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Electronic excitations and spin interactions in chromium trihalides from embedded many-body wavefunctions.
Yadav, Ravi; Xu, Lei; Pizzochero, Michele; van den Brink, Jeroen; Katsnelson, Mikhail I; Yazyev, Oleg V.
Affiliation
  • Yadav R; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland.
  • Xu L; National Centre for Computational Design and Discovery of Novel Materials (MARVEL), Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland.
  • Pizzochero M; Institute for Theoretical Solid State Physics, IFW Dresden, Dresden, Germany.
  • van den Brink J; Present Address: Physical and Computational Sciences Directorate, Pacific Northwest National Laboratory, Richland, WA USA.
  • Katsnelson MI; School of Engineering and Applied Sciences, Harvard University, Cambridge, MA USA.
  • Yazyev OV; Institute for Theoretical Solid State Physics, IFW Dresden, Dresden, Germany.
NPJ 2D Mater Appl ; 8(1): 56, 2024.
Article in En | MEDLINE | ID: mdl-39219845
ABSTRACT
Although chromium trihalides are widely regarded as a promising class of two-dimensional magnets for next-generation devices, an accurate description of their electronic structure and magnetic interactions has proven challenging to achieve. Here, we quantify electronic excitations and spin interactions in CrX 3 (X = Cl, Br, I) using embedded many-body wavefunction calculations and fully generalized spin Hamiltonians. We find that the three trihalides feature comparable d-shell excitations, consisting of a high-spin 4 A 2 ( t 2 g 3 e g 0 ) ground state lying 1.5-1.7 eV below the first excited state 4 T 2 ( t 2 g 2 e g 1 ). CrCl3 exhibits a single-ion anisotropy A sia = - 0.02 meV, while the Cr spin-3/2 moments are ferromagnetically coupled through bilinear and biquadratic exchange interactions of J 1 = - 0.97 meV and J 2 = - 0.05 meV, respectively. The corresponding values for CrBr3 and CrI3 increase to A sia = -0.08 meV and A sia= - 0.12 meV for the single-ion anisotropy, J 1 = -1.21 meV, J 2 = -0.05 meV and J 1 = -1.38 meV, J 2 = -0.06 meV for the exchange couplings, respectively. We find that the overall magnetic anisotropy is defined by the interplay between A sia and A dip due to magnetic dipole-dipole interaction that favors in-plane orientation of magnetic moments in ferromagnetic monolayers and bulk layered magnets. The competition between the two contributions sets CrCl3 and CrI3 as the easy-plane (A sia + A dip >0) and easy-axis (A sia + A dip <0) ferromagnets, respectively. The differences between the magnets trace back to the atomic radii of the halogen ligands and the magnitude of spin-orbit coupling. Our findings are in excellent agreement with recent experiments, thus providing reference values for the fundamental interactions in chromium trihalides.
Key words

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: NPJ 2D Mater Appl Year: 2024 Document type: Article Affiliation country: Switzerland Country of publication: United kingdom

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: NPJ 2D Mater Appl Year: 2024 Document type: Article Affiliation country: Switzerland Country of publication: United kingdom