Generation of mechanical interference fringes by multi-photon quantum measurement

Author(s):  
M. Ringbauer ◽  
T. J. Weinhold ◽  
A. G. White ◽  
M. R. Vanner
2018 ◽  
Vol 20 (5) ◽  
pp. 053042 ◽  
Author(s):  
M Ringbauer ◽  
T J Weinhold ◽  
L A Howard ◽  
A G White ◽  
M R Vanner

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.


Author(s):  
Vladimir B. Braginsky ◽  
Farid Ya Khalili ◽  
Kip S. Thorne
Keyword(s):  

1996 ◽  
Vol 193 (Part_1_2) ◽  
pp. 226-227
Author(s):  
H. Schmiedel
Keyword(s):  

Author(s):  
Mark Kimball

Abstract Silicon’s index of refraction has a strong temperature coefficient. This temperature dependence can be used to aid sample thinning procedures used for backside analysis, by providing a noncontact method of measuring absolute sample thickness. It also can remove slope ambiguity while counting interference fringes (used to determine the direction and magnitude of thickness variations across a sample).


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