Kamba S, Kempa M, Bovtun V, Petzelt J, Brinkman K, Setter N
Institute of Physics, Academy of Sciences of the Czech Republic, Na Slovance 2, 182 21 Prague 8, Czech Republic.
J Phys Condens Matter. 2005 Jun 29;17(25):3965-74. doi: 10.1088/0953-8984/17/25/022. Epub 2005 Jun 10.
The relaxor ferroelectric PbMg(1/3)Nb(2/3)O(3) (PMN) is investigated by means of dielectric and Fourier transform far infrared transmission spectroscopy in the frequency range from 10 kHz to 15 THz at temperatures between 20 and 900 K using mostly thin films on infrared transparent sapphire substrates. While the thin film relaxors display reduced dielectric permittivity at low frequencies, their high frequency lattice response is shown to be the same as for single-crystal/ceramic specimens. In contrast to the results of inelastic neutron scattering, the optic soft mode is found to be underdamped at all temperatures. On heating, the TO1 soft phonon follows the Cochran law with an extrapolated critical temperature of 670 K near to the Burns temperature. Above 450 K the soft mode frequency levels off near 50 cm(-1) and above the Burns temperature it slightly hardens. Central-mode-type dispersion assigned to the dynamics of polar nanoclusters appears below the Burns temperature at frequencies near to but below the soft mode and slows down and broadens dramatically on cooling, finally, below the freezing temperature of 200 K, giving rise to frequency independent losses from the microwave range down. A new explanation of the phonon 'waterfall' effect in inelastic neutron scattering spectra is proposed.
利用介电和傅里叶变换远红外透射光谱,在20至900 K的温度范围内,于10 kHz至15 THz的频率区间,主要通过红外透明蓝宝石衬底上的薄膜对弛豫铁电体PbMg(1/3)Nb(2/3)O(3)(PMN)进行了研究。虽然薄膜弛豫体在低频下表现出降低的介电常数,但其高频晶格响应与单晶/陶瓷样品相同。与非弹性中子散射的结果相反,发现光学软模在所有温度下均为欠阻尼。加热时,TO1软声子遵循科克伦定律,外推临界温度为670 K,接近伯恩斯温度。在450 K以上,软模频率在50 cm(-1)附近趋于平稳,在伯恩斯温度以上则略有变硬。归因于极性纳米团簇动力学的中心模型色散在伯恩斯温度以下出现在接近但低于软模的频率处,在冷却时显著减慢并展宽,最终在200 K的冻结温度以下,导致从微波频段向下的频率无关损耗。提出了对非弹性中子散射光谱中声子“瀑布”效应的新解释。