scholarly journals New Type of Intensity Correlation in Random Media

1999 ◽  
Vol 83 (23) ◽  
pp. 4733-4735 ◽  
Author(s):  
B. Shapiro
2000 ◽  
Vol 62 (5) ◽  
pp. 7348-7352 ◽  
Author(s):  
P. Sebbah ◽  
R. Pnini ◽  
A. Z. Genack

1991 ◽  
Vol 157 (4-5) ◽  
pp. 265-269 ◽  
Author(s):  
R. Pnini ◽  
B. Shapiro

1990 ◽  
Vol 65 (17) ◽  
pp. 2129-2132 ◽  
Author(s):  
A. Z. Genack ◽  
N. Garcia ◽  
W. Polkosnik

2021 ◽  
Author(s):  
Tian Shi ◽  
Li Liangsheng ◽  
He Cai ◽  
Xianli Zhu ◽  
Qingfan Shi ◽  
...  

Abstract Non-line-of-sight (NLOS) imaging makes it possible to reconstruct hidden objects around corners, which is of fundamental importance in various fields. Despite recent advances, NLOS imaging has not been studied in certain typical random scenarios, such as tortuous corridors filled with random media. We dub such a category of complex environment “random corridor”, and propose a reduced spatial- and ensemble-speckle intensity correlation (RSESIC) method to image a moving object obscured by a random corridor. Experimental results show that the method can reconstruct image of a centimeter-sized hidden object with a sub-millimeter resolution by a low-cost digital camera. The imaging capability depends on three system parameters and can be characterized by the correlation fidelity (CF). Furthermore, the RSESIC method is able to recover the image of objects even for a single pixel containing the contribution of about $10^2$ speckle grains, which overcomes the theoretical limitation of traditional speckle imaging methods. Last but not least, when the power attenuation of speckle intensity leads to the serious deterioration of CF, the image of hidden objects can still be reconstructed by the corrected intensity correlation.


Author(s):  
Lucien F. Trueb

A new type of synthetic industrial diamond formed by an explosive shock process has been recently developed by the Du Pont Company. This material consists of a mixture of two basically different forms, as shown in Figure 1: relatively flat and compact aggregates of acicular crystallites, and single crystals in the form of irregular polyhedra with straight edges.Figure 2 is a high magnification micrograph typical for the fibrous aggregates; it shows that they are composed of bundles of crystallites 0.05-0.3 μ long and 0.02 μ. wide. The selected area diffraction diagram (insert in Figure 2) consists of a weak polycrystalline ring pattern and a strong texture pattern with arc reflections. The latter results from crystals having preferred orientation, which shows that in a given particle most fibrils have a similar orientation.


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