TY - JOUR
T1 - Dynamical diffraction effects on higher-order laue zone lines in CBED patterns of semiconductors
AU - Okuyama, T.
AU - Matsumura, S.
AU - Kuwano, N.
AU - Oki, K.
AU - Tomokiyo, Y.
N1 - Funding Information:
The authorsw ouldlike to thank Mr. E. Tanaka and Mr. T. Manabe for their technicaals sistance in operationo f an electron microscopea t the HVEM LaboratoryK, yushuUniversity. This work was supportedin part by Grant-in-Aid No. 62550477fo r ScientificR esearch(c ) and No. 62104005f or Special Project Researcho n "Alloy SemiconductoPr hysics and Electronics" from the Ministry of Education,S ciencea nd Culture of Japan. One of us (T.O.) is also indebtedto Kazato ResearchF oundation.
PY - 1989/11
Y1 - 1989/11
N2 - We studied the dynamical diffraction effects on the defect lines of higher-order Laue zone reflections (HOLZ lines) in bright field disks of convergent-beam electron diffraction (CBED). The positions of the HOLZ lines were confirmed experimentally to deviate by a small amount from the positions expected from the kinematical approximation. The amount of line shift is represented by the corresponding deviation of the accelerating voltage Δ E. In the case of [111] incidence, one HOLZ reflection can generate two lines with negative and positive values of Δ E. Calculations based on the dynamical diffraction theory clarified that the HOLZ lines with negative and positive Δ E arise from the first and second branches of the zeroth-layer dispersion surface, respectively. Either, or occasionally both, of the lines is observed in the HOLZ pattern, depending upon which branch is dominantly excited. The dependency of Δ E on the material species and thickness of specimen and on the zone axis is discussed in detail for Si, Ge and some III-V compound semiconductors.
AB - We studied the dynamical diffraction effects on the defect lines of higher-order Laue zone reflections (HOLZ lines) in bright field disks of convergent-beam electron diffraction (CBED). The positions of the HOLZ lines were confirmed experimentally to deviate by a small amount from the positions expected from the kinematical approximation. The amount of line shift is represented by the corresponding deviation of the accelerating voltage Δ E. In the case of [111] incidence, one HOLZ reflection can generate two lines with negative and positive values of Δ E. Calculations based on the dynamical diffraction theory clarified that the HOLZ lines with negative and positive Δ E arise from the first and second branches of the zeroth-layer dispersion surface, respectively. Either, or occasionally both, of the lines is observed in the HOLZ pattern, depending upon which branch is dominantly excited. The dependency of Δ E on the material species and thickness of specimen and on the zone axis is discussed in detail for Si, Ge and some III-V compound semiconductors.
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U2 - 10.1016/0304-3991(89)90053-3
DO - 10.1016/0304-3991(89)90053-3
M3 - Article
AN - SCOPUS:0024761897
SN - 0304-3991
VL - 31
SP - 309
EP - 317
JO - Ultramicroscopy
JF - Ultramicroscopy
IS - 3
ER -