期刊
PHYSICAL REVIEW B
卷 106, 期 3, 页码 -出版社
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.106.035103
关键词
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资金
- National Science Foundation [ECCS-1952957]
- U.S. Department of Energy, Office of Basic Energy Sciences, Division of Materials Sciences and Engineering [DEFG02-07ER46438]
- Gordon and Betty Moore Foundation's EPiQS Initiative [GBMF9069]
This study shows that magnetism in the chiral helimagnet Cr1/3NbS2 can be induced by an ultrafast optical pulse. The laser pulse excitation leads to a phase transition from the chiral helimagnetic phase to a chiral conical helimagnetic phase. The mechanism behind this observation is further explained through ab initio density functional calculations and the resonant magnon-phonon coupling.
Chiral helimagnetic materials have recently attracted much attention for spintronic applications due to their long-range helical magnetic order, topological spin textures, and potential for hosting skyrmions. Their robust spin texture would provide a new concept of ultrafast magnetic memory if it can be controlled by an ultrafast optical pulse. Using time-resolved magneto-optical Kerr spectroscopy, we show that magnetism in the single-crystalline chiral helimagnet Cr1/3NbS2 can be induced by an ultrafast optical pulse. At low temperatures and in the absence of magnetic fields, Cr1/3NbS2 exhibits a chiral helical magnetic phase with a long-range helical spin order, but it contains zero net magnetization. However, after the laser pulse excitation we observe magnetization forming over tens of picoseconds, far exceeding the duration of the laser pulse. We attribute this peculiar behavior to a laser-induced phase transition from the chiral helimagnetic phase, with zero net magnetization, to a chiral conical helimagnetic phase, with finite magnetization. Ab initio density functional calculations provide a detailed microscopic picture of the mechanism behind the observation. The resonant magnon-phonon coupling with specific phonons leads to an elastic deformation of the chiral helimagnetic phase. Finally, at finite magnetic fields, the net magnetization is excited by the laser pulse and precesses around the equilibrium position, leading to anomalous magnetization precession as a function of the external magnetic field at specific magnetic phases.
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