An electron beam lithography and digital image acquisition system for scanning electron microscopes

2007 ◽  
Vol 226 (1) ◽  
pp. 64-70 ◽  
Author(s):  
S. RUSSEV ◽  
G. TSUTSUMANOVA ◽  
S. ANGELOV ◽  
K. BACHEV
1995 ◽  
Vol 66 (2) ◽  
pp. 1151-1153 ◽  
Author(s):  
W. M. Ang ◽  
Terry McMahon ◽  
Don Schulte ◽  
Leon Ungier

Author(s):  
Klaus-Ruediger Peters ◽  
William H. Martin ◽  
Eisaku Oho

Digital image acquisition and display of field emission scanning electron micrographs face limitations in terms of detail recognition, sampling of high resolution information, image output and storage space for high pixel density images. The image acquisition and image output of a JEOL JSEM-890 “in lens” field emission SEM were digitized and several approaches for adequate access to the scanned electron probe data have been developed. Images are acquired digitally in 3×4 VGA format (in multiples of 640×490 pixels) and stored in a RECOGNITION CONCEPTS INC. image processor (Trapix Plus). The images are displayed on workstation monitors with 1280×1024 format (HITACHI CM2085MU), and image documentation is done by several techniques of varying output quality. Low quality image documentation on plain paper can be obtained using a laser jet printer (HEWLETT PACKARD: Laser Jet III). High quality output is provided by a video printer utilizing special but inexpensive paper (SEIKOSHA VP350H). In addition, conventional analog CRT output and CRT photography on 4×5 inch POLAROID (Type 55 Positive/Negative) film is used.


2006 ◽  
Vol 51 (20) ◽  
pp. 5089-5103 ◽  
Author(s):  
Gina M Clarke ◽  
Chris Peressotti ◽  
Gordon E Mawdsley ◽  
Martin J Yaffe

MRS Bulletin ◽  
1991 ◽  
Vol 16 (3) ◽  
pp. 41-45 ◽  
Author(s):  
K. Sujata ◽  
Hamlin M. Jennings

Scanning electron microscopes offer several unique advantages and they have evolved into complex integrated instruments that often incorporate several important accessories. Their principle advantage stems from the method of constructing an image from a highly focused electron beam that scans across the surface of a specimen. The beam generates backscattered electrons and excites secondary electrons and x-rays in a highly localized “spot.” These signals can be detected, and the results of the analysis are displayed as a specific intensity on a screen at a position that represents the position of the electron spot. As with a television image, after a given period, information about the entire field of view is displayed on the screen, resulting in a complete image. If the specimen is thin, the same type of information can be gathered from the transmitted electrons, and a scanning transmission image is thus constructed.The scanning electron microscope is highly versatile and widely used. The quality of the image is related to its resolution and contrast, which, in turn, depend on the diameter of the focused beam as well as its energy and current. Because electron lenses have inherently high aberrations, the usable aperture angles are much smaller than in a light microscope and, therefore, the electron beam remains focused over a relatively large distance, giving these instruments a very large depth of focus.Scanning electron microscopes are versatile in their ability to detect and analyze a lot of information. As a result, modern versions of these instruments are equipped with a number of detectors. Developments are sometimes related to placing the detectors in a geometrically attractive position close to the specimen.


1993 ◽  
Vol 1 (4) ◽  
pp. 16-17
Author(s):  
Doug Rathkey

Over the years, we've seen major developments in electron source technologies in response to the demands for better performance. This article presents a brief overview of the cathode technologies in use today.Two types of electron sources are used in commercially available scanning electron microscopes (SEMs), transmission electron microscopes (TEMs), scanning Auger microprobes, and electron beam lithography systems: thermionic and field emission electron cathodes. Thermionic cathodes reiease electrons from the cathode material when they are heated while field emission cathodes rely on a high electric field to draw electrons from the cathode material.


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