Lattice Dynamics of Bi2Te3 and Vibrational Modes in Raman Scattering of Topological Insulators MnBi2Te4•n(Bi2Te3)

被引:13
|
作者
Abdullaev, N. A. [1 ,2 ]
Amiraslanov, I. R. [1 ,2 ]
Aliev, Z. S. [2 ]
Jahangirli, Z. A. [1 ,2 ]
Sklyadneva, I. Yu [3 ]
Alizade, E. G. [1 ]
Aliyeva, Y. N. [1 ,2 ]
Otrokov, M. M. [4 ,5 ]
Zverev, V. N. [6 ]
Mamedov, N. T. [1 ,2 ]
Chulkov, E., V [7 ,8 ]
机构
[1] Azerbaijan Natl Acad Sci, Inst Phys, AZ-1141 Baku, Azerbaijan
[2] Baku State Univ, AZ-1148 Baku, Azerbaijan
[3] Tomsk State Univ, Tomsk 634050, Russia
[4] Ctr Mixto CSIC UPV EHU, Ctr Fis Mat CFM MPC, Donostia San Sebastian 20018, Basque Country, Spain
[5] Basque Fdn Sci, Ikerbasque, Bilbao 48011, Spain
[6] Russian Acad Sci, Inst Solid State Phys, Chernogolovka 142432, Moscow Region, Russia
[7] St Petersburg State Univ, St Petersburg 198504, Russia
[8] Univ Pas Vasco UPV EHU, Dept Polimeros & Mat Avanzados Fis Quim & Tecnol, Fac Ciencias Quim, San Sebastian 20080, Basque Country, Spain
关键词
BI2SE3; FILMS;
D O I
10.1134/S0021364022600987
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
This work is devoted to the experimental study and symmetry analysis of the Raman-active vibration modes in MnBi2Te4 center dot n(Bi2Te3) van der Waals topological insulators, where n is the number of Te-Bi-Te-Bi-Te quintuple layers between two neighboring Te-Bi-Te-Mn-Te-Bi-Te septuple layers. Confocal Raman spectroscopy is applied to study Raman spectra of crystal structures with n = 0,1, 2, 3, 4, 5, 6, and infinity. The experimental frequencies of vibration modes of the same symmetry in the structures with different n are compared. The lattice dynamics of free-standing one, three, and four quintuple layers, as well as of bulk Bi2Te3 (n = infinity) and MnBi2Te4 (n = 0), is considered theoretically. Vibrational modes of the last two systems have the same symmetry, but different displacement fields. These fields in the case of a Raman-active mode do not contain displacements of manganese atoms for any finite n. It is shown that two vibrational modes in the low-frequency region of the spectrum (35-70 cm(-1)) of structures with n = 1, 2, 3, 4, 5, and 6 practically correspond to the lattice dynamics of n free quintuple Bi2Te3 layers. For this reason, the remaining two vibration modes, which are observed in the high-frequency region of the spectrum (100-140 cm(-1)) and are experimentally indistinguishable in the sense of belonging to quintuple or septuple layer or to both layers simultaneously, should also be assigned to vibrations in quintuple layers under immobile atoms of septuple layers.
引用
收藏
页码:749 / 756
页数:8
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