“…In this study, the current density is calculated as 1.0 10 10 Á m −2 when a current of 10 mA is applied. Because the current density is approximately 10-50% that of previous studies, [23][24][25][26][27] the domain wall could be displaced due to STT. However, the results in experiment (A) show that the magnetic reversal domain induced by the AOS phenomenon with no electric current did not move or change its shape SB1014-4…”
We experimentally demonstrated electrical detection of All-Optical magnetization switching (AOS) induced by a single femtosecond laser pulse irradiation by measuring alternate rapid changes in anomalous Hall voltage and magneto-optic image pulse by pulse in a Hall-cross shape ferrimagnetic GdFeCo alloy thin film. We also demonstrated that the amplitude of the change in anomalous Hall voltage depended on the position of the AOS-created magnetic domain on the Hall cross. Furthermore, the AOS-created magnetic domains were stable against subsequent current applications in the Hall cross circuit, whereas reversed magnetic domains were not created when the laser pulse was irradiated with a high current. We found that cooperative effect among magnetism, light, and electric current was assumed to have effects on absence of the AOS. Combined the AOS phenomenon and an electrical measurement/control techniques can realize ultrafast, deterministic, and distinguishable applications.
“…In this study, the current density is calculated as 1.0 10 10 Á m −2 when a current of 10 mA is applied. Because the current density is approximately 10-50% that of previous studies, [23][24][25][26][27] the domain wall could be displaced due to STT. However, the results in experiment (A) show that the magnetic reversal domain induced by the AOS phenomenon with no electric current did not move or change its shape SB1014-4…”
We experimentally demonstrated electrical detection of All-Optical magnetization switching (AOS) induced by a single femtosecond laser pulse irradiation by measuring alternate rapid changes in anomalous Hall voltage and magneto-optic image pulse by pulse in a Hall-cross shape ferrimagnetic GdFeCo alloy thin film. We also demonstrated that the amplitude of the change in anomalous Hall voltage depended on the position of the AOS-created magnetic domain on the Hall cross. Furthermore, the AOS-created magnetic domains were stable against subsequent current applications in the Hall cross circuit, whereas reversed magnetic domains were not created when the laser pulse was irradiated with a high current. We found that cooperative effect among magnetism, light, and electric current was assumed to have effects on absence of the AOS. Combined the AOS phenomenon and an electrical measurement/control techniques can realize ultrafast, deterministic, and distinguishable applications.
“…We attribute this to heating effects in the CoGd films that results in an increase of the net angular momentum and thus a decrease of the DW velocity (Supporting Information). Additionally, the Joule heating is also responsible for the lower DW velocities compared to recent studies that reported DW velocities higher than 1000 m s –1 in CoGd-based ferrimagnets , as the heating pushes our CoGd films away from angular momentum compensation. These results demonstrate that the CoGd films we optimized , have low DW pinning and density of natural defects leading to fast DW motion induced by SOTs making these structures ideal to study skyrmion motion.…”
Skyrmion racetrack memories are highly attractive for
next-generation
data storage technologies. Skyrmions are noncollinear spin textures
stabilized by chiral interactions. To achieve a fast-operating memory
device, it is critical to move skyrmions at high speeds. The skyrmion
dynamics induced by spin–orbit torques (SOTs) in the commonly
studied ferromagnetic films is hindered by strong pinning effects
and a large skyrmion Hall effect causing deflection of the skyrmion
toward the racetrack edge, which can lead to information loss. Here,
we investigate the current-induced nucleation and motion of skyrmions
in ferrimagnetic Pt/CoGd/(W or Ta) thin films. We first reveal field-free
skyrmion nucleation mediated by Joule heating. We then achieve fast
skyrmion motion driven by SOTs with velocities as high as 610 m s–1 and a small skyrmion Hall angle |θSkHE| ≲ 3°. Our results show that ferrimagnets are better
candidates for fast skyrmion-based memory devices with low risk of
information loss.
“…The reading module is composed of a doublet of V-shaped gold plasmonic nanoantennas coupled with a magnetic racetrack as a top-cladding on the InP waveguide. A magnetic racetrack enables densely storing of information as up and down magnetization states [18], which can be moved along the racetrack by electrical current [19], [20], [21]. The racetrack is modelled as a multilayer stack (from bottom to top) of 4 nm heavy metal tantalum seed layer, 2 nm platinum layer, 2 nm ferromagnetic cobalt layer with a MO Voigt constant of Q = 0.154-0.100i [22] (responsible for PMOKE in our simulation model), and a 2 nm platinum capping layer.…”
Section: Design Structure and Function Principlementioning
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