Chiral Magnetism: Coupling Static and Dynamic Chirality

The synthesis, structure, magnetic properties and magnetic structure of two molecular chiral magnets and one inorganic chiral magnet are presented. In magnetic crystals belonging to the Sohncke group, which includes the chiral group, the chiral non-collinear spin structure is achieved through Dzyaloshinsky-Moriya interactions in addition to the usual exchange spin interactions and dipole-dipole spin interactions. Experimentally, a chiral helical magnetic (CHM) structure is observed as the ground state in most of this category of uniaxial chiral magnets as a non-collinear spin structure. CHM structure transforms into a chiral spin soliton (CS) magnetic structure in a magnetic field. The (CS) magnetic structure forms a chiral spin soliton lattice (CSL) magnetic structure when the nearest neighbor magnetic interaction is ferromagnetic. Since the CHM and CSL magnetic structures are topologically protected, they are not affected by defects and are therefore extremely stable. A series of studies have revealed that the chiral magnetic structure is perfectly coupled to the non-symmetric crystal structure. It was also found that the CHM and CSL magnetic structures are macroscopic spin-phase coherent states.

Automated summary

The synthesis, structure, magnetic properties, and magnetic structure of two molecular chiral magnets and one inorganic chiral magnet are discussed. The chiral non-collinear spin structure is achieved through the Dzyaloshinsky-Moriya interactions, and the transition from CHM structure to CSL structure is observed experimentally. The chiral magnetic structures are found to be topologically protected and exhibit extremely stability due to the lack of defects affecting them.