TY - JOUR
T1 - Phase transition and bandgap engineering in B1-xAlxN alloys
T2 - DFT calculations and experiments
AU - Zhang, Qifan
AU - Li, Qiang
AU - Zhang, Weihan
AU - Zhang, Haoran
AU - Zheng, Feng
AU - Zhang, Mingyin
AU - Hu, Peng
AU - Wang, Mingdi
AU - Tian, Zhenhuan
AU - Li, Yufeng
AU - Liu, Yuhuai
AU - Yun, Feng
N1 - Publisher Copyright:
© 2021
PY - 2022/2/1
Y1 - 2022/2/1
N2 - BAlN is a promising ultrawide bandgap semiconductor, but systematic studies of its bandgap are scarce. Here, bandgap engineering of BAlN containing the phase transition factor (from hexagonal to wurtzite structures) has been investigated by DFT calculations and verified experimentally. The calculated bandgap bowing parameter of hexagonal BAlN (h-BAlN) is 2.29 eV, while the bandgap bowing parameters of wurtzite BAlN (w-BAlN) are −4.09 eV and 2.48 eV in the B-rich and Al-rich regions, respectively. Meanwhile, calculations indicate that BAlN preferentially forms w-BAlN at Al composition above 18.7%. So, the bandgap variation of BAlN is divided into three regions based on Al composition: h-BAlN (0–18.7%), B-rich w-BAlN (18.7%–50%), Al-rich w-BAlN (50%–1), and each has its own trend. Experimentally, h-BAlN and w-BAlN films were prepared by magnetron co-sputtering technique and the phase transition was observed in X-ray diffraction (XRD) patterns. h-BAlN shows a typical triangular morphology and the Raman and XRD peaks are located at 1371 cm−1 and 44.3°, tending to (1 0 1) h-BN. w-BAlN has a “needle-felt” surface with Raman and XRD peaks at 656 cm−1 and 35.9°, tending to (0 0 2) w-AlN. The experimental bandgap variation of BAlN shows a “W” shape, which can be well explained by the calculation results.
AB - BAlN is a promising ultrawide bandgap semiconductor, but systematic studies of its bandgap are scarce. Here, bandgap engineering of BAlN containing the phase transition factor (from hexagonal to wurtzite structures) has been investigated by DFT calculations and verified experimentally. The calculated bandgap bowing parameter of hexagonal BAlN (h-BAlN) is 2.29 eV, while the bandgap bowing parameters of wurtzite BAlN (w-BAlN) are −4.09 eV and 2.48 eV in the B-rich and Al-rich regions, respectively. Meanwhile, calculations indicate that BAlN preferentially forms w-BAlN at Al composition above 18.7%. So, the bandgap variation of BAlN is divided into three regions based on Al composition: h-BAlN (0–18.7%), B-rich w-BAlN (18.7%–50%), Al-rich w-BAlN (50%–1), and each has its own trend. Experimentally, h-BAlN and w-BAlN films were prepared by magnetron co-sputtering technique and the phase transition was observed in X-ray diffraction (XRD) patterns. h-BAlN shows a typical triangular morphology and the Raman and XRD peaks are located at 1371 cm−1 and 44.3°, tending to (1 0 1) h-BN. w-BAlN has a “needle-felt” surface with Raman and XRD peaks at 656 cm−1 and 35.9°, tending to (0 0 2) w-AlN. The experimental bandgap variation of BAlN shows a “W” shape, which can be well explained by the calculation results.
KW - BAlN
KW - Bandgap engineering
KW - DFT calculations
KW - Magnetron sputtering
KW - Phase transition
UR - https://www.scopus.com/pages/publications/85118582133
U2 - 10.1016/j.apsusc.2021.151641
DO - 10.1016/j.apsusc.2021.151641
M3 - 文章
AN - SCOPUS:85118582133
SN - 0169-4332
VL - 575
JO - Applied Surface Science
JF - Applied Surface Science
M1 - 151641
ER -