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Correlation between magnetism and lattice dynamics for cubic FeGe under pressure

R. A. Tonacatl-Monez, R. Heid, O. De la Peña-Seaman

TL;DR

This study investigates how magnetism interacts with lattice dynamics in ferromagnetic cubic FeGe under pressure using a spin-scaling exchange-correlation approach to align the predicted critical pressure $p_c$ with experiment. By combining DFT with phonon calculations and electron-phonon coupling analyses, the work shows that reducing the magnetic moment via ssxc mitigates the R-point phonon anomaly and associated linewidths, with these features disappearing as pressure rises toward and beyond $p_c$. The momentum dependence of electron-phonon matrix elements, rather than Fermi-surface nesting, drives the observed linewidth behavior, linking the magnetism to lattice dynamics through e-ph coupling. These results reveal a distinct mechanism in FeGe for magnetism–lattice dynamics coupling, offering a pathway to tune magnetic and vibrational properties under pressure and contrasting with Mn$_{1-x}$Fe$_x$Si where nesting dominates.

Abstract

This first-principles study investigates the structural, electronic, lattice dynamical properties, and electron-phonon coupling in ferromagnetic cubic B20 FeGe under applied pressure. The implemented spin-scaling exchange-correlation (ssxc) approach allowed to modify the magnetic moment and ferromagnetic phase energetics using a single scaling parameter, thereby yielding an adjustment of the critical pressure ($p_c$) to its experimental value. The ssxc scheme resulted in a subtle energy shift of the electronic bands in the spin-up channel, and reduced the magnetic moment, bringing it closer to the experimentally reported value. Application of the ssxc approach to phonon dispersion and electron-phonon interaction resulted in a slight mitigation of the pronounced softening and large linewidths of the lowest-frequency acoustic branch close to the $R$-point, typically observed with standard DFT calculations. With increasing pressure, phonon anomaly and linewidths diminish significantly and practically disappear at $p_c$ and beyond. This trend parallels the pressure dependence of the magnetic moment. A comparative analysis of the electronic joint density of states with the phonon linewidths revealed that the momentum dependence of linewidths around the $R$-point closely follow the momentum dependence of the electron-phonon matrix elements. This indicates that the correlation between magnetic moment and linewidths under applied pressure originates from the electron-phonon matrix elements, presenting a distinct scenario compared to other B20 family members, where nesting plays a more dominating role.

Correlation between magnetism and lattice dynamics for cubic FeGe under pressure

TL;DR

This study investigates how magnetism interacts with lattice dynamics in ferromagnetic cubic FeGe under pressure using a spin-scaling exchange-correlation approach to align the predicted critical pressure with experiment. By combining DFT with phonon calculations and electron-phonon coupling analyses, the work shows that reducing the magnetic moment via ssxc mitigates the R-point phonon anomaly and associated linewidths, with these features disappearing as pressure rises toward and beyond . The momentum dependence of electron-phonon matrix elements, rather than Fermi-surface nesting, drives the observed linewidth behavior, linking the magnetism to lattice dynamics through e-ph coupling. These results reveal a distinct mechanism in FeGe for magnetism–lattice dynamics coupling, offering a pathway to tune magnetic and vibrational properties under pressure and contrasting with MnFeSi where nesting dominates.

Abstract

This first-principles study investigates the structural, electronic, lattice dynamical properties, and electron-phonon coupling in ferromagnetic cubic B20 FeGe under applied pressure. The implemented spin-scaling exchange-correlation (ssxc) approach allowed to modify the magnetic moment and ferromagnetic phase energetics using a single scaling parameter, thereby yielding an adjustment of the critical pressure () to its experimental value. The ssxc scheme resulted in a subtle energy shift of the electronic bands in the spin-up channel, and reduced the magnetic moment, bringing it closer to the experimentally reported value. Application of the ssxc approach to phonon dispersion and electron-phonon interaction resulted in a slight mitigation of the pronounced softening and large linewidths of the lowest-frequency acoustic branch close to the -point, typically observed with standard DFT calculations. With increasing pressure, phonon anomaly and linewidths diminish significantly and practically disappear at and beyond. This trend parallels the pressure dependence of the magnetic moment. A comparative analysis of the electronic joint density of states with the phonon linewidths revealed that the momentum dependence of linewidths around the -point closely follow the momentum dependence of the electron-phonon matrix elements. This indicates that the correlation between magnetic moment and linewidths under applied pressure originates from the electron-phonon matrix elements, presenting a distinct scenario compared to other B20 family members, where nesting plays a more dominating role.
Paper Structure (9 sections, 1 equation, 9 figures, 1 table)

This paper contains 9 sections, 1 equation, 9 figures, 1 table.

Figures (9)

  • Figure 1: Evolution of (a) the enthalpy difference (between NM and FM phases) as a function of pressure, where a negative value indicates a more stable magnetic phase, and (b) magnetic moment for the FM ssp and ssxc schemes. The vertical lines indicate the critical pressure ($p_c$): $28.7$ GPa for ssxc with $s=0.979$, and $35.3$ GPa for ssp.
  • Figure 2: Determined critical pressure ($p_c$) and magnetic moment as a function of the ssxc parameter $s$. The dotted horizontal line indicates the experimental $p_c$ value barla.
  • Figure 3: Electronic band structure and density of states of FM FeGe ($p=0$ GPa), for both spin-channels, comparing ssp and ssxc (with $s=0.979$) schemes. The related first Brillouin of the simple cubic structure zone is presented as an inset.
  • Figure 4: Spin-polarized density of states (DOS) for FM FeGe, obtained with the ssxc scheme (using $s=0.979$) without applied pressure, showing the contribution by atom (in the unit cell).
  • Figure 5: Spin-polarized DOS of two different applied pressure values, $0$ GPa and $35$ GPa, calculated under the ssxc scheme with $s=0.979$.
  • ...and 4 more figures