Fig. 6: Angular dependence of the SdH oscillations for the SrRuO3 film with t = 10 nm using the mid-pulse magnets.
From: High-mobility two-dimensional carriers from surface Fermi arcs in magnetic Weyl semimetal films
a Angular dependence of the background-subtracted SdH oscillations at 0.7 K with B (10 T < B < 52 T) for the SrRuO3 film with t = 10 nm, measured by the mid-pulse magnet. These spectra were smoothed (see the Sec. III of the supplementary information). The arrows indicate the quantum limit, which is the inverse value of the FFT frequency in c. b Angular dependence of the FFT spectra of SdH oscillations at 0.7 K for the film with t = 10 nm. The dashed line is a guide for the peak shift. c Angular dependence of the FFT frequency. Here, the data obtained by the long-pulse magnet are also shown. The dashed line is the fitting of a two-dimensional angular dependence (~1/cos(90°−θ)).
