Fig. 3: Second harmonic Hall measurements to obtain hL and hT. | npj 2D Materials and Applications

Fig. 3: Second harmonic Hall measurements to obtain hL and hT.

From: Monolayer WSe2 induced giant enhancement in the spin Hall efficiency of Tantalum

Fig. 3

a Measurement schematic to obtain the SOT effective fields. The magnitude of the external magnetic field (Bext) is swept while its direction is fixed in the XY plane of the film stack, either parallel (ϕB = 90°) or perpendicular (ϕB = 0°) to the current direction. R is obtained by dividing the second harmonic quadrature component of the anomalous Hall voltage by the R.M.S of the AC current excitation. Obtained second harmonic response of the devices made from b stack A, c stack B, and d stack C. The top panel shows measurement results for the ϕB = 90° configuration and the bottom panel shows that for the ϕB = 0° configuration. The longitudinal (hL) and transverse (hT) effective fields are obtained by fitting the high field regions (highlighted in yellow) of the measured curve (black symbols) with the expression given in Eq. 1 (plotted in red line). The required values of RA and HK are obtained previously as shown in Fig. 2. Note here that for the longitudinal configuration, the R curve is anti-symmetric while for the transverse configuration it is symmetric, as expected from the sign change of SOT effective fields with the change in magnetization direction. All extracted parameters are listed in the table shown in e.

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