Fig. 4: Transport properties of the Ru0.8Cr0.2O2 film grown on TiO2 (110).
From: Emergent zero-field anomalous Hall effect in a reconstructed rutile antiferromagnetic metal
a Hall conductivity with magnetic field dependence at 3 K. Insets show the Hall configuration (left) and an expanded view of the low-field region (right). σHall, Hall vector. b Anomalous Hall conductivity at 3 K with a dependence on the magnetic moment (M). The σxyAHE was obtained by subtracting a field-linear-dependent ordinary Hall contribution from σxy. M was measured by an MPMS at 3 K. c Anomalous Hall conductivity derived from the canting moment (i.e., σxyM) and the antiferromagnetic ___domain (i.e., σxyAF) in Ru0.8Cr0.2O2 (110) with a dependence on magnetic field sweeping at 3 K. The magnetic moment is shown by a dashed line. d Temperature-dependent σxyM and σxyAF. The data at 7 T are used.
