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We describe a mechanism by which both a ferroelectric polarization and a magnetization can be created in nonpolar, nonmagnetic materials. Using a combination of phenomenological modeling and first-principles calculations, we demonstrate that ferroelectric polarization, magnetization, or both simultaneously can be transiently induced by an ultrashort laser pulse upon linearly, circularly, or elliptically polarized excitation of phonon modes in γ-LiBO_{2}. The direction and magnitude of the multiferroic polarization can be controlled by the chirality of the laser pulse and the phonon modes, offering a pathway for controlling multiferroicity and magnetoelectricity on ultrafast timescales.
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http://dx.doi.org/10.1103/7lm1-wm3y | DOI Listing |
Adv Mater
September 2025
School of Physics and Astronomy, Tel Aviv University, Tel Aviv, 6997801, Israel.
Graphene layers can assemble in two shifted metastable positions per interface, leading to eight possible structural arrangements in five-layer graphene, six of which correspond to distinct periodic crystals. These polytypes exhibit diverse symmetries, interlayer electronic hybridization, van der Waals adhesion, and optical responses. Arrangements lacking inversion [I] and mirror [M] symmetries host intrinsic polarizations, while those with sufficiently flat electronic bands display orbital magnetization, unconventional superconductivity, and anomalous fractional quantum Hall states.
View Article and Find Full Text PDFACS Appl Mater Interfaces
September 2025
Faculty of Materials Science and Engineering, Kunming University of Science and Technology, Kunming 650093, People's Republic of China.
Emerging phenomena such as the valley Hall effect and layer Hall effect, showing promise for next-generation electronics and valleytronic devices, have attracted considerable attention. However, most studies of the layer Hall effect have been restricted to antiferromagnetic or topological systems. Based on first-principles calculations, we establish a valley-layertronics framework and predict that two-dimensional ScI is a multiferroic material exhibiting substantial spontaneous valley polarization in both its monolayer (93.
View Article and Find Full Text PDFAdv Mater
August 2025
Institute for Advanced Materials Technology, University of Science and Technology Beijing, Beijing, 100083, China.
Double-perovskite ferroelectrics have attracted increasing attention due to their highly tunable structures, multifunctional coupling effects, and potential applications in next-generation nonvolatile ferroelectric semiconductor devices. Here, an atomical-rippled-nanodomains (ARNs) are introduced to BiCoO and SmCoO solid solution double-perovskite film due to its ferroelectric single-domain coupling. By engineering triaxial tensile strain, the ferroelectric ARNs are robustly formed in BiSmCoO double-perovskite films, leading to a large ferroelectric polarization (≈23.
View Article and Find Full Text PDFPhys Rev Lett
August 2025
Tel Aviv University, School of Physics and Astronomy, Tel Aviv 6997801, Israel.
We describe a mechanism by which both a ferroelectric polarization and a magnetization can be created in nonpolar, nonmagnetic materials. Using a combination of phenomenological modeling and first-principles calculations, we demonstrate that ferroelectric polarization, magnetization, or both simultaneously can be transiently induced by an ultrashort laser pulse upon linearly, circularly, or elliptically polarized excitation of phonon modes in γ-LiBO_{2}. The direction and magnitude of the multiferroic polarization can be controlled by the chirality of the laser pulse and the phonon modes, offering a pathway for controlling multiferroicity and magnetoelectricity on ultrafast timescales.
View Article and Find Full Text PDFPhys Chem Chem Phys
August 2025
College of Integrative Studies, Abdullah Al Salem University (AASU), Block 3, Khaldiya, Kuwait.
We present a comprehensive micromagnetic investigation of the spin textures and magnetization dynamics in a thin multi-ferroic CoC MXene flake subjected to external magnetic fields ranging from 0 T to 8 T. At zero field, the system exhibits a complex spin spiral structure, indicative of strong competing magnetic interactions. As the applied magnetic field increases, the spin configurations undergo a continuous topological transition-from a skyrmion lattice to a uniformly magnetized ferromagnetic phase.
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