Theory and use of in-line refractive index analyzers for improved process control

Author(s):  
J.G. Groetsch
2015 ◽  
Vol 2015 ◽  
pp. 1-5 ◽  
Author(s):  
Xianfang Gou ◽  
Xiaoyan Li ◽  
Su Zhou ◽  
Shaoliang Wang ◽  
Weitao Fan ◽  
...  

Voltage bias of several hundred volts which are applied between solar cells and module frames may lead to significant power losses, so-called potential-induced degradation (PID), in normal photovoltaic (PV) installations system. Modules and minimodules are used to conduct PID test of solar cells. The test procedure is time consuming and of high cost, which cannot be used as process monitoring method during solar cells fabrication. In this paper, three kinds of test including minimodule,Rsh, and V-Q test are conducted on solar cells or wafers with SiNxof different refractive index. All comparisons between test results ofRsh, V-Q, and minimodule tests have shown equal results. It is shown thatRshtest can be used as quality inspection of solar cells and V-Q test of coated wafer can be used as process control of solar cells.


1994 ◽  
Author(s):  
Johannes K. Schaller ◽  
S. Wassenberg ◽  
Detlev K. Fiedler ◽  
Christo G. Stojanoff

1959 ◽  
Vol 51 (11) ◽  
pp. 69A-70A
Author(s):  
R. F. Wall

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).


1956 ◽  
Vol 48 (2) ◽  
pp. 81-84
Author(s):  
William Priestley ◽  
B. Dudenbostel, Jr.

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