Inhomogeneity in Refractive Index of Evaporated MgF2 Film
- 1 October 1968
- journal article
- Published by IOP Publishing in Japanese Journal of Applied Physics
- Vol. 7 (10) , 1181-1185
- https://doi.org/10.1143/jjap.7.1181
Abstract
By the use of a zero-order approximate formula for reflectance the thickness and inhomogeneity of a transparent film can be determined from angles of incidence for minimum reflectance measured for different wavelengths with p-polarized light. The method was applied to evaporated MgF2 films. The results are as follows. Up to thicknesses of about 1200 Å, the films are homogeneous. For thicknesses from 1300 to 2200 Å, the difference between the refractive indices at the front and rear surfaces of film is less than 0.002, and is undetermined. For thicknesses from 2300 to 6100 Å, the difference is measured as 0.003∼0.034 and increases linearly with film thickness. The refractive index at the front surface of film is larger than at the rear one. The inhomogeneity begins increasing at about 2300 Å.Keywords
This publication has 15 references indexed in Scilit:
- Reflection of Light from Filmed Rough Surface: Determination of Film Thickness and rms RoughnessJapanese Journal of Applied Physics, 1967
- On the production and properties of inhomogeneous thin filmsJournal de Physique, 1964
- Homogeneous-Inhomogeneous Thin-Film CombinationsJournal of the Optical Society of America, 1961
- Reflectance of an Inhomogeneous Thin FilmJournal of the Optical Society of America, 1961
- Reflection Coefficient of Optically Inhomogeneous LayersJournal of the Optical Society of America, 1958
- Propagation of Plane Electromagnetic Waves in Inhomogeneous MediaJournal of the Optical Society of America, 1958
- Reflection of Waves by an Inhomogeneous MediumPhysical Review B, 1954
- Reflexion elektromagnetischer Wellen an einer inhomogenen SchichtAnnalen der Physik, 1947
- Bemerkung zur Theorie des Lichtdurchgangs durch inhomogene durchsichtige SchichtenAnnalen der Physik, 1941
- Reflexion elektromagnetischer Wellen an einer inhomogenen Schicht nach der Wentzel‐Kramers‐Brillouin‐MethodeAnnalen der Physik, 1941