Ion-assisted pulsed laser deposition of cubic boron nitride films

Abstract

Ion-assisted pulsed laser deposition has been used to produce films containing ≳85% sp3-bonded cubic boron nitride (c-BN). By ablating from a target of hexagonal boron nitride (h-BN), BN films have been deposited on heated (50–800 °C) Si(100) surfaces. The growing films are irradiated with ions from a broad beam ion source operated with Ar and N2 source gasses. Successful c-BN synthesis has been confirmed by Fourier transform infrared (FTIR) spectroscopy, high-resolution transmission electron microscopy (TEM), selected-area electron diffraction, electron energy-loss spectroscopy, and x-ray diffraction. The films are polycrystalline and show grain sizes up to 300 Å. In addition, Rutherford backscattering, elastic recoil detection, and Auger electron spectroscopies have been used to further characterize the samples. The effects of varying ion current density, substrate growth temperature, growth time, and ion energy have been investigated. It is found that stoichiometric films with a high c-BN percentage can be grown between 150 and 500 °C. Below ∼150 °C, the c-BN percentage drops dramatically, and the deposited film is completely resputtered at the current densities and ablation deposition rates used. As the deposition temperature rises above ∼500 °C the c-BN percentage also drops, but less dramatically than at low temperatures. In addition, the IR-active c-BN mode narrows considerably as the deposition temperature increases, suggesting that the c-BN material has fewer defects or larger grain size. It is found that films with a high c-BN percentage are deposited only in a narrow window of ion/atom arrival values that are near unity at beam energies between 800 and 1200 eV. Below this window the deposited films have a low c-BN percentage, and above this window the deposited film is completely resputtered. Using FTIR analysis, it is found that the c-BN percentage in these samples is dependent upon growth time. The initial deposit is essentially all sp2-bonded material and sp3-bonded material forms above this layer. Consistently, cross-section TEM samples reveal this layer to consist of an amorphous BN layer (∼30 Å thick) directly on the Si substrate followed by highly oriented turbostratic BN (∼300 Å thick) and finally the c-BN layer. The h-BN/t-BN interfacial layer is oriented with the 002 basal planes perpendicular to the plane of the substrate. Importantly, the position of the c-BN IR phonon changes with growth time. Initially this mode appears near 1130 cm−1 and decreases with growth time to a constant value of 1085 cm−1. Since in bulk c-BN the IR mode appears at 1065 cm−1, a large compressive stress induced by the ion bombardment is suggested. Possible mechanisms are commented on for the conversion process to c-BN based upon the results.

The theoretical study on interaction of hydrogen with single-walled boron nitride nanotubes. I. The reactive force field ReaxFFHBN development

“…[15][16][17] However, the boron nitride thin films synthesized so far exhibit multilayered structures with different phases. 18,19 The interfacial region next to the substrate was usually an amorphous layer of a few nanometers, on the top of which was a textured h-BN layer, and a c-BN layer was observed upon the h-BN layer.…”

Nanohardness and chemical bonding of boron nitride films

“…high voltage, bias sputtering or ion beam bombardment at the substrate. [20][21][22][23] Mechanisms proposed for cBN stabilization in BN films include both preferential sputtering effects [24] , the presence of large stresses [25][26] and subplantation [27][28] wherein low energy ions are implanted below the surface to increase local density. Post deposition treatments of hBN are also revealing, as 180 keV N 2 + (i.e.…”

Nitrogen Implantation Effects on the Chemical Bonding and Hardness of Boron and Boron Nitride Coatings

“…high voltage, bias sputtering or ion beam bombardment at the substrate. [18][19][20][21] Mechanisms proposed for cBN stabilization in BN films include both preferential sputtering effects [22] , the presence of large stresses [23][24] and subplantation [25][26] wherein low energy ions are implanted below the surface to increase local density. Post deposition treatments of hBN are also revealing, as 180 keV N 2 + ion implantation at a 10 mA cm -2 current density induced a significant proportion of sp 3 bonding characteristic of cBN.…”