Rohrbeck A, de la Flor G, Aroyo M I, Gospodinov M, Bismayer U, Mihailova B
Fachbereich Geowissenschaften, Universität Hamburg, 20146 Hamburg, Germany.
J Phys Condens Matter. 2016 Nov 30;28(47):475902. doi: 10.1088/0953-8984/28/47/475902. Epub 2016 Sep 23.
Resonance Raman spectroscopy was applied to doped PbSc0.5Ta0.5O3 and PbSc0.5Nb0.5O3 relaxor ferroelectrics, to better understand the effect of composition disorder on the mesoscopic-scale polar order in complex perovskite-type (ABO3) ferroelectrics. The excitation photon energy used was 3.8 eV, which is slightly above the energy gap and corresponds to the maximum of the optical dielectric permittivity. Group-theory analysis reveals that the resonance Raman scattering (RRS) observed under these conditions is allowed only in polar crystal classes. Therefore, RRS is dominated by the atomic dynamics of nanoregions with coherent polar distortions, which considerably facilitates the comparison of polar order in various compounds. The results show that A-site doping (Ba(2+), Sr(2+), La(3+), Bi(3+)) has significantly stronger effect on the structural polarity than the introduction of a third element at the B site (Nb(5+) or Sn(4+) doped in PbSc0.5Ta0.5O3). The A-site substitution by cations that in contrast to Pb(2+) have isotropic outermost electron shells disturbs the system of lone-pair electrons, thus reducing the correlation length of coupled polar distortions and the strength of the electric field associated with the mean polarization of polar nanoregions. A-site doping with larger cations (Ba(2+)) augments the polar deformation of the individual BO6 octahedra due to local elastic fields. As a result, such A-site doping intensifies the initial structural polarity at high temperatures and prevails the enlargement of the polar fraction at low temperatures. A-site doping with smaller cations (Sr(2+), La(3+)), regardless if they are isovalent or aliovalent to Pb(2+), increases the correlation length of antiferrodistortive order (BO6 tilts), which in turn assists the development of double-perovskite structure with coherent local polar distortions. A-site doping with aliovalent cations (Bi(3+)) having the same outermost electron shell and ionic radius as the host A-site Pb(2+) cations leads to stronger coupling along the -B-O-B- bond linkages due to enhanced random local electric fields.
共振拉曼光谱被应用于掺杂的PbSc0.5Ta0.5O3和PbSc0.5Nb0.5O3弛豫铁电体,以更好地理解成分无序对复杂钙钛矿型(ABO3)铁电体介观尺度极性有序的影响。所使用的激发光子能量为3.8 eV,略高于能隙且对应于光学介电常数的最大值。群论分析表明,在这些条件下观察到的共振拉曼散射(RRS)仅在极性晶体类中是允许的。因此,RRS由具有相干极性畸变的纳米区域的原子动力学主导,这极大地便于比较各种化合物中的极性有序。结果表明,A位掺杂(Ba(2+)、Sr(2+)、La(3+)、Bi(3+))对结构极性的影响比在B位引入第三种元素(在PbSc0.5Ta0.5O3中掺杂Nb(5+)或Sn(4+))显著更强。与Pb(2+)相比具有各向同性最外层电子壳的阳离子对A位的取代扰乱了孤对电子体系,从而减小了耦合极性畸变的相关长度以及与极性纳米区域平均极化相关的电场强度。用较大阳离子(Ba(2+))进行A位掺杂由于局部弹性场增强了单个BO6八面体的极性变形。结果,这种A位掺杂在高温下增强了初始结构极性,并在低温下主导了极性分数的增大。用较小阳离子(Sr(2+)、La(3+))进行A位掺杂,无论它们与Pb(2+)是等价还是异价,都会增加反铁畸变有序(BO6倾斜)的相关长度,这反过来又有助于具有相干局部极性畸变的双钙钛矿结构的发展。用与主体A位Pb(2+)阳离子具有相同最外层电子壳和离子半径的异价阳离子(Bi(3+))进行A位掺杂,由于增强的随机局部电场导致沿 -B-O-B- 键连接的更强耦合。