33,518 research outputs found
Electrical detection of ferromagnetic resonance in ferromagnet/n-GaAs heterostructures by tunneling anisotropic magnetoresistance
We observe a dc voltage peak at ferromagnetic resonance (FMR) in samples
consisting of a single ferromagnetic (FM) layer grown epitaxially on the
GaAs (001) surface. The FMR peak is detected as an interfacial
voltage with a symmetric line shape and is present in samples based on various
FM/-GaAs hetrostructures, including CoMnSi/-GaAs,
CoFeSi/-GaAs and Fe/-GaAs. We show that the interface bias voltage
dependence of the FMR signal is identical to that of the tunneling anisotropic
magnetoresistance (TAMR) over most of the bias range. Furthermore, we show how
the precessing magnetization yields a dc FMR signal through the TAMR effect and
how the TAMR phenomenon can be used to predict the angular dependence of the
FMR signal. This TAMR-induced FMR peak can be observed under conditions where
no spin accumulation is present and no spin-polarized current flows in the
semiconductor.Comment: 4 pages, 4 figure
Spin torque ferromagnetic resonance with magnetic field modulation
We demonstrate a technique of broadband spin torque ferromagnetic resonance
(ST-FMR) with magnetic field modulation for measurements of spin wave
properties in magnetic nanostructures. This technique gives great improvement
in sensitivity over the conventional ST-FMR measurements, and application of
this technique to nanoscale magnetic tunnel junctions (MTJs) reveals a rich
spectrum of standing spin wave eigenmodes. Comparison of the ST-FMR
measurements with micromagnetic simulations of the spin wave spectrum allows us
to explain the character of low-frequency magnetic excitations in nanoscale
MTJs.Comment: Also see: http://faculty.sites.uci.edu/krivorotovgroup
A fundamental relation between mass, SFR and metallicity in local and high redshift galaxies
We show that the mass-metallicity relation observed in the local universe is
due to a more general relation between stellar mass M*, gas-phase metallicity
and SFR. Local galaxies define a tight surface in this 3D space, the
Fundamental Metallicity Relation (FMR), with a small residual dispersion of
~0.05 dex in metallicity, i.e, ~12%. At low stellar mass, metallicity decreases
sharply with increasing SFR, while at high stellar mass, metallicity does not
depend on SFR. High redshift galaxies, up to z~2.5 are found to follow the same
FMR defined by local SDSS galaxies, with no indication of evolution. The
evolution of the mass-metallicity relation observed up to z=2.5 is due to the
fact that galaxies with progressively higher SFRs, and therefore lower
metallicities, are selected at increasing redshifts, sampling different parts
of the same FMR. By introducing the new quantity mu_alpha=log(M*)-alpha
log(SFR), with alpha=0.32, we define a projection of the FMR that minimizes the
metallicity scatter of local galaxies. The same quantity also cancels out any
redshift evolution up to z~2.5, i.e, all galaxies have the same range of values
of mu_0.32. At z>2.5, evolution of about 0.6 dex off the FMR is observed, with
high-redshift galaxies showing lower metallicities. The existence of the FMR
can be explained by the interplay of infall of pristine gas and outflow of
enriched material. The former effect is responsible for the dependence of
metallicity with SFR and is the dominant effect at high-redshift, while the
latter introduces the dependence on stellar mass and dominates at low redshift.
The combination of these two effects, together with the Schmidt-Kennicutt law,
explains the shape of the FMR and the role of mu_0.32. The small metallicity
scatter around the FMR supports the smooth infall scenario of gas accretion in
the local universe.Comment: 14 pages, new version accepted by MNRA
Ferromagnetic resonance study of Co/Pd/Co/Ni multilayers with perpendicular anisotropy irradiated with Helium ions
We present a ferromagnetic resonance (FMR) study of the effect of Helium ion
irradiation on the magnetic anisotropy, the linewidth and the Gilbert damping
of a Co/Ni multilayer coupled to Co/Pd bilayers. The perpendicular magnetic
anisotropy decreases linearly with He ion fluence, leading to a transition to
in-plane magnetization at a critical fluence of 5x10^{14} ions/cm^2. We find
that the damping is nearly independent of fluence but the FMR linewidth at
fixed frequency has a maximum near the critical fluence, indicating that the
inhomogeneous broadening of the FMR line is a non-monotonic function of the He
ion fluence. Based on an analysis of the angular dependence of the FMR
linewidth, the inhomogeneous broadening is associated with spatial variations
in the magnitude of the perpendicular magnetic anisotropy. These results
demonstrate that ion irradiation may be used to systematically modify the
magnetic anisotropy and distribution of magnetic anisotropy parameters of
Co/Pd/Co/Ni multilayers for applications and basic physics studies
Ferromagnetic resonance imaging of Co films using magnetic resonance force microscopy
Lateral one-dimensional imaging of cobalt (Co) films by means of microscopic ferromagnetic resonance (FMR) detected using the magnetic resonance force microscope (MRFM) is demonstrated. A novel approach involving scanning a localized magnetic probe is shown to enable FMR imaging in spite of the broad resonance linewidth. We introduce a spatially selective local field by means of a small, magnetically polarized spherical crystallite of yttrium iron garnet (YIG). Using MRFM-detected FMR signals from a sample consisting of two Co films, we can resolve the ∼20 μm lateral separation between the films. The results can be qualitatively understood by consideration of the calculated spatial profiles of the magnetic field generated by the YIG sphere
Dual-frequency ferromagnetic resonance
We describe a new experimental technique to investigate coupling effects
between different layers or modes in ferromagnetic resonance (FMR). Dual FMR
frequencies are excited (2-8 GHz) simultaneously and detected selectively in a
broadband RF circuit, using lock-in amplifier detection at separate modulation
frequencies.Comment: 4 pages, 4 figures, accepted by "Review of Scientific Instruments",
200
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