TY - JOUR
T1 - Optical constants and band structure of trigonal NiO
AU - Ghosh, Ayana
AU - Nelson, Cayla M.
AU - Abdallah, Lina S.
AU - Zollner, Stefan
N1 - Publisher Copyright:
© 2015 American Vacuum Society.
PY - 2015/11/1
Y1 - 2015/11/1
N2 - Using spectroscopic ellipsometry and transmission measurements, the authors determined the optical constants (absorption coefficient, complex refractive index, and dielectric function) of bulk trigonal NiO from 0.08 to 6.5 eV. By careful discussion of the data, elastic scattering by oxygen bubbles was ruled out and the effects of surface roughness were removed numerically to obtain an accurate dielectric function of NiO. A direct band gap of 0.85 eV was found from transmission and assigned to direct interband transitions from the Ni-O hybrid valence band states to the Ni 4s conduction band at the center of the Brillouin zone. At 4 eV, the authors find the well-known charge transfer gap from the lower to the upper Hubbard band. Several intermediate sharp peaks were also found. The temperature dependence of the NiO charge transfer gap is similar to the E1 gap of Si between 100 and 700 K. At higher temperatures, heating NiO in vacuum leads to sublimation, which has drastic irreversible consequences for the pseudodielectric function of the sample, including a strong Ni nanoparticle plasmon peak at 2 eV.
AB - Using spectroscopic ellipsometry and transmission measurements, the authors determined the optical constants (absorption coefficient, complex refractive index, and dielectric function) of bulk trigonal NiO from 0.08 to 6.5 eV. By careful discussion of the data, elastic scattering by oxygen bubbles was ruled out and the effects of surface roughness were removed numerically to obtain an accurate dielectric function of NiO. A direct band gap of 0.85 eV was found from transmission and assigned to direct interband transitions from the Ni-O hybrid valence band states to the Ni 4s conduction band at the center of the Brillouin zone. At 4 eV, the authors find the well-known charge transfer gap from the lower to the upper Hubbard band. Several intermediate sharp peaks were also found. The temperature dependence of the NiO charge transfer gap is similar to the E1 gap of Si between 100 and 700 K. At higher temperatures, heating NiO in vacuum leads to sublimation, which has drastic irreversible consequences for the pseudodielectric function of the sample, including a strong Ni nanoparticle plasmon peak at 2 eV.
UR - http://www.scopus.com/inward/record.url?scp=84943646370&partnerID=8YFLogxK
U2 - 10.1116/1.4932514
DO - 10.1116/1.4932514
M3 - Article
AN - SCOPUS:84943646370
SN - 0734-2101
VL - 33
JO - Journal of Vacuum Science and Technology, Part A: Vacuum, Surfaces and Films
JF - Journal of Vacuum Science and Technology, Part A: Vacuum, Surfaces and Films
IS - 6
M1 - 061203
ER -