2020
DOI: 10.1088/1361-6463/ab7038
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Voltage manipulation of magnetic particles using multiferroics

Abstract: Precise control and manipulation of nano-beads have various applications, e.g. cell sorter, 3D printing and nano-motors. In this paper we present an approach in which we use voltage on a piezolecetric substrate in order to reorient the magnetization of a nano-disk. In turn this magnetization drives the dynamic of the nano-beads. This is an energy efficient method to control the nano-beads motion since only voltage is applied to the substrate. The mechanism consists of a Ni disk and three pairs of surface elect… Show more

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Cited by 8 publications
(6 citation statements)
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“…Because the sublattice orientations at remanence are the same, the direction of M inverts upon hydrogen loading/unloading, which accounts for the observed change in sign of the exchange bias field. This functionality, namely voltage control of the net magnetization, would be desirable in a variety of potential applications, such as dipole-coupled nanomagnetic logic 37,38 , reconfigurable magnonic crystals based on magnetostatic spin waves 39,40 and stray field control and steering of fluid-borne particles 41,42 . By replacing the NiO layer with a stray field biasing layer, the preferred direction of M can instead be fixed, allowing for controlling the orientation of N. We achieved this by integrating an L1 0 -FePd layer with bulk perpendicular magnetic anisotropy 43,44 as a stray field pinning layer (Fig.…”
Section: Field-free Net Magnetization and Néel Vector Reversalmentioning
confidence: 99%
“…Because the sublattice orientations at remanence are the same, the direction of M inverts upon hydrogen loading/unloading, which accounts for the observed change in sign of the exchange bias field. This functionality, namely voltage control of the net magnetization, would be desirable in a variety of potential applications, such as dipole-coupled nanomagnetic logic 37,38 , reconfigurable magnonic crystals based on magnetostatic spin waves 39,40 and stray field control and steering of fluid-borne particles 41,42 . By replacing the NiO layer with a stray field biasing layer, the preferred direction of M can instead be fixed, allowing for controlling the orientation of N. We achieved this by integrating an L1 0 -FePd layer with bulk perpendicular magnetic anisotropy 43,44 as a stray field pinning layer (Fig.…”
Section: Field-free Net Magnetization and Néel Vector Reversalmentioning
confidence: 99%
“…In a rotating magnetic field, these bowl‐shaped microrobots exhibit outstanding roll motion performance when approaching the surface of glass plates or other substrates. This is because the friction with the substrate surface will cause greater resistance to the part of the microrobot close to the substrate surface, [ 29 ] and the rotation center of the microrobot will move toward the substrate surface. Therefore, the end of the bowl‐shaped microrobot furthest from the substrate surface moves faster, as shown in Figure 2C (a), and eventually a net displacement will be generated for each revolution to form a rolling motion.…”
Section: Resultsmentioning
confidence: 99%
“…The bi-coupled model has been validated on a Ni system [35]. This model was tested for Terfenol-D [34] and FeGa [36] but such systems has not been develop, therefore lacking validation. The results presented here are first validation for FeGa system.…”
Section: Fea Resultsmentioning
confidence: 99%