2020
DOI: 10.1103/physrevapplied.14.014012
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Charge-To-Spin Conversion Efficiency in Ferromagnetic Nanowires by Spin Torque Ferromagnetic Resonance: Reconciling Lineshape and Linewidth Analysis Methods

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Cited by 16 publications
(12 citation statements)
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“…It is worth mentioning that the lineshape method based on Eq. 2 only provides an estimation of the upper limit of J S /J C due to the resonance-driven spin pumping effect from Py to Pt as reported in a previous work [46,49].…”
Section: St-fmr Measurementsmentioning
confidence: 92%
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“…It is worth mentioning that the lineshape method based on Eq. 2 only provides an estimation of the upper limit of J S /J C due to the resonance-driven spin pumping effect from Py to Pt as reported in a previous work [46,49].…”
Section: St-fmr Measurementsmentioning
confidence: 92%
“…Following the aforementioned procedure, we prepared a series of epitaxial Pt (10)/ Py (8) (Py, Ni 81 Fe 19 ) samples for ST-FMR measurements and both epitaxial Pt (111) (5)/Co(0.8)/Ni(1) and polycrystalline Pt (15)/ Co(0.8)/Ni(1) samples with perpendicular magnetic anisotropy for harmonic measurements (thickness in nanometer throughout the text unless otherwise stated). Note that the choice of Py as the FM layer is motivated by its wide application as an efficient spin detector [15,[45][46][47][48][49][50] and the usage of Co/Ni is due to its spontaneous perpendicular magnetic anisotropy, a prerequisite for harmonic measurements [51,52].…”
Section: Sample Growth and Characterizationmentioning
confidence: 99%
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“…In order to have a large resistance response, we apply an in-plane field at to the current direction. In our measurements, we fix the rf frequency and sweep the external magnetic field from high to low field, 0.6 to 0 T. Further, we modulate the field to increase the signal-to-noise ratio, with a modulation amplitude much less than the resonance linewidth ( ) 21 , 28 .…”
Section: Methodsmentioning
confidence: 99%
“…The curves are offset by 2 µV to make the different frequency spectra visible and align their baseline with the rf frequency on the right-hand axis. The spectra are then fit to the sum of the derivative of Lorentzian and anti-Lorentzian to determine the resonance parameters 21 . The resulting resonance field is indicated by the solid squares in the figure . A fit to the rf frequency-resonance field dispersion with the Kittel model for this geometry 22 is shown as the pink curve in Fig.…”
Section: Nanoconstriction Responsementioning
confidence: 99%