance estimated by the Kamlet−Jacobs empirical equations is one of the most important indicators of energetic materials38. The detonation performances of traditional high-energy-density materials, e.g., TNT and RDX, are shown in Supplementary Table 4, and detailed descriptions are provided in Supplementary Note 139. The cyclo-N6 anions that release a large amount of nitrogen are considered environmental friendly clean energetic materials. According to the principle of maximum heat release, the detonation products are determined to be tellurium and nitrogen under ambient conditions. Herein, the gravimetric energy loading density of TeN6 was calculated to be approximately 8.16 g/cm3. We estimated the detonation velocity (D) and detonation pressure (P) using decomposition products at ambient pressure. Intriguingly, due to the dual effects of its high-energy density and loading density, its detonation pressure is four times greater than that of traditional TNT and two times greater than that of pentazolate anion in MgN10 salt40,41.

In summary, we report an armchair-like cyclo-N6 anion salt with an inherent single covalent bond though swarm-intelligence structure searches of the TeN6 system. The covalent bond modifies the distribution density of local electron clouds and effectively increases the kinetic energy, which is an important factor for metallization in the TeN6 structure. More importantly, the armchair-like cyclo-N6 anion can be stabilized by additional covalent bond entrapment, which effectively improves the chemical barrier and insensitivity. In addition, the energy density of cyclo-N6 anions is higher than that of multitudinous pentazolate and six-membered anions under high pressure in binary nitrides. The simulated detonation performance of the armchair-like cyclo-N6 anion salt is much higher than that of traditional TNT/RDX blasting materials. This study is important regarding the insensitivity of cyclo-N6 anions and may facilitate high-pressure synthesis.

Methods

Structure search

The predicted crystalline phases are based on the global minimization of energy surface merging particle swarm optimization methodology as actualized in the CALYPSO code42. The favorite structures of tellurium nitride were predicted at 0, 20, 50, 100, 150, and 200 GPa using the simulation cell, which consisted of 2−4 f.u.

Electronic structure and total energy calculations

Density functional theory in the Perdew–Burke–Ernzerhof parameterization of the generalized gradient approximation as implemented in the Vienna ab initio simulation (VASP) code was employed for the relaxations43,44,45. Van der Waals (vdW-DF2) interactions were used to correct the structural rationality46. The projector-augmented wave method was utilized with the Te and N potentials, where 5s25p4 and 2s22p3 were considered valence electrons. A plane-wave (PW) basis set cutoff of 850 eV and a Monkhorst–Pack k meshes spacing of 2π × 0.03 Å−1 were used; the self-consistent field tolerance was of 0.1 × 10−5 eV/atom. The COHP analyses executed in the LOBSTER code47 were performed for the TeN6 compound to elucidate its bonding information. To provide detailed information, the COHP was calculated based on the PW method and was performed by re-extracting atom-resolved information from the delocalized PW basis sets48. Based on counted energy-weighted population of the wave functions between two atomic orbitals, the ICOHP value quantitatively represented the covalent bonding strength. In addition, the phonon calculations were performed using a supercell approach in the finite displacement theory as implemented in the PHONOPY code49.

Molecular dynamics simulation

We also performed a first-principles molecular dynamics simulation to determine the thermal stability of the anti-CdCl2 structure via NPT ensembles (N is particle number, P is pressure, and T is temperature). The 84 nitrogen atoms in the super-lattice were used. Molecular dynamics calculations were performed at temperatures of 500 and 1000 K, each of which included 5000 1-fs time steps. Referring to the previous analysis, we generally reached a consensus that the bond lengths of the single bond, double bond, and triple bond were 1.45, 1.25, and 1.10 Å, respectively, under ambient conditions. The N−N single bond distance in cg-N is 1.31 Å at 200 GPa6, which can guide the assignment of N−N bonds to rationalize the local structural environments with the VSEPR theory.

Data availability

The data supporting this publication are available from the authors on request.

References

  1. 1.

    Pickard, C. J. & Needs, R. J. High-pressure phases of nitrogen. Phys. Rev. Lett. 102, 125702 (2009).

  2. 2.

    Eremets, M. I., Gavriliuk, A. G., Trojan, I. A., Dzivenko, D. A. & Boehler, R. Single-bonded cubic form of nitrogen. Nat. Mater. 3, 558–563 (2004).

  3. 3.

    Ma, Y. M., Oganov, A. R., Li, Z., Xie, Y. & Kotakoski, J. Novel high pressure structures of polymeric nitrogen. Phys. Rev. Lett. 102, 065501 (2009).

  4. 4.

    Ashcroft, N. W. Hydrogen dominant metallic alloys: high temperature superconductors? Phys. Rev. Lett. 92, 187002 (2004).

  5. 5.

    Peng, F., Yao, Y., Liu, H. & Ma, Y. M. Crystalline LiN5 predicted from first-principles as a possible high-energy material. J. Phys. Chem. Lett. 6, 2363–2366 (2015).

  6. 6.

    Huang, B. & Frapper, G. Barium–Nitrogen phases under pressure: emergence of structural diversity and nitrogen-rich compounds. Chem. Mater. 30, 7623–7636 (2018).

