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Figure 1
(a) The geometry of large-angle convergent-beam electron diffraction (LACBED) for one diffracted beam, ignoring all other diffracted beams. The Bragg condition is satisfied when the incident and exit beams make an angle [\theta_{hkl}] to the diffracted planes, defining a cone. This gives a parabola on the diffraction pattern which, because of the very small Bragg angle, appears as a straight line in an LACBED pattern (b), taken from a [100] silicon crystal. (c) The corresponding CBED pattern, with a small part of the LACBED pattern visible in the [2{\overline 2}0] disc.

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ISSN: 2053-2733
Volume 69| Part 4| May 2013| Pages 427-434
doi:10.1107/S0108767313010143
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