Previous work employed X-ray three-beam diffraction techniques to obtain
part of the L-arginine hydrochloride monohydrate (L-AHCL. H2O)
piezoelectric coefficients, namely d(21), d(22), d(23) and d(25). Those
coefficients were obtained by measuring the shift in the angular
position of a number of secondary reflections as a function of the
electric field applied in the 010 piezoelectric direction. In this
paper a similar procedure has been used to measure the remaining four
piezoelectric coefficients in L-AHCL. H2O: with the electric field
applied in the 100 direction, d(14) and d(16) were measured; with
the electric field applied in the 001 direction, d(34) and d(36)
were obtained. Therefore the entire piezoelectric matrix of the L-AHCL.
H2O crystal has been successfully measured.
%0 Journal Article
%1 WOS:000241363300005
%A Almeida, Juliana M A
%A Miranda, Marcus A R
%A Avanci, Luis H
%A de Menezes, Alan S
%A Cardoso, Lisandro P
%A Sasaki, Jose M
%C 2 ABBEY SQ, CHESTER, CH1 2HU, ENGLAND
%D 2006
%I INT UNION CRYSTALLOGRAPHY
%J JOURNAL OF SYNCHROTRON RADIATION
%K arginine; diffraction; fields; materials} piezoelectric strain-induced {X-ray
%N 6
%P 435-439
%R 10.1107/S0909049506033061
%T Piezoelectric coefficients d(14), d(16), d(34) and d(36) of an
L-arginine hydrochloride monohydrate crystal by X-ray three-beam
diffraction
%V 13
%X Previous work employed X-ray three-beam diffraction techniques to obtain
part of the L-arginine hydrochloride monohydrate (L-AHCL. H2O)
piezoelectric coefficients, namely d(21), d(22), d(23) and d(25). Those
coefficients were obtained by measuring the shift in the angular
position of a number of secondary reflections as a function of the
electric field applied in the 010 piezoelectric direction. In this
paper a similar procedure has been used to measure the remaining four
piezoelectric coefficients in L-AHCL. H2O: with the electric field
applied in the 100 direction, d(14) and d(16) were measured; with
the electric field applied in the 001 direction, d(34) and d(36)
were obtained. Therefore the entire piezoelectric matrix of the L-AHCL.
H2O crystal has been successfully measured.
@article{WOS:000241363300005,
abstract = {Previous work employed X-ray three-beam diffraction techniques to obtain
part of the L-arginine hydrochloride monohydrate (L-AHCL. H2O)
piezoelectric coefficients, namely d(21), d(22), d(23) and d(25). Those
coefficients were obtained by measuring the shift in the angular
position of a number of secondary reflections as a function of the
electric field applied in the [ 010] piezoelectric direction. In this
paper a similar procedure has been used to measure the remaining four
piezoelectric coefficients in L-AHCL. H2O: with the electric field
applied in the [100] direction, d(14) and d(16) were measured; with
the electric field applied in the [001] direction, d(34) and d(36)
were obtained. Therefore the entire piezoelectric matrix of the L-AHCL.
H2O crystal has been successfully measured.},
added-at = {2022-05-23T20:00:14.000+0200},
address = {2 ABBEY SQ, CHESTER, CH1 2HU, ENGLAND},
author = {Almeida, Juliana M A and Miranda, Marcus A R and Avanci, Luis H and de Menezes, Alan S and Cardoso, Lisandro P and Sasaki, Jose M},
biburl = {https://www.bibsonomy.org/bibtex/25fe44ddd6d95329b14659cbaaced8d6c/ppgfis_ufc_br},
doi = {10.1107/S0909049506033061},
interhash = {9e0d92e607ea4120bda3ef89b9955ff0},
intrahash = {5fe44ddd6d95329b14659cbaaced8d6c},
issn = {1600-5775},
journal = {JOURNAL OF SYNCHROTRON RADIATION},
keywords = {arginine; diffraction; fields; materials} piezoelectric strain-induced {X-ray},
number = 6,
pages = {435-439},
publisher = {INT UNION CRYSTALLOGRAPHY},
pubstate = {published},
timestamp = {2022-05-23T20:00:14.000+0200},
title = {Piezoelectric coefficients d(14), d(16), d(34) and d(36) of an
L-arginine hydrochloride monohydrate crystal by X-ray three-beam
diffraction},
tppubtype = {article},
volume = 13,
year = 2006
}