X-Ray Imaging Characteristics Of The Vacuum-Demountable Microchannel Spatial Light Modulator

1986 ◽  
Vol 25 (2) ◽  
pp. 252269 ◽  
Author(s):  
Robert F. Dillon ◽  
Cardinal Warde
2001 ◽  
Vol 72 (1) ◽  
pp. 1248-1248 ◽  
Author(s):  
S. G. Lee ◽  
J. G. Bak ◽  
H. G. Lee ◽  
M. Kwon ◽  
M. Bitter ◽  
...  

1991 ◽  
Author(s):  
Oberto Citterio ◽  
Paolo Conconi ◽  
Giancarlo Conti ◽  
E. Mattaini ◽  
E. Santambrogio ◽  
...  

2002 ◽  
Vol 738 ◽  
Author(s):  
R.P. Raffaelle ◽  
T. Gennett ◽  
J. E. Lau ◽  
P. Jenkins ◽  
S.L. Castro ◽  
...  

ABSTRACTThe ability to determine the in-situ optoelectronic behavior of semiconductor materials has become especially important as the size of device architectures is reduced and the development of complex microsystems has increased. Scanning Tunneling Optical Resonance Microscopy or STORM has the ability to interrogate the optical bandgap as a function of position within a semiconductor microstructure. This technique uses a tunable solid-state Ti sapphire laser whose output is “chopped” using a spatial light modulator and is coupled by a fiber optic to a scanning tunneling microscope in order to illuminate the tip-sample junction. The photoenhanced portion of the tunneling current is spectroscopically measured using a lock-in technique. The capabilities of this technique were verified using semiconductor microstructure calibration standards that were grown by organometallic vapor phase epitaxy (OMVPE) at the NASA Glenn Research Center. Bandgaps characterized by STORM measurements were found to be in good agreement with the bulk values determined by transmission spectroscopy, photoluminescence, and with the theoretical values that were based on x-ray diffraction results.


1997 ◽  
Author(s):  
Brian Rodricks ◽  
Denny L. Lee ◽  
Lawrence K. Cheung ◽  
Lothar S. Jeromin ◽  
Eugene F. Palecki

Open Physics ◽  
2018 ◽  
Vol 16 (1) ◽  
pp. 751-756
Author(s):  
Zhao Lingling ◽  
Jon Knepper

AbstractIn the last 20 years, requirements for x-ray lithography, space technology and ICF process diagnosis, the x-ray imaging technology has been developed. However, x-ray imaging turns out to be more difficult due to intense absorption of x-rays, and the refractive index of x band is slightly less than 1. Normal imaging method may not be suitable for x-ray band. At present, grazing reflective imaging and coded aperture imaging are commonly used for this band. This paper presents a detailed analysis of the imaging characteristics of single-mirror and double-mirror. Then the focal distance, field obliquity and aperture position of the mirrors of the KBA microscopes at grazing incidence are studied. The results show that the structure arrangement of the KBA microscope is rather reasonable, and can be considered as theoretical evidence in the design and manufacture of KBA microscopes.


1994 ◽  
Author(s):  
Giancarlo Conti ◽  
E. Mattaini ◽  
E. Santambrogio ◽  
Bruno Sacco ◽  
Giancarlo Cusumano ◽  
...  

Author(s):  
M.G. Baldini ◽  
S. Morinaga ◽  
D. Minasian ◽  
R. Feder ◽  
D. Sayre ◽  
...  

Contact X-ray imaging is presently developing as an important imaging technique in cell biology. Our recent studies on human platelets have demonstrated that the cytoskeleton of these cells contains photondense structures which can preferentially be imaged by soft X-ray imaging. Our present research has dealt with platelet activation, i.e., the complex phenomena which precede platelet appregation and are associated with profound changes in platelet cytoskeleton. Human platelets suspended in plasma were used. Whole cell mounts were fixed and dehydrated, then exposed to a stationary source of soft X-rays as previously described. Developed replicas and respective grids were studied by scanning electron microscopy (SEM).


Author(s):  
James F. Mancuso ◽  
William B. Maxwell ◽  
Russell E. Camp ◽  
Mark H. Ellisman

The imaging requirements for 1000 line CCD camera systems include resolution, sensitivity, and field of view. In electronic camera systems these characteristics are determined primarily by the performance of the electro-optic interface. This component converts the electron image into a light image which is ultimately received by a camera sensor.Light production in the interface occurs when high energy electrons strike a phosphor or scintillator. Resolution is limited by electron scattering and absorption. For a constant resolution, more energy deposition occurs in denser phosphors (Figure 1). In this respect, high density x-ray phosphors such as Gd2O2S are better than ZnS based cathode ray tube phosphors. Scintillating fiber optics can be used instead of a discrete phosphor layer. The resolution of scintillating fiber optics that are used in x-ray imaging exceed 20 1p/mm and can be made very large. An example of a digital TEM image using a scintillating fiber optic plate is shown in Figure 2.


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