Diffuse reflection and transmission of light by a medium with an arbitrary scattering indicatrix

2000 ◽  
Vol 44 (8) ◽  
pp. 495-500
Author(s):  
D. N. Rachkovskii
1967 ◽  
Vol 1 (1) ◽  
pp. 11-11
Author(s):  
R. B. T. Black

It has become recognized that the dominant mechanism in the formation of the cores of resonance lines in the solar spectrum is non-coherent scattering, e.g., Thomas (1957). A study, preliminary to the theoretical investigation of the spectra of chromospheric structures, is the evaluation of the effect of diffuse reflection and transmission by non-coherently scattering media.


1983 ◽  
Vol 89 (2) ◽  
pp. 345-354 ◽  
Author(s):  
E. A. Saad ◽  
S. A. El Wakil ◽  
M. H. Haggag

1966 ◽  
Vol 44 (16) ◽  
pp. 1945-1950 ◽  
Author(s):  
R. W. Frei ◽  
D. E. Ryan ◽  
V. T. Lieu

Diffuse reflectance spectroscopy can be used for the analysis of multicomponent systems in the adsorbed state. The Kubelka–Munk theory for diffuse reflection and transmission on light-scattering layers has been applied for this analysis. Simple dye mixtures adsorbed on thin-layer chromatography-grade adsorbents were employed. The method can be adapted directly to the analysis of incompletely separated components on chromatographic adsorbents.


1967 ◽  
Vol 20 (3) ◽  
pp. 271 ◽  
Author(s):  
RBT Black

Diffusely reflected and transmitted spectral line profiles are calculated for uniform noncoherently scattering media onto which radiation of frequency near that of a resonance line of the medium is incident. Profiles are calculated for incident light that is either collimated or unifQrmly diffused and that is either monochromatic, or of uniform frequency distribution, or contains an absorption line centred on the resonance line under discussion. Spectral lines generated by uniformly excited media are also calculated.


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