TY - JOUR
T1 - Spectroscopic dielectric tensor of monoclinic crystals
T2 - CdWO4
AU - Jellison, G. E.
AU - McGuire, M. A.
AU - Boatner, L. A.
AU - Budai, J. D.
AU - Specht, E. D.
AU - Singh, D. J.
PY - 2011/11/9
Y1 - 2011/11/9
N2 - Generalized ellipsometry measurements were made using 12 orientations of a monoclinic CdWO4 crystal. Using these measurements and the associated analytical methods presented here, it is shown that the four independent complex elements of the dielectric tensor can be determined at each wavelength. Below the band edge (∼4 eV), the dielectric tensor is real, and, therefore, it is possible to uniquely diagonalize the dielectric tensor and determine the birefringence for light passing along the unique axis, but the orientation of the dielectric tensor axes will be a function of wavelength. Above the band edge, unique diagonalization is not possible. The generalized ellipsometric spectra show some symmetry in the cross-polarization coefficients. When the unique axis is perpendicular to the sample surface, the condition ρps = -ρsp is valid. If the unique axis is perpendicular to the plane of incidence, ρsp = ρps = 0, and if the unique axis is in the plane of incidence, parallel to the sample surface, then ρps = ρsp ≠ 0. The combined experimental and analytical methods described here are applicable to the determination of the spectroscopic dielectric tensors of monoclinic crystals in general.
AB - Generalized ellipsometry measurements were made using 12 orientations of a monoclinic CdWO4 crystal. Using these measurements and the associated analytical methods presented here, it is shown that the four independent complex elements of the dielectric tensor can be determined at each wavelength. Below the band edge (∼4 eV), the dielectric tensor is real, and, therefore, it is possible to uniquely diagonalize the dielectric tensor and determine the birefringence for light passing along the unique axis, but the orientation of the dielectric tensor axes will be a function of wavelength. Above the band edge, unique diagonalization is not possible. The generalized ellipsometric spectra show some symmetry in the cross-polarization coefficients. When the unique axis is perpendicular to the sample surface, the condition ρps = -ρsp is valid. If the unique axis is perpendicular to the plane of incidence, ρsp = ρps = 0, and if the unique axis is in the plane of incidence, parallel to the sample surface, then ρps = ρsp ≠ 0. The combined experimental and analytical methods described here are applicable to the determination of the spectroscopic dielectric tensors of monoclinic crystals in general.
UR - http://www.scopus.com/inward/record.url?scp=82655168281&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.84.195439
DO - 10.1103/PhysRevB.84.195439
M3 - Article
AN - SCOPUS:82655168281
SN - 1098-0121
VL - 84
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 19
M1 - 195439
ER -