| publicationDate,title,abstract,id | |
| 2022-01-12,Light and microwave driven spin pumping across FeGaB-BiSb interface,"3-D topological insulators (TI) with large spin Hall conductivity have | |
| emerged as potential candidates for spintronic applications. Here, we report | |
| spin to charge conversion in bilayers of amorphous ferromagnet (FM) | |
| Fe_{78}Ga_{13}B_{9} (FeGaB) and 3-D TI Bi_{85}Sb_{15} (BiSb) activated by two | |
| complementary techniques: spin pumping and ultrafast spin-current injection. DC | |
| magnetization measurements establish the soft magnetic character of FeGaB | |
| films, which remains unaltered in the heterostructures of FeGaB-BiSb. Broadband | |
| ferromagnetic resonance (FMR) studies reveal enhanced damping of precessing | |
| magnetization and large value of spin mixing conductance (5.03 x 10^{19} | |
| m^{-2}) as the spin angular momentum leaks into the TI layer. Magnetic field | |
| controlled bipolar dc voltage generated across the TI layer by inverse spin | |
| Hall effect is analyzed to extract the values of spin Hall angle and spin | |
| diffusion length of BiSb. The spin pumping parameters derived from the | |
| measurements of the femtosecond light-pulse-induced terahertz emission are | |
| consistent with the result of FMR. Kubo-Bastin formula and tight-binding model | |
| calculations shed light on the thickness-dependent spin-Hall conductivity of | |
| the TI films, with predictions that are in remarkable agreement with the | |
| experimental data. Our results suggest that room temperature deposited | |
| amorphous and polycrystalline heterostructures provide a promising platform for | |
| creating novel spin orbit torque devices.",2201.04686v1 | |
| 2024-03-21,Picotesla-sensitivity microcavity optomechanical magnetometry,"Cavity optomechanical systems have enabled precision sensing of magnetic | |
| fields, by leveraging the optical resonance-enhanced readout and mechanical | |
| resonance-enhanced response. Previous studies have successfully achieved | |
| scalable and reproducible microcavity optomechanical magnetometry (MCOM) by | |
| incorporating Terfenol-D thin films into high-quality ($Q$) factor whispering | |
| gallery mode (WGM) microcavities. However, the sensitivity was limited to 585 | |
| pT/Hz$^{1/2}$, over 20 times inferior to those using Terfenol-D particles. In | |
| this work, we propose and demonstrate a high-sensitivity and scalable MCOM | |
| approach by sputtering a FeGaB thin film onto a high-$Q$ SiO$_2$ WGM microdisk. | |
| Theoretical studies are conducted to explore the magnetic actuation constant | |
| and noise-limited sensitivity by varying the parameters of the FeGaB film and | |
| SiO$_2$ microdisk. Multiple magnetometers with different radii are fabricated | |
| and characterized. By utilizing a microdisk with a radius of 355 $\mu$m and a | |
| thickness of 1 $\mu$m, along with a FeGaB film with a radius of 330 $\mu$m and | |
| a thickness of 1.3 $\mu$m, we have achieved a remarkable peak sensitivity of | |
| 1.68 pT/Hz$^{1/2}$ at 9.52 MHz. This represents a significant improvement of | |
| over two orders of magnitude compared with previous studies employing sputtered | |
| Terfenol-D film. Notably, the magnetometer operates without a bias magnetic | |
| field, thanks to the remarkable soft magnetic properties of the FeGaB film. | |
| Furthermore, as a proof-of-concept, we have demonstrated the real-time | |
| measurement of a pulsed magnetic field simulating the corona current in a | |
| high-voltage transmission line using our developed magnetometer. These | |
| high-sensitivity magnetometers hold great potential for various applications, | |
| such as magnetic induction tomography and corona current monitoring.",2403.14301v1 | |
| 2015-08-28,Control of magnetic relaxation by electric-field-induced ferroelectric phase transition and inhomogeneous domain switching,"Electric-field modulation of magnetism in strain-mediated multiferroic | |
| heterostructures is considered a promising scheme for enabling memory and | |
| magnetic microwave devices with ultralow power consumption. However, it is not | |
| well understood how electric-field-induced strain influences magnetic | |
| relaxation, an important physical process for device applications. Here we | |
| investigate resonant magnetization dynamics in ferromagnet/ferrolectric | |
| multiferroic heterostructures, FeGaB/PMN-PT and NiFe/PMN-PT, in two distinct | |
| strain states provided by electric-field-induced ferroelectric phase | |
