TY - JOUR
T1 - Vibrational properties of AIN grown on (111)-oriented silicon
AU - Prokofyeva, T.
AU - Seon, M.
AU - Vanbuskirk, J.
AU - Holtz, M.
AU - Nikishin, S. A.
AU - Faleev, N. N.
AU - Temkin, H.
AU - Zollner, S.
N1 - Funding Information:
This work was supported by the Air Force Office of Scientific Research under grant number AFOSR-84-0377.
PY - 2001
Y1 - 2001
N2 - We study the vibrational spectrum of AIN grown on Si(111). The AIN was deposited using gas-source molecular beam epitaxy. Raman backscattering along the growth c axis and from a cleaved surface perpendicular to the wurtzite c direction allows us to determine the E21, E22, A1(TO), A1(LO), and E1(TO) phonon energies. For a 0.8-μm-thick AIN layer under a biaxial tensile stress of 0.6 GPa, these are 249.0, 653.6, 607.3, 884.5, and 666.5 cm-1, respectively. By combining the Raman and x-ray diffraction studies, the Raman stress factor of AIN is found to be -6.3±1.4 cm-1/GPa for the E22 phonon. This factor depends on published values of the elastic constants of AIN, as discussed in the text. The zero-stress E22 energy is determined to be 657.4±0.2 cm-1. Fourier-transform infrared reflectance and absorption techniques allow us to measure the E1(TO) and A1(LO) phonon energies. The film thickness (from 0.06 to 1.0 μm) results in great differences in the reflectance spectra, which are well described by a model using damped Lorentzian oscillators taking into account the crystal anisotropy and the film thickness.
AB - We study the vibrational spectrum of AIN grown on Si(111). The AIN was deposited using gas-source molecular beam epitaxy. Raman backscattering along the growth c axis and from a cleaved surface perpendicular to the wurtzite c direction allows us to determine the E21, E22, A1(TO), A1(LO), and E1(TO) phonon energies. For a 0.8-μm-thick AIN layer under a biaxial tensile stress of 0.6 GPa, these are 249.0, 653.6, 607.3, 884.5, and 666.5 cm-1, respectively. By combining the Raman and x-ray diffraction studies, the Raman stress factor of AIN is found to be -6.3±1.4 cm-1/GPa for the E22 phonon. This factor depends on published values of the elastic constants of AIN, as discussed in the text. The zero-stress E22 energy is determined to be 657.4±0.2 cm-1. Fourier-transform infrared reflectance and absorption techniques allow us to measure the E1(TO) and A1(LO) phonon energies. The film thickness (from 0.06 to 1.0 μm) results in great differences in the reflectance spectra, which are well described by a model using damped Lorentzian oscillators taking into account the crystal anisotropy and the film thickness.
UR - http://www.scopus.com/inward/record.url?scp=0034894678&partnerID=8YFLogxK
M3 - Article
AN - SCOPUS:0034894678
SN - 0163-1829
VL - 63
SP - 1253131
EP - 1253137
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 12
M1 - 125313
ER -