English

Boron and nitrogen isotope effects on hexagonal boron nitride properties

Materials Science 2023-06-26 v1

Abstract

The unique physical, mechanical, chemical, optical, and electronic properties of hexagonal boron nitride (hBN) make it a promising two-dimensional material for electronic, optoelectronic, nanophotonic, and quantum devices. Here we report on the changes in hBN's properties induced by isotopic purification in both boron and nitrogen. Previous studies on isotopically pure hBN have focused on purifying the boron isotope concentration in hBN from its natural concentration (approximately 20 at%\% 10^{10}B, 80 at%\% 11^{11}B) while using naturally abundant nitrogen (99.6 at%\% 14^{14}N, 0.4 at%\% 15^{15}N), i.e. almost pure 14^{14}N. In this study, we extend the class of isotopically-purified hBN crystals to 15^{15}N. Crystals in the four configurations, namely h10^{10}B14^{14}N, h11^{11}B14^{14}N, h10^{10}B15^{15}N, and h11^{11}B15^{15}N, were grown by the metal flux method using boron and nitrogen single isotope (>99%>99\%) enriched sources, with nickel plus chromium as the solvent. In-depth Raman and photoluminescence spectroscopies demonstrate the high quality of the monoisotopic hBN crystals with vibrational and optical properties of the 15^{15}N-purified crystals at the state of the art of currently available 14^{14}N-purified hBN. The growth of high-quality h10^{10}B14^{14}N, h11^{11}B14^{14}N, h10^{10}B15^{15}N, and h11^{11}B15^{15}N opens exciting perspectives for thermal conductivity control in heat management, as well as for advanced functionalities in quantum technologies.

Keywords

Cite

@article{arxiv.2306.13358,
  title  = {Boron and nitrogen isotope effects on hexagonal boron nitride properties},
  author = {E. Janzen and H. Schutte and J. Plo and A. Rousseau and T. Michel and W. Desrat and P. Valvin and V. Jacques and G. Cassabois and B. Gil and J. H. Edgar},
  journal= {arXiv preprint arXiv:2306.13358},
  year   = {2023}
}

Comments

13 pages, 7 figures

R2 v1 2026-06-28T11:12:36.132Z