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The EMC determines G, that is, the amplitude loss and phase retardation associated with the scattering of an incident wave vector k to an exiting wave vector k′ (see Fig. 1).
Each wave that enters angular bin p at time t j has a phase ϕ j To determine the change to the electric field coordinate system, we must determine the change to the exiting wave coordinates relative to the initial coordinates.
In Figure VB in the Data Supplement, phase propagation graphs are somewhat sensitive to the initial directionality of the exiting wave, but the sequence of the phases is mainly determined by the spatial location of the pacing site; ie, V6 and V5 precede other precodials when pacing the lateral wall; V1 and V2 precede other precordials when pacing the septum.
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This leads to exit wave phase images in the reconstructions that are somewhat flatter (lower peak-to-peak range) than the true exit wave phases.
b Phase of the simulated exit wave function.
There is a substantial difference between the exit wave intensities.
c Mean absolute difference of exit wave between each iteration.
This fitted aberration function is then applied to the original exit wave as in Fig. 3g, generating an updated guess for the aberration-free exit wave.
Our algorithm relies on creating a synthetic exit wave by applying point-symmetrization to all atomic columns in a reference region, to approximate the aberration-free exit wave.
In all cases, the symmetrized exit wave is in perfect or good agreement with the original exit waves shown in Fig. 1a.
This process can be achieved by solving two inverse problems: reconstruction of the exit wave and reconstruction of the electron distribution from exit waves.
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CEO of Professional Science Editing for Scientists @ prosciediting.com