Refractive Indices of Lithium Fluoride and Fused Silica from 2000 to 3000 Å

1965 ◽  
Vol 55 (4) ◽  
pp. 453 ◽  
Author(s):  
H. G. Jerrard ◽  
J. Turpin

The present work forms a continuation of an enquiry begun by Mr. C. Cuthbertson on the refractive indices of the vapours of elements not gaseous at ordinary temperatures. The refractometer of Jamin was again employed, but tubes of fused silica were now used and other improvements introduced.


2019 ◽  
Vol 3 (4) ◽  
pp. 21-29
Author(s):  
Zaheer Hussain Shah ◽  
Imtiaz Ahmad ◽  
Rabia Nasar

In the present work the refractive indices of thermally evaporated films of cadmium sulfide (CdS) on fused silica substrates were obtained from measurement of transmittance (T, alone) at normal incidence. Earlier, the same were determined by using measurements of reflectance (R) and transmittance (T) again at normal incidence. On comparison of the two results, we noted that the present results are in fact more, closer than those obtained earlier to the corresponding values reported for the bulk cadmium sulfide.


2006 ◽  
Vol 23 (2) ◽  
pp. 302-313 ◽  
Author(s):  
Giuseppe Zibordi

Abstract The spectral immersion factor of in-water radiance sensors If quantifies the effects of changes in the sensor's response when operated in water versus in air. The values of If are currently computed with a relationship derived from a basic sensor model, which only requires knowledge of the refractive indices of the water and the material constituting the sensor's optical window in contact herewith. Uncertainties in the computation of If are investigated in the 400–700-nm spectral range for a specific class of widely used multispectral radiometers. The analysis is made by comparing If values from the theoretical relationship currently in use with (i) If from a new relationship based on an extended sensor model accounting for the actual solid-angle field of view and the reflectance and transmittance of the external and internal optical components, and (ii) experimental If determined with sample radiometers having diverse optical windows made of materials with different refractive indices. Results highlight that the relationship derived from the basic sensor model introduces a 0.4% negative bias when applied to the considered class of radiometers having a fused silica optical window, a 13° in-air half-angle field of view, and an estimated detector reflectance of 0.15. Reference values of If for the specific class of radiometers, determined with the newly proposed relationship, are presented, and their dependence on seawater temperature and salinity is discussed.


1998 ◽  
Vol 37 (25) ◽  
pp. 5964 ◽  
Author(s):  
Rajeev Gupta ◽  
John H. Burnett ◽  
Ulf Griesmann ◽  
Matthew Walhout

Although numerous accurate and extended determinations have been made of the refractive indices of gases which exist as such at ordinary temperatures, few have been made with the vapours of elements or compounds which, at room temperatures, are solids and possess a low equilibrium vapour pressure in that state. Notable among the latter are the determinations made by Prof. R. W. Wood with sodium vapour and those made by Messrs. C. Cuthbertson and E. Parr Metcalfe with the vapours of sulphur, phosphorus, mercury, zinc, cadmium, selenium, and tellurium. In the work of both of these investigations an interference method was adopted. In Wood’s a Michelson interferometer was used and in Cuthbertson and Metcalfe’s one of the Jamin type. For the investigation of Cuthbertson and Metcalfe the glass interferometer tubes ordinarily used with Jamin interferometers were wholly unsuitable. These, as is well known, are provided with plane parallel plate glass ends ground in and luted with shellac or a wax having similar properties, and when heated to 300°C. or higher, the shellac chars and the tubes frequently crack, soften or become distorted. For these reasons Cuthbertson and Metcalfe had recourse to interferometer tubes made of fused silica which were made, with great skill, by Messrs. Heraeus, of Hanau. The ends of the tubes through which the interfering rays passed were plates of quartz ground optically flat, fused into the tubes and again polished. In their manufacture such tubes are, however, difficult to make. Failures are frequent and consequently the tubes are expensive. On this account investigators have been deterred hitherto from studying the refractivities of the vapours of metals and other substances, having moderately high melting points and vapourising temperatures.


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