Abstract
A formalism developed in a previous paper [1] is now applied in a general way to the special three beam case (111, 1̄11). The restriction for the incoming wave to be located in the symmetry plane is abolished. The individual behavior of the dispersion surfaces and reflection curves are determined and discussed.
Received: 1978-10-18
Published Online: 2014-6-2
Published in Print: 1978-12-1
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