论文标题
抗铁磁到顺磁相转变附近的α-芬(Goothite)的拉曼光谱
Raman spectroscopy of alpha-FeOOH (goethite) near antiferromagnetic to paramagnetic phase transition
论文作者
论文摘要
在300 k至473 K的温度下,研究了使用极化的拉曼光谱的谷岩($α-$ feOOH)的合成粉,矿石样品和矿物质的单晶($α-$ feOOH)。振动模式的对称性在不同的散射构型中观察到,并非方程性地确定。两种类型的晶格 - 动力计算支持了拉曼活性模式对确定的原子振动的分配:经验壳模型和$ \ textit {ab intio} $ dft。一些拉曼活性振动的线形参数的温度依赖性接近抗铁磁 - paragnetic-paramagnetic相变,用于该化合物中显着的自旋晶格耦合。在这方面,最有用的是387 cm $^{ - 1} $的$ b_ {3g} $ phonon,它覆盖了宽阔的散射背景,并显示出明显的不对称fano-lineshape。不对称的磁磁状态在Neel温度以上($ t _ {\ text {n}} $ = 393 K)上增加,表明这种模式与基础激发连续性的强烈相互作用。根据我们的实验结果以及$α-$ feOOH的磁性结构和传输性能的现有数据讨论了激发背景的起源。我们合理地认为,背景很可能源于磁性激发,而$ b_ {3g} $ phonon的不对称形状是该模式与Fe-O1-Fe旋转二聚体的线性自旋偶联的结果。还考虑了另一种机制,即与$ t _ {\ text {n}} $高于$ t _ {\ text {n}} $的声子相互作用。
Synthetic powder, ore samples and mineral single crystals of goethite ($α-$FeOOH) were investigated with polarized Raman spectroscopy at temperatures from 300 K to 473 K. The symmetry of the vibrational modes, observed in different scattering configurations, was determined unequivocally. The assignment of the Raman-active modes to definite atomic vibrations is supported by two types of lattice-dynamical calculations: empirical shell-model and $\textit{ab initio}$ DFT. The temperature dependencies of the lineshape parameters of some Raman-active vibrations near to the antiferromagnetic-paramagnetic phase transition infers for a significant spin-lattice coupling in this compound. The most informative in this aspect is the $B_{3g}$ phonon at 387 cm$^{-1}$, which overlays a broad scattering background and displays a pronounced asymmetric Fano-lineshape. The asymmetry increases in the paramagnetic state above the Neel temperature ($T_{\text{N}}$ = 393 K) indicating a strong interaction of this mode with the underlying excitation continuum. The origin of the excitation background is discussed in light of our experimental results and the existing data for the magnetic structure and transport properties of $α-$FeOOH. We rationalize that, most probably, the background stems from magnetic excitations, and the asymmetric shape of the $B_{3g}$ phonon is a result of a linear spin-phonon coupling of this mode with the Fe-O1-Fe spin dimers. Another mechanism, a phonon interaction with thermally activated charge carriers above above $T_{\text{N}}$, is also considered.