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Updated: Jan 11, 2026

Author Spotlight: Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
Published on: June 9, 2023
Magnetizing phosphorene via transition-metal doping: unveiling unconventional compensated magnetism
Guruprasad Sahoo1, Ajit Kumar Jena2, Durgamadhab Pati1
1Department of Physics, Narasingha Choudhury Autonomous College, Jajpur 755001, Odisha, India.
None:
This study explores the magnetic and electronic properties of 3dtransition metal doped phosphorene monolayers using first principles calculations, with a focus on their potential two dimensional (2D) spintronics applications. We identify Ti, V, Cr, Mn and Fe doping induces magnetism in otherwise nonmagnetic phosphorene with respective magnetic moment of 1μB, 2μB, 3μB, 4μBand 3μBper dopant. The induced magnetic moment is attributed to the intra-atomic charge transfer (from 4sto 3d) and subsequent spin-dependent electronic redistribution at the dopant site. Among the doped systems, Cr and Mn doped phosphorene exhibit ferromagnetic (FM) ground states with critical temperatures of 217.8 K and 733.5 K, respectively. On the other hand, Ti, V and Fe doping favor antiferromagnetic ordering with relatively lower critical temperatures, 147.1 K, 58.7 K and 52.2 K, respectively. While Ti and V doping retains semiconducting character with a band gap of 0.31 eV and 0.17 eV, respectively, the Cr, Mn and Fe doped systems are found to be metallic in nature. Notably, the Fe and V doped phosphorene monolayers exhibit unconventional compensated magnetism that combines the privilege of both ferromagnetism (spin-split band structure) and antiferromagnetism (zero net magnetization). While the former doped system is identified as a quasi-altermagnetic material, the latter one is predicted to be a Luttinger compensated magnetic semiconductor. Since they can facilitate an effective spin transport without any unwanted FM coupling, therefore, the Fe and V doped phosphorene monolayers are the preferred superior materials for applications in next-generation 2D spintronics.
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