Optical filters constructed from multilayers of dielectric and thin metallic films operating in the anomalous skin effect region

1989 ◽  
Vol 6 (6) ◽  
pp. 1103 ◽  
Author(s):  
Juh-Tzeng Lue ◽  
Yann-Shyh Hor
1972 ◽  
Vol 94 (4) ◽  
pp. 467-472 ◽  
Author(s):  
C. H. Forsberg ◽  
G. A. Domoto

The spectral radiation properties of thin metallic films are obtained through the numerical solution of the governing integrodifferential equation for the anomalous skin effect with size effects included. The theory predicts that at low temperatures there will be a film thickness for which the emittance is a minimum. This minimum, which is lower than the emittance for a bulk specimen, is apparently due to interference effects arising from the finite film thickness. It is also found that for certain cases transmission through a film is not negligible compared with the emission from the film. The analysis is extended to include metal-coated dielectric films, and the theoretical results are compared with existing experimental data.


2021 ◽  
Vol 129 (7) ◽  
pp. 889
Author(s):  
А.Б. Сотский ◽  
Е.А. Чудаков ◽  
Л.И. Сотская

Inhomogeneous Fredholm’s integral equations of the second kind are formulated, which describe the fields of TE and TM polarized waves in metallic films with allowance for the anomalous skin effect. The equations are solved numerically by the quadrature method. The electric fields in gold and aluminum films located on a silicon substrate and the angular dependences of the polarization angles of light reflected from the films are investigated. It is found that the solution of the inverse problem of multi-angle ellipsometry for metallic films using the standard model of the normal skin effect is characterized by instability of the reconstructed complex refractive index of the metal with a change in the thickness of the metallic film.


1962 ◽  
Vol 27 (4) ◽  
pp. 842-843 ◽  
Author(s):  
Sadao Nakajima ◽  
Mitsuo Watabe

1972 ◽  
Vol 43 (7) ◽  
pp. 2996-3001 ◽  
Author(s):  
G. R. Henry

The anomalous skin effect arises in good conductors at low temperatures and high frequencies when the electronic mean free path becomes comparable with or greater than the classically calculated skin depth. Measurements have been made on a number of metals at frequencies of 1200 and 3600 Mc/s, and the form of variation of r. f. surface conductance with d. c. conductivity agrees well with that predicted theoretically by Reuter & Sondheimer, assuming that the electrons are scattered diffusely when they hit the surface of the metal. From the results, estimates are made of the effective value of σ/ l , the ratio of d. c. conductivity to mean free path, and hence of the free surface area of the occupied region of k -space. The estimate for copper agrees well with that expected theoretically; those for silver and gold are rather lower than the theoretical values. For the other metals investigated, tin, cadmium, lead and aluminium, no theoretical estimates are available. The results are very sensitive to the presence of surface imperfections; the effect of these is discussed.


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