Figures & data
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Figure 1. (a) θ–2θ X-ray diffractograms of 40.3 nm (red) and 156 nm (black) thick (Cr0.5Mn0.5)2GaC films. (b–e) Scanning electron microscopy images of (Cr0.5Mn0.5)2GaC film surfaces for film thickness d = 12.5, 20.8, 40.3 and 156 nm.
![Figure 1. (a) θ–2θ X-ray diffractograms of 40.3 nm (red) and 156 nm (black) thick (Cr0.5Mn0.5)2GaC films. (b–e) Scanning electron microscopy images of (Cr0.5Mn0.5)2GaC film surfaces for film thickness d = 12.5, 20.8, 40.3 and 156 nm.](/cms/asset/dcf0eebd-2325-4e29-b1e7-2b8800cca1c5/tmrl_a_1570980_f0001_oc.jpg)
Figure 2. (a) FMR spectra of (Cr0.5Mn0.5)2GaC films with different thickness measured at the temperature of T = 110 K. The ‘noisy’ features from 0.31 to 0.37 T are electron paramagnetic resonance (EPR) signals from impurities in the MgO substrate. (b) Temperature dependence of the FMR field for different thicknesses of (Cr0.5Mn0.5)2GaC films, solid lines are a guide to the eye.
![Figure 2. (a) FMR spectra of (Cr0.5Mn0.5)2GaC films with different thickness measured at the temperature of T = 110 K. The ‘noisy’ features from 0.31 to 0.37 T are electron paramagnetic resonance (EPR) signals from impurities in the MgO substrate. (b) Temperature dependence of the FMR field Hr for different thicknesses of (Cr0.5Mn0.5)2GaC films, solid lines are a guide to the eye.](/cms/asset/318cf836-a7d5-4234-8962-ce1e174a46ee/tmrl_a_1570980_f0002_oc.jpg)