Acoustic field structure simulation in quasi-collinear acousto-optic cells with ultrasound beam reflection

Ultrasonics ◽  
2017 ◽  
Vol 78 ◽  
pp. 175-184 ◽  
Author(s):  
S.N. Mantsevich ◽  
V.Ya. Molchanov ◽  
K.B. Yushkov ◽  
V.S. Khorkin ◽  
M.I. Kupreychik
2017 ◽  
Vol 141 (5) ◽  
pp. 3810-3810
Author(s):  
Sergey Mantsevich ◽  
Vladimir Balakshy ◽  
Vladimir Molchanov ◽  
Konstantin Yushkov

2000 ◽  
Vol 46 (3) ◽  
pp. 274-283 ◽  
Author(s):  
O. P. Galkin ◽  
E. A. Kharchenko ◽  
L. V. Shvachko

Author(s):  
H. Banzhof ◽  
I. Daberkow

A Philips EM 420 electron microscope equipped with a field emission gun and an external STEM unit was used to compare images of single crystal surfaces taken by conventional reflection electron microscopy (REM) and scanning reflection electron microscopy (SREM). In addition an angle-resolving detector system developed by Daberkow and Herrmann was used to record SREM images with the detector shape adjusted to different details of the convergent beam reflection high energy electron diffraction (CBRHEED) pattern.Platinum single crystal spheres with smooth facets, prepared by melting a thin Pt wire in an oxyhydrogen flame, served as objects. Fig. 1 gives a conventional REM image of a (111)Pt single crystal surface, while Fig. 2 shows a SREM record of the same area. Both images were taken with the (555) reflection near the azimuth. A comparison shows that the contrast effects of atomic steps are similar for both techniques, although the depth of focus of the SREM image is reduced as a result of the large illuminating aperture. But differences are observed at the lengthened images of small depressions and protrusions formed by atomic steps, which give a symmetrical contrast profile in the REM image, while an asymmetric black-white contrast is observed in the SREM micrograph. Furthermore the irregular structures which may be seen in the middle of Fig. 2 are not visible in the REM image, although it was taken after the SREM record.


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