  7. 7.

    Liu, Z. et al. Metallic and anti-metallic properties of strongly covalently bonded energetic AlN5 nitrides. Phys. Chem. Chem. Phys. 21, 12029–12035 (2019).

  8. 8.

    Li, X. et al. Hard BN clathrate superconductors. J. Phys. Chem. Lett. 10, 2554–2560 (2019).

  9. 9.

    Sun, W. et al. A map of the inorganic ternary metal nitrides. Nat. Mater. 18, 732–739 (2019).

  10. 10.

    Zhu, H. et al. Pressure-induced series of phase transitions in sodium azide. J. Appl. Phys. 113, 033511 (2013).

  11. 11.

    Li, D. et al. Pressure-induced phase transitions in rubidium azide: studied by in-situ x-ray diffraction. Appl. Phys. Lett. 105, 071903 (2014).

  12. 12.

    Jiang, J. et al. Effect of pressure on 4-toluenesulfonyl azide studied by Raman scattering and synchrotron X-ray diffraction. J. Phys. Chem. C 121, 1032–1039 (2017).

  13. 13.

    Laniel, D. et al. Synthesis of magnesium-nitrogen salts of polynitrogen anions. Nat. Commun. 10, 4515 (2019).

  14. 14.

    Wang, P., Lin, Q., Xu, Y. & Lu, M. Pentazole anion cyclo-N5 : a rising star in nitrogen chemistry and energetic materials. Sci. China Chem. 61, 1355–1358 (2018).

  15. 15.

    Zhang, L. et al. Stabilization of the dual-aromatic cyclo-N5(−) anion by acidic entrapment. J. Phys. Chem. Lett. 10, 2378–2385 (2019).

  16. 16.

    Christe, K. O. Recent advances in the chemistry of N5 +, N5 and high-oxygen compounds. Propellants Explos. Pyrotech. 32, 194–204 (2007).

  17. 17.

    Zhang, C. et al. Synthesis and characterization of the pentazolate anion cyclo-N5 in (N5)6(H3O)3(NH4)4Cl. Science 355, 374–376 (2017).

  18. 18.

    Huang, H. et al. Reconciling the debate on the existence of pentazole HN5 in the pentazolate salt of (N5)6(H3O)3(NH4)4Cl. J. Am. Chem. Soc. 141, 2984–2989 (2019).

  19. 19.

    Steele, B. A. et al. High-pressure synthesis of a pentazolate salt. Chem. Mater. 29, 735–741 (2017).

  20. 20.

    Laniel, D., Weck, G., Gaiffe, G., Garbarino, G. & Loubeyre, P. High-pressure synthesized lithium pentazolate compound metastable under ambient conditions. J. Phys. Chem. Lett. 9, 1600–1604 (2018).

  21. 21.

    Moran, N., Shmuel, Z. & Yehuda, H. Stability of polynitrogen compounds: the importance of separating the σ and π electron systems. J. Phys. Chem. A 113, 7376–7382 (2009).

  22. 22.

    Prasad, D. L. V. K. & Ashcroft, N. W., . & HoffmannR. Evolving structural diversity and metallicity in compressed lithium azide. J. Phys. Chem. C 117, 20838–20846 (2013).

  23. 23.

    Wang, X. et al. Layered polymeric nitrogen in RbN3 at high pressures. Sci. Rep. 5, 16677 (2015).

  24. 24.

    Wei, S. et al. Alkaline-earth metal (Mg) polynitrides at high pressure as possible high-energy materials. Phys. Chem. Chem. Phys. 19, 9246 (2017).

  25. 25.

    Zhu, S. et al. Stable calcium nitrides at ambient and high pressures. Inorg. Chem. 55, 7550–7555 (2016).

  26. 26.

    Xia, K. et al. A novel superhard tungsten nitride predicted by machine-learning accelerated crystal structure search. Sci. Bull. 63, 817–824 (2018).

  27. 27.

    Yu, H., Lin, X., Li, K. & Chen, Y. Unveiling a novel, cation-rich compound in a high-pressure Pb-Te binary system. ACS Cent. Sci. 5, 683–687 (2019).

  28. 28.

    Klapotke, T. M., Krumm, B., Mayer, P. & Schwab, I. Binary tellurium(IV) azides: Te(N3)4 and [Te(N3)5]. Angew. Chem. 42, 5843–5846 (2003).

  29. 29.

    Ohanessian, G., Hiberty, P. C., Lefour, J. M., Flament, J. P. & Shaik, S. S. Is delocalization a driving force in chemistry? First- and second-row heteroannulenes. Inorg. Chem. 27, 2219–2224 (1988).

  30. 30.

    Liu, H. & Ma, Y. M. Proton or deuteron transfer in phase IV of solid hydrogen and deuterium. Phys. Rev. Lett. 110, 025903 (2013).

  31. 31.

    Zhang, M. L. et al. Superhard BC(3) in cubic diamond structure. Phys. Rev. Lett. 114, 015502 (2015).

  32. 32.

