[10] Construction of line-scan confocal microscope for physiological recording

Author(s):  
Nick Callamaras ◽  
Ian Parker
2010 ◽  
Vol 98 (3) ◽  
pp. 179a-180a ◽  
Author(s):  
Zhaonian Zhang ◽  
Yong Wu ◽  
Pedro Felipe ◽  
Gardeazábal Rodríguez ◽  
Hui Zhao ◽  
...  

Author(s):  
P.E. Batson ◽  
C.R.M. Grovenor ◽  
D.A. Smith ◽  
C. Wong

In this work As doped polysilicon was deposited onto (100) silicon wafers by APCVD at 660°C from a silane-arsine mixture, followed by a ten minute anneal at 1000°C, and in one case a further ten minute anneal at 700°C. Specimens for TEM and STEM analysis were prepared by chemical polishing. The microstructure, which is unchanged by the final 700°C anneal,is shown in Figure 1. It consists of numerous randomly oriented grains many of which contain twins.X-ray analysis was carried out in a VG HB5 STEM. As K α x-ray counts were collected from STEM scans across grain and twin boundaries, Figures 2-4. The incident beam size was about 1.5nm in diameter, and each of the 20 channels in the plots was sampled from a 1.6nm length of the approximately 30nm line scan across the boundary. The bright field image profile along the scanned line was monitored during the analysis to allow correlation between the image and the x-ray signal.


Author(s):  
C J R Sheppard

The confocal microscope is now widely used in both biomedical and industrial applications for imaging, in three dimensions, objects with appreciable depth. There are now a range of different microscopes on the market, which have adopted a variety of different designs. The aim of this paper is to explore the effects on imaging performance of design parameters including the method of scanning, the type of detector, and the size and shape of the confocal aperture.It is becoming apparent that there is no such thing as an ideal confocal microscope: all systems have limitations and the best compromise depends on what the microscope is used for and how it is used. The most important compromise at present is between image quality and speed of scanning, which is particularly apparent when imaging with very weak signals. If great speed is not of importance, then the fundamental limitation for fluorescence imaging is the detection of sufficient numbers of photons before the fluorochrome bleaches.


2005 ◽  
Vol 43 (05) ◽  
Author(s):  
M Goetz ◽  
MF Neurath ◽  
P Delaney ◽  
S Gregor ◽  
D Strand ◽  
...  
Keyword(s):  

2017 ◽  
Vol 61 (3) ◽  
pp. 305031-3050311 ◽  
Author(s):  
Timo Eckhard ◽  
Jia Eckhard ◽  
Eva M. Valero ◽  
Javier Hernández-Andrés
Keyword(s):  
B Spline ◽  

2015 ◽  
Vol 57 (11-12) ◽  
pp. 985-991
Author(s):  
Andreas Kupsch ◽  
Axel Lange ◽  
Manfred P. Hentschel ◽  
Gerd-Rüdiger Jaenisch ◽  
Nikolay Kardjilov ◽  
...  
Keyword(s):  
X Ray ◽  

2007 ◽  
Vol 227 (3) ◽  
pp. 203-215 ◽  
Author(s):  
J. H. FRANK ◽  
A. D. ELDER ◽  
J. SWARTLING ◽  
A. R. VENKITARAMAN ◽  
A. D. JEYASEKHARAN ◽  
...  

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