GdTi3Bi4 shows a giant anomalous Hall conductivity of ~8600 Ohm^{-1} cm^{-1} at 2 K from Berry curvature and spin-cluster textures, with intrinsic and skew-scattering contributions.
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4 Pith papers cite this work. Polarity classification is still indexing.
years
2026 4verdicts
UNVERDICTED 4representative citing papers
GdTi3Bi4 shows a tunable bifurcation of in-plane magnetic anisotropy at 2 K into two 7-degree-offset orientations, revealing hidden bi-oriented AFM order and three distinct domain phases under transverse magnetic fields.
ARPES and XMCD data show Ti bands dominate the electronic structure of these kagome metals, with a small Ti magnetic moment induced in GdTi3Bi4 by proximity to Gd zigzag chains.
In the kagome metal GdTi3Bi4, rotating magnetic fields drive hysteretic switching between two 60-degree-apart CDW domain orientations, mediated by antiferromagnetic spin reorientation via spin-lattice coupling.
citing papers explorer
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Berry curvature induced giant anomalous and spin texture driven Hall responses in the layered kagome antiferromagnet GdTi3Bi4
GdTi3Bi4 shows a giant anomalous Hall conductivity of ~8600 Ohm^{-1} cm^{-1} at 2 K from Berry curvature and spin-cluster textures, with intrinsic and skew-scattering contributions.
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Tunable bifurcation of magnetic anisotropy and bi-oriented antiferromagnetic order in kagome metal GdTi3Bi4
GdTi3Bi4 shows a tunable bifurcation of in-plane magnetic anisotropy at 2 K into two 7-degree-offset orientations, revealing hidden bi-oriented AFM order and three distinct domain phases under transverse magnetic fields.
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Revealing magnetism in the distorted kagome $R$Ti$_3$Bi$_4$ ($R$ = Nd, Sm, Gd) via ARPES and XMCD
ARPES and XMCD data show Ti bands dominate the electronic structure of these kagome metals, with a small Ti magnetic moment induced in GdTi3Bi4 by proximity to Gd zigzag chains.
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Spin-mediated hysteretic switching of unidirectional charge density waves by rotating magnetic fields
In the kagome metal GdTi3Bi4, rotating magnetic fields drive hysteretic switching between two 60-degree-apart CDW domain orientations, mediated by antiferromagnetic spin reorientation via spin-lattice coupling.