Pavlovska A, Werner S, Maximov B, Mill B
Universität München, Institut für Kristallographie und Angewandte Mineralogie, Theresienstrasse 41, Germany.
Acta Crystallogr B. 2002 Dec;58(Pt 6):939-47. doi: 10.1107/s0108768102010273. Epub 2002 Nov 28.
The hydrostatic compression of piezoelectric single crystals of La(3)Nb(0.5)Ga(5.5)O(14) (LNG) and La(3)Ta(0.5)Ga(5.5)O(14) (LTG) was studied at pressures of up to 23 GPa in diamond-anvil high-pressure cells using single-crystal X-ray diffraction techniques. The reflection-intensity data for LNG and LTG were collected at pressures of up to 22.8 GPa and 16.7 GPa, respectively. Both compounds show anisotropic behaviour under pressure, which is caused by differences in bonding parallel to the a and c directions. The compression of strongly rigid structures leads to increasing internal strains and results, at pressures of 12.4 (3) GPa for LNG and 11.7 (3) GPa for LTG, in a transition to lower symmetry. The compressibilities along the c axis are almost the same for LNG and LTG through the whole investigated pressure range. In contrast, the pressure dependencies of the a axis of these materials are similar only for the initial phase, and the axial compressibilities for the high-pressure polymorphs of LNG and LTG are significantly different to each other. The volume compressibilities of trigonal LNG and LTG (space group P321) are about 0.007 GPa(-1); respective bulk moduli are 145 (3) GPa and 144 (2) GPa. The monoclinic high-pressure phases (space group A2) of LNG and LTG show differing compressions, which can be explained by the substitution of Ta(5+) for Nb(5+). Thus, the bulk moduli for the high-pressure polymorphs of LNG and LTG are B(0) = 93 (2) GPa and B(0) = 128 (12) GPa, respectively. The volume compressibilities of the high-pressure phases at 0.011 GPa(-1) for LNG and 0.008 GPa(-1) for LTG are higher than the initial phases, this effect being more pronounced in the case of LNG.
在金刚石对顶砧高压腔中,利用单晶X射线衍射技术,在高达23吉帕的压力下研究了镧铌镓酸镧(LNG,化学式为La(3)Nb(0.5)Ga(5.5)O(14))和镧钽镓酸镧(LTG,化学式为La(3)Ta(0.5)Ga(5.5)O(14))压电单晶的静水压压缩情况。分别在高达22.8吉帕和16.7吉帕的压力下收集了LNG和LTG的反射强度数据。两种化合物在压力下均表现出各向异性行为,这是由平行于a轴和c轴方向的键合差异所致。强刚性结构的压缩导致内部应变增加,并在LNG为12.4(3)吉帕、LTG为11.7(3)吉帕的压力下转变为较低对称性。在整个研究压力范围内,LNG和LTG沿c轴的压缩率几乎相同。相比之下,这些材料a轴的压力依赖性仅在初始阶段相似,LNG和LTG高压多晶型物的轴向压缩率彼此显著不同。三方晶系的LNG和LTG(空间群P321)的体积压缩率约为0.007吉帕⁻¹;相应的体模量分别为145(3)吉帕和144(2)吉帕。LNG和LTG的单斜晶系高压相(空间群A2)表现出不同的压缩情况,这可以用Ta(5+)取代Nb(5+)来解释。因此,LNG和LTG高压多晶型物的体模量分别为B(0)=93(2)吉帕和B(0)=128(12)吉帕。LNG高压相在0.011吉帕⁻¹时的体积压缩率以及LTG在0.008吉帕⁻¹时的体积压缩率高于初始相,这种效应在LNG中更为明显。