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. 2011 Jan 6;2(2):278–290. doi: 10.1364/BOE.2.000278

Fig. 1.

Fig. 1.

Schematic of the diffraction geometry. The wavefront of the initial field Efar is modified to Edfar, which captures the effects of a given medium. Waves launched from a Lambertian source (symbolized by semi-circle) with a wave vector k are allowed to scatter in a medium of thickness T, and the amplitude and phase at each exit wave vector k′ is determined.