    Shaik, S., Shurki, A., Danovich, D. & Hiberty, P. C. A different story of π-delocalizations: the distortivity of π-electrons and its chemical manifestations. Chem. Rev. 101, 1501–1539 (2001).

  33. 33.

    He, J., Xia, Y., Naghavi, S. S., Ozolins, V. & Wolverton, C. Designing chemical analogs to PbTe with intrinsic high band degeneracy and low lattice thermal conductivity. Nat. Commun. 10, 719 (2019).

  34. 34.

    Vega, D., Almeida, D., Ruette, F., Sierralta, A. & Sánchez, M. AIM-UC: an application for QTAIM analysis. J. Comput. Methods Sci. Eng. 14, 131–136 (2014).

  35. 35.

    Song, X. Q. et al. Exotic hydrogen bonding in compressed ammonia hydrides. J. Phys. Chem. Lett. 10, 2761–2766 (2019).

  36. 36.

    Gillespie, R. J. The valence-shell electron-pair repulsion (VSEPR) theory of directed valency. J. Chem. Educ. 40, 295–301 (1963).

  37. 37.

    Jiao, F. & Zhang, C. Origin of the considerably high thermal stability of cyclo-N5 containing salts at ambient conditions. Cryst. Eng. Comm. 21, 3592–3604 (2019).

  38. 38.

    Kamlet, M. J. & Jacobs, S. J. Chemistry of detonations. I. A simple method for calculating detonation properties of C–H–N–O explosives. J. Chem. Phys. 48, 23–35 (1968).

  39. 39.

    Zhang, Q. et al. Prediction of detonation pressure and velocity of explosives with micrometer aluminum powders. Cent. Eur. J. Energetic Mater. 9, 77–86 (2012).

  40. 40.

    Xia, K. et al. Pressure-stabilized high-energy-density alkaline-earth-metal pentazolate salts. J. Phys. Chem. C. 123, 10205–10211 (2019).

  41. 41.

    Keshavarz, M. H. & Pouretedal, H. R. Predicting detonation velocity of ideal and less ideal explosives via specific impulse. Indian J. Eng. Mater. Sci. 11, 429–432 (2004).

  42. 42.

    Wang, H. et al. CALYPSO structure prediction method and its wide application. Comput. Mater. Sci. 112, 406–415 (2016).

  43. 43.

    Dunnington, B. D. & Schmidt, J. R. Generalization of natural bond orbital analysis to periodic systems: applications to solids and surfaces via plane-wave density functional theory. J. Chem. Theory Comput 8, 1902–1911 (2012).

  44. 44.

    Blöchl, P. E. Projector augmented-wave method. Phys. Rev. B 50, 17953–17979 (1994).

  45. 45.

    Parr, R. G. Density functional theory. Ann. Rev. Phys. Chem. 34, 631–656 (1983).

  46. 46.

    Thonhauser, T. et al. Spin signature of nonlocal correlation binding in metal-organic frameworks. Phys. Rev. Lett. 115, 136402 (2015).

  47. 47.

    Maintz, S., Deringer, V. L., Tchougreeff, A. L. & Dronskowski, R. Analytic projection from plane-wave and PAW wavefunctions and application to chemical-bonding analysis in solids. J. Comput. Chem. 34, 2557–2567 (2013).

  48. 48.

    Dronskowski, R. Crystal Orbital Hamilton Populations (COHP): energy-resolved visualization of chemical bonding in solids based on density-functional calculations. J. Phys. Chem. A 97, 8617–8624 (1993).

  49. 49.

    Togo, A., Oba, F. & Tanaka, I. First-principles calculations of the ferroelastic transition between rutile-type and CaCl2-type SiO2 at high pressures. Phys. Rev. B 78, 134106 (2008).

Download references

Acknowledgements

This work was supported by the National Key R&D Program of China (2018YFA0703404), National Key Research and Development Program (No. 2017YFA0403704), National Natural Science Foundation of China (Nos. 91745203, 11404134, 11574109, 11474127, and 11674122), National Key Research and Development Program of China (2016YFB0201204). Program for Changjiang Scholars and Innovative Research Team in University (No. IRT_15R23), National Found for Fostering Talents of basic Science (No. J1103202), Parts of calculations were performed in the High Performance Computing Center (HPCC) of Jilin University.

Author information

Affiliations

Authors

Contributions

D.L. designed this project. Z.L., Q.Z., F.T., D.D., and F.L. analyzed the data; Z.L., D.L., and T.C. made the analysis and wrote the paper. All authors discussed the results and commented on the paper.

Corresponding authors

Correspondence to Da Li or Tian Cui.

Ethics declarations

Competing interests

The authors declare no competing interests.

Additional information

Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Supplementary information

Rights and permissions

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.

Reprints and Permissions

About this article

Verify currency and authenticity via CrossMark

Cite this article

Liu, Z., Li, D., Zhuang, Q. et al. Formation mechanism of insensitive tellurium hexanitride with armchair-like cyclo-N6 anions. Commun Chem 3, 42 (2020). https://doi.org/10.1038/s42004-020-0286-1

Download citation

Comments

By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.