A multi-ring phosphor convertor with gradient concentration for improving the thermal uniformity in a laser illumination system

Author(s):  
Yi Yang ◽  
Xuewei Du ◽  
Mu Li ◽  
Bin Liu ◽  
Binhai Yu ◽  
...  
1997 ◽  
Vol 3 (S2) ◽  
pp. 807-808
Author(s):  
J.M. Fernandez

A rapid Ca++ signal is known to be the main trigger for exocytosis in excitable cells. However, its mode of action is unknown. Recently, it has become clear that the spatial distribution of a Ca++ stimulus is important for exocytosis. To investigate this question we have developed a novel instrument capable of imaging Ca++ gradients in patch clamped cells. We have equipped a standard fluorescence microscope with a CCD camera and an image processing station. This combination can generate a thin section view of the fluorescence of a single cell. We have equipped this microscope with a pulsed laser illumination system. The distribution of intracellular calcium can be obtained by exciting the Ca++ indicator dye (e.g., rhod-2) with a brief laser pulse [300 ns long at 525 nm ], then an image can be formed with the light emitted by the dye. by synchronizing the laser pulse with a depolarizing stimulus in a patch-clamped chromaffin cell loaded with the fluorescent Ca++ indicator rhod-2, we could easily obtain snapshots of the Ca++ distribution at known times after a stimulus.


1965 ◽  
Vol 2 (1) ◽  
pp. 56-58
Author(s):  
A. A. Kaminskii ◽  
L. S. Kornienko

1994 ◽  
Vol 48 (10) ◽  
pp. 1277-1281 ◽  
Author(s):  
David M. Pallister ◽  
Michael D. Morris

A comparison of microscopic Raman images acquired with an optical-fiber critical (Nelson) illumination system, an optical-fiber Koehler laser illumination system, and Koehler laser illumination without an optical fiber demonstrates performance differences between the three illumination methods. Best images are obtained with optical-fiber Koehler illumination.


Author(s):  
E. A. Kenik ◽  
J. Bentley

Cliff and Lorimer (1) have proposed a simple approach to thin foil x-ray analy sis based on the ratio of x-ray peak intensities. However, there are several experimental pitfalls which must be recognized in obtaining the desired x-ray intensities. Undesirable x-ray induced fluorescence of the specimen can result from various mechanisms and leads to x-ray intensities not characteristic of electron excitation and further results in incorrect intensity ratios.In measuring the x-ray intensity ratio for NiAl as a function of foil thickness, Zaluzec and Fraser (2) found the ratio was not constant for thicknesses where absorption could be neglected. They demonstrated that this effect originated from x-ray induced fluorescence by blocking the beam with lead foil. The primary x-rays arise in the illumination system and result in varying intensity ratios and a finite x-ray spectrum even when the specimen is not intercepting the electron beam, an ‘in-hole’ spectrum. We have developed a second technique for detecting x-ray induced fluorescence based on the magnitude of the ‘in-hole’ spectrum with different filament emission currents and condenser apertures.


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