scholarly journals Wide-field Fourier ptychographic microscopy using laser illumination source

2016 ◽  
Vol 7 (11) ◽  
pp. 4787 ◽  
Author(s):  
Jaebum Chung ◽  
Hangwen Lu ◽  
Xiaoze Ou ◽  
Haojiang Zhou ◽  
Changhuei Yang
2007 ◽  
Author(s):  
Phil Surman ◽  
Ian Sexton ◽  
Klaus Hopf ◽  
Richard Bates ◽  
Wing Kai Lee ◽  
...  

2017 ◽  
Vol 8 (11) ◽  
pp. 4798 ◽  
Author(s):  
Yuri Lysov ◽  
Victor Barsky ◽  
Dmitriy Urasov ◽  
Roman Urasov ◽  
Alecksey Cherepanov ◽  
...  

2000 ◽  
Vol 197 (1) ◽  
pp. 1-4 ◽  
Author(s):  
Neil ◽  
Squire ◽  
Juskaitis ◽  
Bastiaens ◽  
Wilson

1996 ◽  
Author(s):  
Mi K. Hong ◽  
Shyamsunder Erramilli ◽  
Philip Huie ◽  
Gregory E. James ◽  
Andrew G. Jeung

Author(s):  
M. G. Lagally

It has been recognized since the earliest days of crystal growth that kinetic processes of all Kinds control the nature of the growth. As the technology of crystal growth has become ever more refined, with the advent of such atomistic processes as molecular beam epitaxy, chemical vapor deposition, sputter deposition, and plasma enhanced techniques for the creation of “crystals” as little as one or a few atomic layers thick, multilayer structures, and novel materials combinations, the need to understand the mechanisms controlling the growth process is becoming more critical. Unfortunately, available techniques have not lent themselves well to obtaining a truly microscopic picture of such processes. Because of its atomic resolution on the one hand, and the achievable wide field of view on the other (of the order of micrometers) scanning tunneling microscopy (STM) gives us this opportunity. In this talk, we briefly review the types of growth kinetics measurements that can be made using STM. The use of STM for studies of kinetics is one of the more recent applications of what is itself still a very young field.


Author(s):  
J. Barbillat ◽  
M. Delhaye ◽  
P. Dhamelincourt

Raman mapping, with a spatial resolution close to the diffraction limit, can help to reveal the distribution of chemical species at the surface of an heterogeneous sample.As early as 1975,three methods of sample laser illumination and detector configuration have been proposed to perform Raman mapping at the microscopic level (Fig. 1),:- Point illumination:The basic design of the instrument is a classical Raman microprobe equipped with a PM tube or either a linear photodiode array or a two-dimensional CCD detector. A laser beam is focused on a very small area ,close to the diffraction limit.In order to explore the whole surface of the sample,the specimen is moved sequentially beneath the microscope by means of a motorized XY stage. For each point analyzed, a complete spectrum is obtained from which spectral information of interest is extracted for Raman image reconstruction.- Line illuminationA narrow laser line is focused onto the sample either by a cylindrical lens or by a scanning device and is optically conjugated with the entrance slit of the stigmatic spectrograph.


Author(s):  
Van B. Nakagawara ◽  
Ronald W. Montgomery ◽  
Archie E. Dillard ◽  
Leon N. McLin ◽  
C. William Connor

2013 ◽  
Vol 183 (8) ◽  
pp. 888-894
Author(s):  
G.M. Beskin ◽  
S.V. Karpov ◽  
V.L. Plokhotnichenko ◽  
S.F. Bondar ◽  
A.V. Perkov ◽  
...  

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