Individual
grain orientation measurement in the SEM
from backscatter Kikuchi patterns (BKP)
History
of BKD and "Automated EBSD"
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1928 |
Shoji Nishikawa and
Seishi Kikuchi |
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Shoji Nishikawa and
Seishi Kikuchi In the following publications Seishi Kikuchi and Shigeo
Nakagawa concentrated their studies on the
deviation of the lines from the exact Bragg
position due to anomalous dispersion of crossing
lines and the effect of the refractive index of
the lattice on fast electrons.
S. Kikuchi and Sh.
Nakagawa
Already in 1928,
Seishi Kikuchi grew fond of atomic physics. He
published an investigation on the mode of
disintegration of Radium (J.J.Phys. 4(1928)
143.), met Werner von Heisenberg on his visit to
Japan, and joined for some time Heisenberg's team
at the university of Leipzig (Germany). Back in
Japan, starting in 1934 he installed a 600 kV
Cockroft-Walton high-voltage generator, the most
powerful at that time, and a charged particle
accelerator at the (now) Osaka University Physical
Science Department. Seishi Kikuchi is known as an
outstanding Japanese nuclear physicist. |
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1932/33 |
K. Shinohara: |
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1933 |
R. von Meibom and E. Rupp |
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1937 |
H. Boersch |
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Backscatter Kikuchi patterns
obtained from iron (left) and fluorspar (fluorite)
(right, recorded on a cylindrical film) at 20
kV. |
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He used flat photographic plates as well as a cylindrical specimen chamber with a cylindrical film to produce high-angle Kikuchi patterns. The angular range is considerably larger than that obtained before in the TEM and in present SEM appliances. The patterns are remarkably sharp and rich in detail. The widths of the bands was found, in agreement with Bragg's law, to be related to the energy of the incident beam and the interplanar lattice spacings. Boersch has discussed the origin of Kikuchi lines, dark and bright bands and envelops taking von Laue's dynamical theory of electron diffraction into consideration.
G.I. Finch and H. Wilman
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1947, 1948 |
K. Artmann (Remark: Kikuchi envelops can have a ring shape or a parabolic appearance. Perhaps due to the similarity with HOLZ rings of spots in transmission electron diffraction on thin foils, the ring shaped envelops are sometimes named "HOLZ lines" in recent publications even in the case of BKD. One should, however, bear in mind that Kikuchi envelops are definitively an effect of dynamical rather than kinematical diffraction. The Ewald construction is a very useful model for illustrating the formation of diffraction spots, but it is not applicable for BKD. In particular, there is no coherence between a primary beam and the diffracted beams.)
K. Artmann |
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1954 |
M.N. Alam, M.
Blackman and D.W. Pashley |
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1973 |
J.A. Venables, C.J.
Harland |
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1987 |
D. Dingley &
Link: 1st commercial system for the
SEM |
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1990 |
N.-H. Schmidt (Risų;
HKL): commercial system ("Channel") |
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1992 |
N. Krieger Lassen, D.
Juul Jensen, K. Conradsen |
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1993 |
B.L. Adams, S.I.
Wright |
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1994 |
Niels Krieger Lassen
(PhD Thesis at Risų and Univ. Lingby, Denmark) |
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