Charge density and chemical bonding in cubic boron nitride

1986 ◽  
Vol 117 (1-2) ◽  
pp. 61-71 ◽  
Author(s):  
G. Will ◽  
A. Kirfel ◽  
B. Josten
2014 ◽  
Vol 70 (a1) ◽  
pp. C283-C283
Author(s):  
Nanna Wahlberg ◽  
Niels Bindzus ◽  
Lasse Bjerg ◽  
Jacob Becker ◽  
Bo Iversen

The resent progress in powder diffraction provides data of quality beyond multipolar modeling of the valence density. As was recently shown in a benchmark study of diamond by Bindzus et al.[1] The next step is to investigate more complicated chemical bonding motives, to determine the effect of bonding on the core density. Cubic boron nitride lends itself as a perfect candidate because of its many similarities with diamond: bonding pattern in the extended network structure, hardness, and the quality of the crystallites.[2] However, some degree ionic interaction is a part of the bonding in boron nitride, which is not present in diamond. By investigating the core density in boron nitride we may obtain a deeper understanding of the effect of bonding on the total density. We report here a thorough investigation of the charge density of cubic boron nitride with a detailed modelling of the inner atom charge density. By combining high resolution powder X-ray diffraction data and an extended multipolar model an experimental modeling of the core density is possible.[3] The thermal motion is a problem since it is strongly correlated to the changes of the core density, but by combining the average displacement from a Wilson plot and a constrained refinement, a reasonable result has been obtained. The displacement parameters reported here are significantly lower than those previously reported, stressing the importance of an adequate description of the core density. The charge transfer from boron to nitrogen clearly affects the inner electron density, which is evident from theoretical as well as experimental result. The redistribution of electron density will, if not accounted for, result in increased thermal parameters. It is estimated that 1.7-2 electrons is transferred from boron to nitrogen.


2021 ◽  
Author(s):  
Kirill Shumilov ◽  
Zerina Mehmedovic, ◽  
Hang Ying ◽  
Patricia Poths ◽  
Selbi Nuryyeva ◽  
...  

<div>WB<sub>4.2 </sub>is one of the hardest metals known. Though not harder than diamond and cubic boron nitride, it surpasses these established hard materials in being cheaper, easier to produce and process, and also more functional. Metal impurities have been shown to a?ct and in some cases further improve the intrinsic hardness of WB<sub>4.2</sub>, but the mechanism of hardening remained elusive. In this work we ?first theoretically elucidate the preferred placements of Ti, V, Cr, Mn, Zr, Nb, Mo, Hf, Ta in the WB<sub>4.2</sub> structure, and show these metals to preferentially replace W in two competing positions with respect to the partially occupied B<sub>3</sub> cluster site. The impurities avoid the void position in the structure. Next, we analyze the chemical bonding within these identifi?ed doped structures, and propose two different mechanisms of strengthening the material, afforded by these impurities, and dependent on their nature. Smaller impurity atoms (Ti, V, Cr, Mn) with deeply lying valence atomic orbitals cause the inter-layer compression of WB<sub>4.2</sub>, which strengthens the B<sub>hex</sub>–B<sub>cluster</sub> bonding slightly. Larger impurities (Zr, Nb, Mo, Hf, Ta) with higher-energy valence orbitals, while expanding the structure and negatively impacting the B<sub>hex</sub>–B<sub>cluster</sub> bonding, also form strong B<sub>cluster</sub>–M bonds. The latter effect is an order of magnitude more substantial than the effect on the B<sub>hex</sub>–B<sub>cluster</sub> bonding. We conclude that the e effect of the impurities on the boride hardness does not simply reduce to structure interlocking due to the size difference between M and W, but instead, has a significant electronic origin.</div>


2021 ◽  
Author(s):  
Kirill Shumilov ◽  
Zerina Mehmedovic, ◽  
Hang Ying ◽  
Patricia Poths ◽  
Selbi Nuryyeva ◽  
...  

