000089119 001__ 89119
000089119 005__ 20180317093512.0
000089119 0247_ $$2doi$$a10.1063/1.1929091
000089119 022__ $$a0021-8979
000089119 02470 $$2DAR$$a7222
000089119 02470 $$2ISI$$a000231062200080
000089119 037__ $$aARTICLE
000089119 245__ $$aDomain engineering of the transverse piezoelectric coefficient in perovskite ferroelectrics
000089119 260__ $$c2005
000089119 269__ $$a2005
000089119 336__ $$aJournal Articles
000089119 500__ $$aDavis, M Ecole Polytech Fed Lausanne, Ceram Lab, CH-1015 Lausanne, Switzerland Ecole Polytech Fed Lausanne, Ceram Lab, CH-1015 Lausanne, Switzerland
000089119 500__ $$a953FO
000089119 500__ $$aTimes Cited:2
000089119 500__ $$aCited References Count:28
000089119 520__ $$aThe transverse piezoelectric coefficient d(31)*, has been calculated for the six domain-engineered structures occurring in perovskite single crystals, using data for rhombohedral PMN-33PT [0.67Pb(Mg1/3Nb2/3)O-3-0.33PbTiO(3)], orthorhombic potassium niobate (KNbO3), tetragonal barium titanate (BaTiO3), and tetragonal lead titanate (PbTiO3). Unlike the longitudinal coefficient (d(33)*), d(31)* is found to be strongly dependent on the transverse (x(1)') direction of the as-cut crystal. In general, different domains in a domain-engineered structure will contribute different values of d(31)* to that measured. Predicting the global d(31)*, is therefore difficult since it will depend on the proportion of each domain variant in the structure. Important qualitative differences between tetragonal BaTiO3 and PbTiO3 are discussed. Whereas polarization rotation is important in BaTiO3, PbTiO3 shows a stronger collinear piezoelectric effect due the absence of a low-temperature ferroelectric-ferroelectric phase transition. This leads to low values of d(33)* and even positive values of d(31)*, in the [111](C)-poled (C: pseudocubic) domain-engineered structure. The methodology described can be usefully applied to all perovskites. (c) 2005 American Institute of Physics.
000089119 6531_ $$a0.67pb(mg1/3nb2/3)o-3-0.33pbtio(3) single-crystals
000089119 6531_ $$aorientation dependence
000089119 6531_ $$abarium-titanate
000089119 6531_ $$aconfigurations
000089119 6531_ $$asymmetries
000089119 700__ $$0240628$$aDavis, M.$$g156113
000089119 700__ $$0240215$$aDamjanovic, D.$$g104860
000089119 700__ $$aHayem, D.
000089119 700__ $$0240019$$aSetter, N.$$g106416
000089119 773__ $$j98$$k1$$q-$$tJournal of Applied Physics
000089119 909CO $$ooai:infoscience.tind.io:89119$$particle$$pSTI
000089119 909C0 $$0252012$$pLC$$xU10334
000089119 937__ $$aLC-ARTICLE-2005-010
000089119 970__ $$a10/LC
000089119 973__ $$aEPFL$$rREVIEWED$$sPUBLISHED
000089119 980__ $$aARTICLE