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On the microscopic dynamics of the 'Einstein solids' AlV2Al20 and GaV2Al20, and of YV2Al20: a benchmark system for 'rattling' excitations

机译:关于“爱因斯坦固体” AlV2Al20和GaV2Al20以及YV2Al20的微观动力学:“棘手”激发的基准系统

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The inelastic response of AV(2)Al(20) (with A = Al, Ga and Y) was probed by high-resolution inelastic neutron scattering experiments and density functional theory (DFT) based lattice dynamics calculations (LDC). Features characteristic of the dynamics of Al, Ga and Y are established experimentally in the low-energy range of the compounds. In the stereotype 'Einstein-solid' compound AlV2Al20 we identify a unique spectral density extending up to 10 meV at 1.6 K. Its dominating feature is a peak centred at 2 meV at the base temperature. A very similar spectral distribution is established in GaV2Al20 albeit the strong peak is located at 1 meV at 1.6 K. In YV2Al20 signals characteristic of Y dynamics are located above 8 meV. The spectral distributions are reproduced by the DFT-based LDC and identified as a set of phonons. The response to temperature changes between 1.6 and similar to 300 K is studied experimentally and the exceptionally vivid renormalization of the A characteristic modes in AlV2Al20 and GaV2Al20 is quantified by following the energy of the strong peak. At about 300 K it is shifted to higher energies by 300% for A = Al and 450% for A = Ga. The dynamics of A = Y in YV2Al20 show a minor temperature effect. This holds in general for modes located above 10 meV in any of the compounds. They are associated with vibrations of the V2Al20 matrix. Atomic potentials derived through DFT calculations indicate the propensity of A = Al and Ga to a strong positive energy shift upon temperature increase by a high quartic component. The effect of the strong phonon renormalization on thermodynamic observables is computed on grounds of the LDC results. It is shown that through the hybridization of A = Al and Ga with the V2Al20 dynamics the matrix vibrations in the low-energy range follow this renormalization.
机译:通过高分辨率非弹性中子散射实验和基于密度泛函理论(DFT)的晶格动力学计算(LDC)探索了AV(2)Al(20)(A = Al,Ga和Y)的非弹性响应。在化合物的低能范围内,通过实验确定了Al,Ga和Y动力学的特征。在原型“爱因斯坦-固体”化合物AlV2Al20中,我们确定了在1.6 K时扩展到10 meV的独特光谱密度。其主要特征是在基准温度下以2 meV为中心的峰。在GaV2Al20中建立了非常相似的光谱分布,尽管强峰位于1.6 K处的1 meV。在YV2Al20中,Y动力学特性的信号位于8 meV以上。光谱分布由基于DFT的LDC再现,并标识为一组声子。实验研究了温度在1.6到300 K之间变化的响应,并通过跟随强峰的能量来量化AlV2Al20和GaV2Al20中A特征模态的异常生动的重新归一化。在大约300 K时,对于A = Al,它转移到更高的能量,对于A = Ga,它转移到450%。在YV2Al20中,A = Y的动力学表现出较小的温度影响。这通常适用于任何化合物中高于10 meV的模式。它们与V2Al20矩阵的振动有关。通过DFT计算得出的原子电势表明A = Al和Ga随高次方温度升高而倾向于强正能量移动。根据LDC结果计算出强声子重正态化对热力学可观测值的影响。结果表明,通过A = Al和Ga与V2Al20动力学的杂交,低能范围内的基体振动遵循该重新归一化。

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