Abstract

We report the growth of high quality rhombohedral boron nitride (rBN) crystals by the iron flux method at atmospheric pressure. In contrast to the lamellar structure of standard hexagonal boron nitride (hBN) covering the metal ingot, the current synthetized BN shell is composed of many triangular bulk crystallites, of submillimeter size, predominantly in the rhombohedral phase, with only weak traces of hBN detected by high resolution X-ray diffraction. The low-temperature photoluminescence emission confirms the excellent quality of the rhombohedral stacking with unprecedented width for all phonon replicas at the band edge. The Raman spectra are characterized by the absence of any low-energy modes at ~50 cm⁻¹, the presence of an extended band around 800 cm⁻¹ and an asymmetric high energy mode at 1366 cm⁻¹. These observations are in very good agreement with the phonon dispersion calculated for the rhombohedral primitive cell with C3v symmetry.

Abstract

We report the growth of high quality rhombohedral boron nitride (rBN) crystals by the iron flux method at atmospheric pressure. In contrast to the lamellar structure of standard hexagonal boron nitride (hBN) covering the metal ingot, the current synthetized BN shell is composed of many triangular bulk crystallites, of submillimeter size, predominantly in the rhombohedral phase, with only weak traces of hBN detected by high resolution X-ray diffraction. The low-temperature photoluminescence emission confirms the excellent quality of the rhombohedral stacking with unprecedented width for all phonon replicas at the band edge. The Raman spectra are characterized by the absence of any low-energy modes at ~50 cm⁻¹, the presence of an extended band around 800 cm⁻¹ and an asymmetric high energy mode at 1366 cm⁻¹. These observations are in very good agreement with the phonon dispersion calculated for the rhombohedral primitive cell with C3v symmetry.

Abstract

We report the growth of high quality rhombohedral boron nitride (rBN) crystals by the iron flux method at atmospheric pressure. In contrast to the lamellar structure of standard hexagonal boron nitride (hBN) covering the metal ingot, the current synthetized BN shell is composed of many triangular bulk crystallites, of submillimeter size, predominantly in the rhombohedral phase, with only weak traces of hBN detected by high resolution X-ray diffraction. The low-temperature photoluminescence emission confirms the excellent quality of the rhombohedral stacking with unprecedented width for all phonon replicas at the band edge. The Raman spectra are characterized by the absence of any low-energy modes at ~50 cm⁻¹, the presence of an extended band around 800 cm⁻¹ and an asymmetric high energy mode at 1366 cm⁻¹. These observations are in very good agreement with the phonon dispersion calculated for the rhombohedral primitive cell with C3v symmetry.

Abstract

We report the growth of high quality rhombohedral boron nitride (rBN) crystals by the iron flux method at atmospheric pressure. In contrast to the lamellar structure of standard hexagonal boron nitride (hBN) covering the metal ingot, the current synthetized BN shell is composed of many triangular bulk crystallites, of submillimeter size, predominantly in the rhombohedral phase, with only weak traces of hBN detected by high resolution X-ray diffraction. The low-temperature photoluminescence emission confirms the excellent quality of the rhombohedral stacking with unprecedented width for all phonon replicas at the band edge. The Raman spectra are characterized by the absence of any low-energy modes at ~50 cm⁻¹, the presence of an extended band around 800 cm⁻¹ and an asymmetric high energy mode at 1366 cm⁻¹. These observations are in very good agreement with the phonon dispersion calculated for the rhombohedral primitive cell with C3v symmetry.