Helical magnetic order and Fermi surface nesting in noncentrosymmetric ScFeGe
Sunil K. Karna, Damien Tristant, J. K. Hebert, Guang‐Han Cao, Ramakanta Chapai, W. Adam Phelan, Qiang Zhang, Yan Wu, Chetan Dhital, Y. Li, Huibo Cao, Wei Tian, Clarina dela Cruz, A. A. Aczel, O. Zaharko, A. Kh. Khasanov, Michael A. McGuire, Amitava Roy, Weiwei Xie, D. A. Browne, Ilya Vekhter, Vincent Meunier, W. A. Shelton, P. W. Adams, Phillip Sprunger, David P. Young, Rui Jin, J. F. DiTusa
Abstract
An investigation of the structural, magnetic, thermodynamic, and charge transport properties of noncentrosymmetric hexagonal ScFeGe reveals it to be an anisotropic metal with a transition to a weak itinerant incommensurate helimagnetic state below ${T}_{N}=36$ K. Neutron diffraction measurements discovered a temperature and field independent helical wave vector $\mathbit{k}$ = (0 0 0.193) with magnetic moments of 0.53 ${\ensuremath{\mu}}_{B}$ per Fe confined to the $ab$ plane. Density functional theory calculations are consistent with these measurements and find several bands that cross the Fermi level along the $c$ axis with a nearly degenerate set of flat bands just above the Fermi energy. The anisotropy found in the electrical transport is reflected in the calculated Fermi surface, which consists of several warped flat sheets along the $c$ axis with two regions of significant nesting, one of which has a wave vector that closely matches that found in the neutron diffraction. The electronic structure calculations, along with a strong anomaly in the $c$ -axis conductivity at ${T}_{N}$, signal a Fermi surface driven magnetic transition, similar to that found in spin density wave materials. Magnetic fields applied in the $ab$ plane result in a metamagnetic transition with a threshold field of $\ensuremath{\approx}6.7$ T along with a sharp, strongly temperature dependent discontinuity and a change in sign of the magnetoresistance for in-plane currents. Thus, ScFeGe is an ideal system to investigate the effect of in-plane magnetic fields on a helimagnet with a $c$ -axis propagation vector, where the relative strength of the magnetic interactions and anisotropies determine the topology and magnetic structure.