scholarly journals Refractive Index Imaging of Cells with Variable-Angle Near-Total Internal Reflection (TIR) Microscopy

2017 ◽  
Vol 23 (5) ◽  
pp. 978-988 ◽  
Author(s):  
Kevin P. Bohannon ◽  
Ronald W. Holz ◽  
Daniel Axelrod

AbstractThe refractive index in the interior of single cells affects the evanescent field depth in quantitative studies using total internal reflection (TIR) fluorescence, but often that index is not well known. We here present method to measure and spatially map the absolute index of refraction in a microscopic sample, by imaging a collimated light beam reflected from the substrate/buffer/cell interference at variable angles of incidence. Above the TIR critical angle (which is a strong function of refractive index), the reflection is 100%, but in the immediate sub-critical angle zone, the reflection intensity is a very strong ascending function of incidence angle. By analyzing the angular position of that edge at each location in the field of view, the local refractive index can be estimated. In addition, by analyzing the steepness of the edge, the distance-to-substrate can be determined. We apply the technique to liquid calibration samples, silica beads, cultured Chinese hamster ovary cells, and primary culture chromaffin cells. The optical technique suffers from decremented lateral resolution, scattering, and interference artifacts. However, it still provides reasonable results for both refractive index (~1.38) and for distance-to-substrate (~150 nm) for the cells, as well as a lateral resolution to about 1 µm.

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.


1997 ◽  
Vol 51 (10) ◽  
pp. 1554-1558 ◽  
Author(s):  
Robert Altkorn ◽  
Ilia Koev ◽  
Amos Gottlieb

We describe a waveguide capillary cell based on a fused-silica tube coated externally with a thin layer of a low-refractive-index ( n = 1.31) fluoropolymer. When filled with a transparent liquid of refractive index greater than that of the fluoropolymer, the cell is capable of transmitting light through total internal reflection. Loss below 1 dB/m is demonstrated throughout much of the visible region for a 530-μm-i.d., 660-μm-o.d. cell filled with water.


2021 ◽  
Vol 60 (10) ◽  
pp. B106
Author(s):  
Ju-Yi Lee ◽  
Chia-Yu Chiang ◽  
Wei-Yi Sung ◽  
Tzu-Yang Weng ◽  
Jing-Heng Chen ◽  
...  

2015 ◽  
Vol 51 (5) ◽  
pp. 945-947 ◽  
Author(s):  
Seungah Lee ◽  
Hyunung Yu ◽  
Seong Ho Kang

The total internal reflection scattering system incorporating a z-nanopositioner is introduced to explore the precise immunoassay on gold-nanopattemed chips by lateral resolution improvement.


Nanoscale ◽  
2014 ◽  
Vol 6 (14) ◽  
pp. 8177-8184 ◽  
Author(s):  
Peng Mao ◽  
Fangfang Sun ◽  
Hanchao Yao ◽  
Jing Chen ◽  
Bo Zhao ◽  
...  

Porous TiO2nanoparticle layers are fabricated by gas phase cluster beam deposition at glancing incidence.


Author(s):  
John William Evans

Certain optical properties of crystals, and more particularly the refractive index, may be determined either in the directions-image, often referred to as the 'image in convergent light', or in the ordinary object-image in which the object itself is seen. In the former case, in which the index of refraction is 'usually determined by means of the critical angle of total-reflection, every point in the image corresponds to a single direction of propagation of the wave-front through the crystal-structure and to the two corresponding directions of vibration. One of these can, however, be eliminated by the insertion of a nicol in an approximate position, and thus all ambiguity in the determination of the refractive index is removed.


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