| transition. The strain not only modifies magnetic anisotropy but also magnetic | |
| relaxation. In FeGaB/PMN-PT, we observe a nearly two-fold change in intrinsic | |
| Gilbert damping by electric field, which is attributed to strain-induced tuning | |
| of spin-orbit coupling. By contrast, a small but measurable change in extrinsic | |
| linewidth broadening is attributed to inhomogeneous ferroelastic domain | |
| switching during the phase transition of the PMN-PT substrate.",1508.07290v2 | |
| 2022-01-11,Resonant Precession of Magnetization and Precession -- Induced DC voltages in FeGaB Thin Films,"Measurements of frequency dependent ferromagnetic resonance (FMR) and spin | |
| pumping driven dc voltage (V_{dc}) are reported for amorphous films of | |
| Fe_{78}Ga_{13}B_{9} (FeGaB) alloy to address the phenomenon of self-induced | |
| inverse spin Hall effect (ISHE) in plain films of metallic ferromagnets. The | |
| V_{dc} signal, which is antisymmetric on field reversal, comprises of symmetric | |
| and asymmetric Lorentzians centered around the resonance field. Dominant role | |
| of thin film size effects is seen in setting the magnitude of static | |
| magnetization, V_{dc} and dynamics of magnetization precession in thinner films | |
| (\leq 8 nm). The film thickness dependence of magnetization parameters | |
| indicates the presence of a magnetically disordered region at the | |
| film-substrate interface, which may promote preferential flow of spins | |
| generated by the precessing magnetization towards the substrate. However, the | |
| V_{dc} signal also draws contributions from rectification effects of a \approx | |
| 0.4 \% anisotropic magnetoresistance and a large (\approx 54 n\Omega.m) | |
| anomalous Hall resistivity (AHR) of these films which ride over the effect of | |
| spin-orbit coupling driven spin-to-charge conversion near the film-substrate | |
| interface. We have addressed these data in the framework of the existing | |
| theories of electrodynamics of a ferromagnetic film subjected to | |
| radio-frequency field in a coplanar waveguide geometry. Our estimation of the | |
| self-induced ISHE for the sample with 54 n\Omega.m AHR shows that it may | |
| contribute significantly (\approx 90\%) to the measured symmetric voltage. This | |
| study is expected to be very useful for fully understanding the spin pumping | |
| induced dc voltages in metallic ferromagnets with disordered interfaces and | |
| large anomalous Hall effect.",2201.03739v1 | |
| 2014-11-22,Quantification of the spin-Hall anti-damping torque with a resonance spectrometer,"We present a simple technique using a cavity-based resonance spectrometer to | |
| quantify the anti-damping torque due to the spin Hall effect. Modification of | |
| ferromagnetic resonance is observed as a function of small DC current in | |
| sub-mm-wide strips of bilayers, consisting of magnetically soft FeGaB and | |
| strong spin-Hall metal Ta. From the detected current-induced linewidth change, | |
| we obtain an effective spin Hall angle of 0.08-0.09 independent of the magnetic | |
| layer thickness. Our results demonstrate that a sensitive resonance | |
| spectrometer can be a general tool to investigate spin Hall effects in various | |
| material systems, even those with vanishingly low conductivity and | |
| magnetoresistance.",1411.6166v1 | |
| 2021-12-10,Enhanced Planar Antenna Efficiency Through Magnetic Thin-Films,"This work proposes to use magnetic material as the substrate of planar | |
| antennas to overcome the platform effect caused by the conducting ground plane. | |
| The upper bound of the radiation efficiency of an electric-current-driven | |
| low-profile antenna is theoretically derived, which is inversely proportional | |
| to the Gilbert damping factor of the magnetic material. Meanwhile, the | |
| improvement of radiation due to the use of magnetic material is demonstrated by | |
| a three-dimensional (3D) multiphysics and multiscale time-domain model. The | |
| simulation results match the theoretical derivation, showing 25% radiation | |
| efficiency from a planar antenna backed by a FeGaB thin film with 2.56 um | |
| thickness. Furthermore, for conductive ferromagnetic materials, it is shown | |
| that the eddy current loss can be well suppressed by laminating the thin film | |
| into multiple layers. The radiation efficiency of the modeled antenna with a | |
| conductive ferromagnetic substrate is improved from 2.2% to 11.8% by dividing | |
| the substrate into 10 layers, with a ferromagnetic material fill factor of 93%.",2201.04932v1 | |