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首页> 外文期刊>Nano letters >Zone-Folded Phonons and the Commensurate-Incommensurate Charge-Density-Wave Transition in 1T-TaSe2 Thin Films
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Zone-Folded Phonons and the Commensurate-Incommensurate Charge-Density-Wave Transition in 1T-TaSe2 Thin Films

机译:1T-TaSe2薄膜中的区域折叠声子与电荷-密度-波峰转换

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摘要

Bulk 1T-TaSe2 exhibits unusually high charge density wave (CDW) transition temperatures of 600 and 473 K below which the material exists in the incommensurate (I-CDW) and the commensurate (C-CDW) charge-density-wave phases, respectively. The (13)(1/2) x (13)(1/2), C-CDW reconstruction of the lattice coincides with new Raman peaks resulting from zone-folding of phonon modes from middle regions of the original Brillouin zone back to Gamma. The C-CDW transition temperatures as a function of film thickness are determined from the evolution of these new Raman peaks, and they are found to decrease from 473 to 413 K as the film thicknesses decrease from 150 to 35 nm. A comparison of the Raman data with ab initio calculations of both the normal and C-CDW phases gives a consistent picture of the zone-folding of the phonon modes following lattice reconstruction, The Raman peak at similar to 154 cm(-1) originates from the zone-folded phonons in the C-CDW phase. In the I-CDW phase, the loss of translational symmetry coincides with a strong suppression and broadening of the Raman peaks. The observed,change: in the C-CDW transition temperature is consistent with total energy calculations of bulk and monolayer 1T-TaSe2.
机译:体1T-TaSe2表现出600和473 K的异常高的电荷密度波(CDW)转变温度,低于该温度时,材料分别存在于不相称(I-CDW)和相称(C-CDW)电荷密度-波相中。晶格的(13)(1/2)x(13)(1/2)C-CDW重建与新的拉曼峰重合,该新的拉曼峰是声子模态从原始布里渊区的中间区域折回到伽玛的区域折叠而产生的。由这些新拉曼峰的演变确定了C-CDW转变温度与膜厚度的关系,发现随着膜厚度从150 nm降低至35 nm,它们从473 K降低至413K。拉曼数据与正常相和C-CDW相从头算的比较给出了晶格重构后声子模态的区域折叠的一致图像,类似于154 cm(-1)的拉曼峰源自在C-CDW相中的区域折叠声子。在I-CDW阶段,平移对称性的丧失与拉曼峰的强烈抑制和扩大相吻合。观察到的变化:C-CDW转变温度与本体和单层1T-TaSe2的总能量计算一致。

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