Three-Dimensional Evaluation of Paper Surfaces Using Confocal Microscopy

2020 ◽  
pp. 1-40 ◽  
Author(s):  
Marie-Claude Béland ◽  
Patrice J. Mangin
Author(s):  
J. Holy ◽  
G. Schatten

One of the classic limitations of light microscopy has been the fact that three dimensional biological events could only be visualized in two dimensions. Recently, this shortcoming has been overcome by combining the technologies of laser scanning confocal microscopy (LSCM) and computer processing of microscopical data by volume rendering methods. We have employed these techniques to examine morphogenetic events characterizing early development of sea urchin embryos. Specifically, the fourth cleavage division was examined because it is at this point that the first morphological signs of cell differentiation appear, manifested in the production of macromeres and micromeres by unequally dividing vegetal blastomeres.The mitotic spindle within vegetal blastomeres undergoing unequal cleavage are highly polarized and develop specialized, flattened asters toward the micromere pole. In order to reconstruct the three-dimensional features of these spindles, both isolated spindles and intact, extracted embryos were fluorescently labeled with antibodies directed against either centrosomes or tubulin.


1997 ◽  
Vol 3 (S2) ◽  
pp. 305-306
Author(s):  
David W. Piston

Two-photon excitation microscopy (TPEM) provides attractive advantages over confocal microscopy for three-dimensionally resolved fluorescence imaging and photochemistry. It provides three-dimensional resolution and eliminates background equivalent to an ideal confocal microscope without requiring a confocal spatial filter, whose absence enhances fluorescence collection efficiency. This results in inherent submicron optical sectioning by excitation alone. In practice, TPEM is made possible by the very high local instantaneous intensity provided by a combination of diffraction-limited focusing of a single laser beam in the microscope and the temporal concentration of 100 femtosecond pulses generated by a mode-locked laser. Resultant peak excitation intensities are 106 times greater than the CW intensities used in confocal microscopy, but the pulse duty cycle of 10−5 limits the average input power to less than 10 mW, only slightly greater than the power normally used in confocal microscopy. Because of the intensity-squared dependence of the two-photon absorption, the excitation is limited to the focal volume.


Langmuir ◽  
2015 ◽  
Vol 31 (35) ◽  
pp. 9684-9693 ◽  
Author(s):  
Donghee Lee ◽  
Md. Mahmudur Rahman ◽  
You Zhou ◽  
Sangjin Ryu

2016 ◽  
Vol 41 (9) ◽  
pp. 2013 ◽  
Author(s):  
Baoliang Ge ◽  
Yifan Wang ◽  
Yujia Huang ◽  
Cuifang Kuang ◽  
Yue Fang ◽  
...  

1994 ◽  
Vol 16 (1) ◽  
pp. 44-51 ◽  
Author(s):  
Stephen E. Mahoney ◽  
Stephen W. Paddock ◽  
Louis C. Smith ◽  
Dorothy E. Lewis ◽  
Madeleine Duvic

2010 ◽  
Vol 8 (3) ◽  
pp. 120-128 ◽  
Author(s):  
Glen H. MacDonald ◽  
Edwin W Rubel

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