2007
DOI: 10.1016/j.ultramic.2006.10.006
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Many-beam dynamical simulation of electron backscatter diffraction patterns

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Cited by 176 publications
(168 citation statements)
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“…Each electron's contribution to the EBSD pattern was simulated, using the calculated image intensity as a probability distribution function, which also provides the Poisson contribution to the noise. The input image intensity was simulated using dynamical diffraction calculations of the Kikuchi band features in EBSD patterns using code developed by Winkelmann [34]. The patterns simulated using this model for the detector geometry, SEM imaging conditions, and for an electron budget corresponding to our experimental data are shown in Fig.…”
Section: H Y S I C a L R E V I E W L E T T E R S Week Ending 9 Augustmentioning
confidence: 99%
“…Each electron's contribution to the EBSD pattern was simulated, using the calculated image intensity as a probability distribution function, which also provides the Poisson contribution to the noise. The input image intensity was simulated using dynamical diffraction calculations of the Kikuchi band features in EBSD patterns using code developed by Winkelmann [34]. The patterns simulated using this model for the detector geometry, SEM imaging conditions, and for an electron budget corresponding to our experimental data are shown in Fig.…”
Section: H Y S I C a L R E V I E W L E T T E R S Week Ending 9 Augustmentioning
confidence: 99%
“…For each orientation, the process consists of three steps. The first step models the interaction of the electron beam with the sample using the Schrödinger equation with a Bloch wave ansatz [11]. The backscattered electron yield is calculated for a set of directions covering the hemisphere of all possible exit directions.…”
Section: Construction Of Diffraction Pattern Dictionarymentioning
confidence: 99%
“…We used the Nelder-Mead simplex method 25 to find the local maximum of the cross-correlation coefficient between experiment and simulations, with start parameters near an orientation obtained by a conventional indexing procedure based on the Hough transform. 26 For the dynamical electron diffraction simulations 27 and the best-fit optimizations, we applied the software ESPRIT DynamicS (Bruker Nano, Berlin). In the optimization procedure, the simulated Kikuchi patterns are reprojected from stored master data according to the current values of the projection parameters, then the crosscorrelation coefficient is calculated, and new updated projection parameters are chosen for the next iteration according to the simplex approach.…”
mentioning
confidence: 99%