Refractive Index and Transmission Coefficient Recovery Algorithm of Crystal-like Objects

Author(s):  
Yan-kui Sun ◽  
Xi-peng Tong ◽  
Wei Wang ◽  
Hong-chuan Yu
2020 ◽  
Vol 27 (1) ◽  
pp. 75-82
Author(s):  
Mikhail Svechnikov ◽  
Nikolay Chkhalo ◽  
Alexey Lopatin ◽  
Roman Pleshkov ◽  
Vladimir Polkovnikov ◽  
...  

In this work, the refractive index of beryllium in the photon energy range 20.4–250 eV was experimentally determined. The initial data include measurements of the transmittance of two free-standing Be films with thicknesses of 70 nm and 152 nm, as well as reflectometric measurements of similar films on a substrate. Measurements were carried out at the optics beamline of the BESSY II synchrotron radiation source. The absorption coefficient β was found directly from the transmission coefficient of the films, and the real part of the polarizability δ was calculated from the Kramers–Kronig relations. A comparison is carried out with results obtained 20 years ago at the ALS synchrotron using a similar methodology.


It is a matter of common knowledge that an ordinary gold leaf apperars green by transmitted light while silver leaf appears blue. Faraday found that the gold leaf lost all its colour if heated on glass. T. Turner found that this change occurs at about 550° C. in the case of gold and about 240° C. in the case of silver. Faraday obtained thinner films from the "deflagration" of gold wire by the discharge of a Leyden jar battery. These were red and violet in places and green in others. They turned red on heating, but the green colour could be brought back by rubbing with a rounded piece of agate. The gold films used by Beilby, obtained from paints used for ceramic gilding, behaved in a similar manner. One of his thin purple films turned rose-pink on annealing, and his thicker green films became transparent at a temperature above 400°C. R. W. Wood obtained purple, blue and green films of gold by sputtering. He found that films of all other colours could be turned green by heating, as opposed to Faraday and Beilby. Maxwell Garnett has explained the colours observed by Beilby, Faraday and R. W. Wood by considering the films as made up of minute spherical particles of metal. He finds that the transmission-coefficient T, of films for which πd/λ is very small, is given by T = 1 - 4π dn 2 k /λ, where d is the thickness of the film, k the absorption coefficient, n the refractive index, and λ the wave-length of the light used.


2021 ◽  
Vol 3 (1) ◽  
pp. 221-228
Author(s):  
Taat Guswantoro

The phenomenon of total internal reflection can be used to guide the light to be transmitted from one place to another, it is applied to the guiding principle of light in fiber optics. A fiber rope made of clear plastic material with a uniform refractive index, when one end fired a beam of light then the light will be forwarded along the strap so that out at the other end. This principle can be applied as a lighting source in a closed room by passing light from the outdoors by using plastic fiber, so it doesn’t need the electricity. In this study, theoretical analysis of the percentage of the intensity of light transmitted by the fiber plastic succeed as a function of the refractive index and determine the transmission coefficient for some plastic seeds are eligible to be used as a plastic fiber light successor. From the results of deriving the equation, the light transmission coefficient of plastic is  and the terms of plastic seeds that can be used as a plastic fiber are having a refractive index . Based on refractive index data from profesionalplastics, the maximum transmission coefficient value for Ethylene Tetrafluoro Ethylene Copolymer is 82.23% and the minimum transmission value of Fluorinated Ethylene Propylene Copolymer is 55.99%.


2015 ◽  
Vol 05 (01) ◽  
pp. 15-27 ◽  
Author(s):  
Alexander V. Kir’yanov ◽  
Nikolai N. Il’ichev ◽  
Elmira S. Gulyamova ◽  
Alexander S. Nasibov ◽  
Peter V. Shapkin

1976 ◽  
Vol 3 (1) ◽  
pp. 35-38 ◽  
Author(s):  
Michael A. Dopita ◽  
John A. Hart

Fabry-Perot instruments have been extensively used for many years for the study of spatially extended emission nebulae because they offer a potential luminosity resolution product (L × Rpot) which exceeds by a high factor tha attainable by aerating spectrometer. Meaburn (1970) shows that this product is given by the relation where P is the number of resolution elements each containing a maximum solid angle, Ω observed simultaneously, ti is the refractive index of the medium between the plates, A is the acceptance area of the device, εo is the transmission coefficient of the associated optics and εF the transmission coefficient of the Fabry-Perot (which if coated with dielectric multilayers can be very high).


Author(s):  
W. E. Lee

An optical waveguide consists of a several-micron wide channel with a slightly different index of refraction than the host substrate; light can be trapped in the channel by total internal reflection.Optical waveguides can be formed from single-crystal LiNbO3 using the proton exhange technique. In this technique, polished specimens are masked with polycrystal1ine chromium in such a way as to leave 3-13 μm wide channels. These are held in benzoic acid at 249°C for 5 minutes allowing protons to exchange for lithium ions within the channels causing an increase in the refractive index of the channel and creating the waveguide. Unfortunately, optical measurements often reveal a loss in waveguiding ability up to several weeks after exchange.


Author(s):  
Walter C. McCrone

An excellent chapter on this subject by V.D. Fréchette appeared in a book edited by L.L. Hench and R.W. Gould in 1971 (1). That chapter with the references cited there provides a very complete coverage of the subject. I will add a more complete coverage of an important polarized light microscope (PLM) technique developed more recently (2). Dispersion staining is based on refractive index and its variation with wavelength (dispersion of index). A particle of, say almandite, a garnet, has refractive indices of nF = 1.789 nm, nD = 1.780 nm and nC = 1.775 nm. A Cargille refractive index liquid having nD = 1.780 nm will have nF = 1.810 and nC = 1.768 nm. Almandite grains will disappear in that liquid when observed with a beam of 589 nm light (D-line), but it will have a lower refractive index than that liquid with 486 nm light (F-line), and a higher index than that liquid with 656 nm light (C-line).


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