Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                

Optical study of the charge dynamics evolution in the topological insulators MnBi2Te4 and Mn(Bi0.74Sb0.26)2Te4 under high pressure

M. Köpf, S. H. Lee, Z. Q. Mao, and C. A. Kuntscher
Phys. Rev. B 109, 245124 – Published 18 June 2024

Abstract

The van der Waals material MnBi2Te4 and the related Sb-substituted compounds Mn(Bi1xSbx)2Te4 are prominent members of the family of magnetic topological insulators, in which rare quantum mechanical states can be realized. In this work, we study the evolution of the charge dynamics in MnBi2Te4 and the Sb-substituted compound Mn(Bi1xSbx)2Te4 with x=0.26 under hydrostatic pressure. For MnBi2Te4, the pressure dependence of the screened plasma frequency, the dc conductivity, and the reflectance at selected frequencies show weak anomalies at 2 and 4 GPa, which might be related to an electronic phase transition driven by the enhanced interlayer interaction. We observe a pressure-induced decrease in the optical gap, consistent with the decrease in and closing of the energy gap reported in the literature. Both studied materials show an unusual decrease in the low-energy optical conductivity under pressure, which we attribute to the decreasing spectral weight of the Drude terms describing the free charge carrier excitations. Our results suggest a localization of conduction electrons under pressure, possibly due to hybridization effects.

  • Figure
  • Figure
  • Figure
  • Received 9 January 2024
  • Revised 17 May 2024
  • Accepted 23 May 2024

DOI:https://doi.org/10.1103/PhysRevB.109.245124

©2024 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

M. Köpf1, S. H. Lee2,3, Z. Q. Mao2,3,4, and C. A. Kuntscher1,*

  • *Contact author: christine.kuntscher@physik.uni-augsburg.de

Article Text (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 109, Iss. 24 — 15 June 2024

Reuse & Permissions
Access Options
CHORUS

Article part of CHORUS

Accepted manuscript will be available starting 18 June 2025.
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1

    (a) Sketch of the crystal structure of MBST. Pressure-dependent (b) reflectance and (c) optical conductivity σ1 of the pure compound and (d) reflectance and (e) optical conductivity σ1 of the Sb-substituted compound with x=0.26. The corresponding loss functions of both materials are shown in the insets in (b) and (d), respectively. In (c), the intercept point of the linear extrapolations (dashed lines) of σ1 with the frequency axis indicates the onset of interband transitions, corresponding to the optical gap size.

    Reuse & Permissions
  • Figure 2
    Figure 2

    Drude-Lorentz fit of σ1 of the pure compound at (a) 1.13 GPa and (b) 8.0 GPa and of the 26% substituted compound at (d) 3.4 GPa and (e) 10.2 GPa. (c) and (f) display sketches of the corresponding band structures close to the Fermi level (similar to Ref. [38] and based on calculations by Chen et al. [9]). In (c) and (f), the vertical arrows display electronic transitions described by the respective Lorentz oscillators, where L1 describes transitions between two conduction bands, L1* describes transitions between the valence and conduction bands, and L2 corresponds to transitions across the optical gap. The energy gap Egap is indicated by a vertical orange line.

    Reuse & Permissions
  • Figure 3
    Figure 3

    (a) Reflectance values of MBT at selected frequencies as a function of pressure. The dashed vertical lines highlight the anomalies at 2 and 4 GPa. (b) σdc values of MBT obtained with the Drude-Lorentz fits, which are compared to results from Pei et al. [39] and Chen et al. [41]. (c) Plasma frequency ωpl of the two Drude terms, D1 and D2, and the total plasma frequency of the combination D1+D2 (see text for definition) for MBT as a function of pressure. (d) Scattering rate of Drude terms D1 and D2 for MBT as a function of pressure. (e) Screened plasma frequency ωplscr of the pure and the 26% doped samples, as obtained from the plasmon peak position in the loss function. Two anomalies in the pressure dependence of ωplscr for MBT at 2 and 4 GPa are indicated by vertical arrows. (f) Interband transition onset for MBT and the x = 0.26 doped sample as a function of pressure, determined by the zero crossing of the linear extrapolations in the σ1 spectra, which is an estimate for the size of the optical gap. The error bars in (a) have been estimated within the accuracy of the reflection measurement.

    Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×