<div>WB<sub>4.2 </sub>is one of the hardest metals known. Though not harder than diamond and cubic boron nitride, it surpasses these established hard materials in being cheaper, easier to produce and process, and also more functional. Metal impurities have been shown to a?ct and in some cases further improve the intrinsic hardness of WB<sub>4.2</sub>, but the mechanism of hardening remained elusive. In this work we ?first theoretically elucidate the preferred placements of Ti, V, Cr, Mn, Zr, Nb, Mo, Hf, Ta in the WB<sub>4.2</sub> structure, and show these metals to preferentially replace W in two competing positions with respect to the partially occupied B<sub>3</sub> cluster site. The impurities avoid the void position in the structure. Next, we analyze the chemical bonding within these identifi?ed doped structures, and propose two different mechanisms of strengthening the material, afforded by these impurities, and dependent on their nature. Smaller impurity atoms (Ti, V, Cr, Mn) with deeply lying valence atomic orbitals cause the inter-layer compression of WB<sub>4.2</sub>, which strengthens the B<sub>hex</sub>–B<sub>cluster</sub> bonding slightly. Larger impurities (Zr, Nb, Mo, Hf, Ta) with higher-energy valence orbitals, while expanding the structure and negatively impacting the B<sub>hex</sub>–B<sub>cluster</sub> bonding, also form strong B<sub>cluster</sub>–M bonds. The latter effect is an order of magnitude more substantial than the effect on the B<sub>hex</sub>–B<sub>cluster</sub> bonding. We conclude that the e effect of the impurities on the boride hardness does not simply reduce to structure interlocking due to the size difference between M and W, but instead, has a significant electronic origin.</div>


1996 ◽  
Vol 52 (4) ◽  
pp. 586-595 ◽  
Author(s):  
A. Lichanot ◽  
P. Azavant ◽  
U. Pietsch

The electronic charge density of cubic boron nitride is calculated within the ab initio Hartree–Fock approximation using the program CRYSTAL. Based on Debye hypothesis, the thermal motion of atoms is considered by disturbing the atomic orbitals by mean-square displacements given from experiment. The calculated difference charge density obtained by subtraction of the total density and that of an independent atomic model (IAM) is characterized by a charge-density accumulation between next neighbours slightly shifted towards the nitrogen. The calculated X-ray structure amplitudes are compared with two different data sets [Josten (1985). Thesis. University of Bonn, Germany; Eichhorn, Kirfel, Grochowski & Serda (1991). Acta Cryst. B47, 843–848]. In both cases, very good agreement is found beyond the 420 reflection. The first six structure amplitudes are generally lower or larger compared with Josten's and Eichhorn et al.'s data, respectively. Whereas our charge density can be interpreted by a balanced ratio between covalent overlap and electronic charge transfer between neighbouring valence shells, the density plots calculated from experimental data express either the charge transfer (Josten, 1985) or the covalency (Eichorn et al., 1991).


Author(s):  
D. L. Medlin ◽  
T. A. Friedmann ◽  
P. B. Mirkarimi ◽  
M. J. Mills ◽  
K. F. McCarty

The allotropes of boron nitride include two sp2-bonded phases with hexagonal and rhombohedral structures (hBN and rBN) and two sp3-bonded phases with cubic (zincblende) and hexagonal (wurtzitic) structures (cBN and wBN) (Fig. 1). Although cBN is synthesized in bulk form by conversion of hBN at high temperatures and pressures, low-pressure synthesis of cBN as a thin film is more difficult and succeeds only when the growing film is simultaneously irradiated with a high flux of ions. Only sp2-bonded material, which generally has a disordered, turbostratic microstructure (tBN), will form in the absence of ion-irradiation. The mechanistic role of the irradiation is not well understood, but recent work suggests that ion-induced compressive film stress may induce the transformation to cBN.Typically, BN films are deposited at temperatures less than 1000°C, a regime for which the structure of the sp2-bonded precursor material dictates the phase and microstructure of the material that forms from conventional (bulk) high pressure treatment.


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