SDW transition of Fe1 zigzag chains and metamagnetic transition of Fe2 in TaFe$_{1+y}$Te$_3$
R. H. Liu, M. Zhang, P. Cheng, Y. J. Yan, Z. J. Xiang, J. J. Ying, X., F. Wang, A. F. Wang, G. J. Ye, X. G. Luo, X. H. Chen

TL;DR
This study investigates the magnetic phase transitions in TaFe$_{1+y}$Te$_3$, revealing a SDW-type AFM order in Fe1 zigzag chains and a field-induced spin-flop transition of interstitial Fe2, with implications for understanding Fe-based magnetic materials.
Contribution
It provides a detailed analysis of the AFM order and spin-flop transition in Fe1 and Fe2, highlighting the coupling mechanisms and magnetic structure in TaFe$_{1+y}$Te$_3$, a novel Fe-based compound.
Findings
High-temperature AFM transition is SDW-type.
Fe2 undergoes a spin-flop transition at a coercive field.
Resistivity drops sharply across the spin-flop transition.
Abstract
We systematically study the AFM order of Fe1 zigzag chains and spin-flop of excess Fe2 under high magnetic field H through the susceptibility, magnetoresistance (MR), Hall effect and specific heat measurements in high-quality single crystal TaFeTe. These properties suggest that the high temperature AFM transition of the TaFeTe layers should be a SDW-type AFM order. Below T, Fe1 antiferromangetic zigzag chains will induce a inner magnetic field \textbf{H} to interstitial Fe2 and lead Fe2 also forms an AFM alignment, in which the magnetic coupling strength between Fe1 and Fe2 is enhanced by decreasing temperature. On the other hand, the external magnetic field \textbf{H} inclines to tune interstitial Fe2 to form FM alignment along \textbf{H}. When \textbf{H} arrives at the "coercive" field H, which is able to break the coupling…
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