Image intensity fluctuations of an incoherent source observed through a turbulent medium

1985 ◽  
Vol 28 (11) ◽  
pp. 972-977 ◽  
Author(s):  
V. U. Zavorotnyi
1984 ◽  
Vol 27 (10) ◽  
pp. 890-894 ◽  
Author(s):  
S. S. Kashkarov ◽  
T. N. Nesterova ◽  
A. S. Smirnov

1979 ◽  
Vol 26 (5) ◽  
pp. 531-542 ◽  
Author(s):  
V.I. Tatarskii ◽  
A.S. Gurvich ◽  
B.S. Elepov ◽  
Vl.V. Pokasov ◽  
K.K. Sabelfeld

1980 ◽  
Vol 10 (3) ◽  
pp. 308-312 ◽  
Author(s):  
B S Agrovskiĭ ◽  
V V Vorob'ev ◽  
A S Gurvich ◽  
V V Pokasov ◽  
A N Ushakov

Author(s):  
E. Völkl ◽  
L.F. Allard ◽  
B. Frost ◽  
T.A. Nolan

Off-axis electron holography has the well known ability to preserve the complex image wave within the final, recorded image. This final image described by I(x,y) = I(r) contains contributions from the image intensity of the elastically scattered electrons IeI (r) = |A(r) exp (iΦ(r)) |, the contributions from the inelastically scattered electrons IineI (r), and the complex image wave Ψ = A(r) exp(iΦ(r)) as:(1) I(r) = IeI (r) + Iinel (r) + μ A(r) cos(2π Δk r + Φ(r))where the constant μ describes the contrast of the interference fringes which are related to the spatial coherence of the electron beam, and Φk is the resulting vector of the difference of the wavefront vectors of the two overlaping beams. Using a software package like HoloWorks, the complex image wave Ψ can be extracted.


Sign in / Sign up

Export Citation Format

Share Document