Chalcogen Doping Effect on the Insulator-to-Metal Transition in GdPS
arXiv:2603.24762 · doi:10.1016/j.jallcom.2026.187404
Abstract
Topological semimetals offer a rich platform for exploring massless fermion physics and realizing exotic properties with potential technological applications. GdPS, a magnetic semiconductor derived from the nodal-line semimetal ZrSiS family, exhibits a field-induced insulator-to-metal transition driven by exchange splitting. This transition is accompanied by an unusual, isotropic, and gigantic negative magnetoresistance, attributed to negligible magnetic anisotropy resulting from the weak spin-orbit coupling of half-filled Gd3+ 4f orbitals and light S atoms. In this work, we investigate Se substitution, which is expected to enhance spin-orbit coupling. Indeed, we observe slightly increased magnetic anisotropy in magnetotransport. Moreover, Se substitution suppresses the field-induced insulator-to-metal transition, likely due to an enlarged band gap that demands a higher exchange splitting to close. These findings provide deeper insights into the interplay between spin-orbit coupling, magnetic anisotropy, and transport behavior in GdPS, offering guidance for future materials design for desired functionalities.
References in corpus (39)
- Weyl and Dirac Semimetals in Three Dimensional Solids
- Topological Materials: Weyl Semimetals
- Dirac Cone Protected by Non-Symmorphic Symmetry and 3D Dirac Line Node in ZrSiS
- Topological nodal-line fermions in ZrSiSe and ZrSiTe
- Observation of Topological Nodal Fermion Semimetal Phase in ZrSiS
- Electronic Transport and quantum oscillation of Topological Semimetals
- Unexpected Dirac-Node Arc in the Topological Line-Node Semimetal HfSiS
- Two-Dimensional Oxide Topological Insulator With Iron-Pnictide Superconductor LiFeAs Structure
- Dirac Line-nodes and Effect of Spin-orbit Coupling in Non-symmorphic Critical Semimetal MSiS (M=Hf, Zr)
- Tunable Weyl and Dirac states in the nonsymmorphic compound
- Tunability of the topological nodal-line semimetal phase in ZrSiX-type materials
- Non-symmorphic band degeneracy at the Fermi level in ZrSiTe
- Observation of topological nodal-line fermionic phase in GdSbTe
- Emergence of topological bands on the surface of ZrSnTe crystal
- Two-dimensional Spin-Orbit Dirac Point in Monolayer HfGeTe
- Magnetotransport properties and evidence of topological insulating state in LaSbTe
- Controlling magnetic exchange and anisotropy by non-magnetic ligand substitution in layered MPX3 (M = Ni, Mn; X = S, Se)
- Quantum oscillation studies of topological semimetal candidate ZrGeM (M=S, Se, Te)
- Band Engineering of Dirac Semimetals using Charge Density Waves
- Spin-valley locking, bulk quantum Hall effect and chiral surface state in a noncentrosymmetric Dirac semimetal BaMnSb
- Large negative magnetoresistance in the new antiferromagnetic rare-earth dichalcogenide EuTe
- Observation of Gapless Dirac Surface States in ZrGeTe
- Magnetic and electronic properties of a topological nodal line semimetal candidate: HoSbTe
- Topological electronic structure in the antiferromagnet HoSbTe
- Electronic and Magnetic Properties of Topological Semimetal Candidate NdSbTe
- Complex magnetic phases enriched by charge density waves in topological semimetals GdSb_xTe_{2-x-δ}
- Evolving Devil's staircase magnetization from tunable charge density waves in nonsymmorphic Dirac semimetals
- Observation of multiple nodal-lines in SmSbTe
- Quantum oscillation evidence of topological semimetal phase in ZrSnTe
- Possible pressure-induced topological quantum phase transition in the nodal line semimetal ZrSiS
- Experimental evidence of crystal symmetry protection for the topological nodal line semimetal state in ZrSiS
- Competing magnetic phases in LnSbTe (Ln = Ho and Tb)
- Evolution of Electronic and Magnetic Properties in Topological Semimetal SmSbxTe2-x
- Colossal negative magnetoresistance in the complex charge density wave regime of an antiferromagnetic Dirac semimetal
- Evolution of Magnetism in Magnetic Topological Semimetal NdSbTe
- On the magnetic structures of 1:1:1 stoichiometric topological phases LnSbTe (Ln = Pr, Nd, Dy and Er)
- Insulator-to-Metal Transition and Isotropic Gigantic Magnetoresistance in Layered Magnetic Semiconductors
- Large Negative Magnetoresistance in off-Stochiometric Topological Material PrSbTe
- Evolution of Magnetoresistance in the magnetic topological semimetals NdSbxTe2-x