\documentclass[fleqn,10pt]{wlscirep}
\usepackage[T1]{fontenc}
\usepackage[utf8]{inputenc}
\usepackage{authblk, csquotes, indentfirst, graphicx, hyperref, adjustbox, amsmath}
\usepackage[english]{babel}

\newcommand{\mgbt}{$\mathrm{Mn}_{1-x} \mathrm{Ge}_x \mathrm{Bi}_2 \mathrm{Te}_4$}
\newcommand{\kgz}{$K\!\mathit{\varGamma}\!Z$}
\newcommand{\lsoc}{\lambda_\mathrm{SOC}}

\title{Phase transitions, Dirac and Weyl semimetal states in \mgbt{}}
\author[1, *]{A.M.~Shikin}
\author[1, 2]{N.L.~Zaitsev}
\author[1]{T.P.~Estyunina}
\author[1]{D.A.~Estyunin}
\author[1]{A.G.~Rybkin}
\author[1]{D.A.~Glazkova}
\author[3]{I.I.~Klimovskikh}
\author[1]{A.V.~Eryzhenkov}
\author[1,5]{K.A.~Kokh}
\author[1,4]{V.A.~Golyashov}
\author[1,4]{O.E.~Tereshchenko}
\author[6]{S.~Ideta}
\author[6]{Y.~Miyai}
% \author[6]{Y.~Kumar}
\author[7,8]{T.~Iwata}
\author[7]{T.~Kosa}
\author[7,8,9]{K.~Kuroda}
\author[6]{K.~Shimada}
\author[1]{A.V.~Tarasov}
\affil[1]{Saint Petersburg State University, St. Petersburg 198504, Russia}
\affil[2]{Institute of Molecule and Crystal Physics, Subdivision of the Ufa Federal Research Centre of the Russian Academy of Sciences, Ufa 450075, Russia}
\affil[3]{Donostia International Physics Center (DIPC), 20018 Donostia-San Sebasti\'an, Basque Country, Spain}
\affil[4]{Rzhanov Institute of Semiconductor Physics, Siberian Branch, Russian Academy of Sciences, Novosibirsk 630090, Russia}
\affil[5]{Sobolev Institute of Geology and Mineralogy, Siberian Branch, Russian Academy of Sciences, Novosibirsk 630090, Russia}
\affil[6]{Research Institute for Synchrotron Radiation Science, Hiroshima University, Hiroshima 739-0046, Japan}
\affil[7]{Graduate School of Advanced Science and Engineering, Hiroshima University, Higashi-Hiroshima 739-8526, Japan}
\affil[8]{International Institute for Sustainability with Knotted Chiral Meta Matter (WPI-SKCM$^2$), Hiroshima University, Higashi-Hiroshima 739-8526, Japan}
\affil[9]{Research Institute for Semiconductor Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan}
\affil[*]{ashikin@inbox.ru}

\keywords{ARPES, DFT, MnBi2Te4, magnetic topological insulators, Weyl semimetals, doping}
\begin{document}
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    \begin{center}%
    {\LARGE \textbf{Supplementary Information} \par}%
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      {\LARGE \@title \par}%
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    \par
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  \makeatother

  \flushbottom
  \maketitle

  \setcounter{figure}{0} \renewcommand{\thefigure}{S\arabic{figure}}

  \begin{figure}[ht!]
      \centering
      \includegraphics[width=0.8\textwidth]{S1}
      \caption{
        (\textbf{a1}--\textbf{a8}) Bulk band structure calculations of the \mgbt{} primitive cell in the \kgz{} direction
        for different Ge concentrations. Blue (red) points indicate that the Bi $p_z$ orbital contribution at that point
        is greater (lesser) than the corresponding Te $p_z$ contribution.
      }
      \label{fig:S1}
  \end{figure}

  \begin{figure}[ht!]
      \centering
      \includegraphics[width=0.8\textwidth]{S2}
      \caption{
        Theoretically calculated changes in the dispersion dependencies of bulk states for the AFM
        (\textbf{a1}--\textbf{a8}) phase of \mgbt{} with $x = 0.5$ in the \kgz{} direction of the BZ. The modulation of
        the SOC strength $\lsoc$ on the Te and Bi atoms is relative to the initial value, taken as 1. Changes in the
        contributions of the Te $p_z$ and Bi $p_z$ states are shown in red and blue, respectively.
      }
      \label{fig:S2}
  \end{figure}

\end{document}