Joint transform correlator subtracting a modified Fourier spectrum

1995 ◽  
Vol 34 (32) ◽  
pp. 7532 ◽  
Author(s):  
Martin Schönleber ◽  
Gregor Cedilnik ◽  
Hans-J. Tiziani
Author(s):  
Hannes Lichte ◽  
Edgar Voelkl

The object wave o(x,y) = a(x,y)exp(iφ(x,y)) at the exit face of the specimen is described by two real functions, i.e. amplitude a(x,y) and phase φ(x,y). In stead of o(x,y), however, in conventional transmission electron microscopy one records only the real intensity I(x,y) of the image wave b(x,y) loosing the image phase. In addition, referred to the object wave, b(x,y) is heavily distorted by the aberrations of the microscope giving rise to loss of resolution. Dealing with strong objects, a unique interpretation of the micrograph in terms of amplitude and phase of the object is not possible. According to Gabor, holography helps in that it records the image wave completely by both amplitude and phase. Subsequently, by means of a numerical reconstruction procedure, b(x,y) is deconvoluted from aberrations to retrieve o(x,y). Likewise, the Fourier spectrum of the object wave is at hand. Without the restrictions sketched above, the investigation of the object can be performed by different reconstruction procedures on one hologram. The holograms were taken by means of a Philips EM420-FEG with an electron biprism at 100 kV.


2010 ◽  
Vol 30 (8) ◽  
pp. 2094-2097 ◽  
Author(s):  
Xin-ming ZHANG ◽  
Shuang LI ◽  
Yan-bin ZHENG ◽  
Hui-yun ZHANG

2015 ◽  
Author(s):  
Paheding Sidike ◽  
Vijayan K. Asari ◽  
Mohammad S. Alam

1994 ◽  
Vol 41 (6) ◽  
pp. 1253-1261
Author(s):  
B.S. Lowans ◽  
B. Bates ◽  
R.G.H. Greer

Optik ◽  
2021 ◽  
pp. 167654
Author(s):  
Qi Chen ◽  
Xueju Shen ◽  
Yue Cheng ◽  
Chao Lin ◽  
Yunfeng Liu ◽  
...  

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