TABLE I: Results of the Curie-Weiss analysis for the XMCD spectra of the Zn$_{1}$$_{−}$$_{x}$Co$_{x}$O thin films. Here, C is the Curie constant, θ is the Weiss temperature, M XMCD s and M SQUID s are the saturation magnetizations estimated from the XMCD sum rules and measured by the SQUID, respectively. TABLE II: Results of the Curie-Weiss analysis for the XMCD spectra of the as-grown and annealed Zn$_{0}$$_{.}$$_{9}$Co$_{0}$$_{.}$$_{1}$O thin films deposited at P$_{O2}$ = 10 − 2 Pa. Here, χ is the paramagnetic susceptibility. 15 χ ( µ$_{B}$ /Co T) M XMCD s (10 − $^{2}$µ$_{B}$ /Co) M SQUID s (10 − $^{2}$µ$_{B}$ /Co) As-grown 0.059 3 . 4 ± 0 . 8 2 . 5 ± 0 . 3 Annealed 0.031 1 . 0 ± 0 . 8 1 . 7 ± 0 . 3 Samples C ( µ$_{B}$ K/T) θ (K) M XMCD s (10 − $^{2}$µ$_{B}$ /Co) M SQUID s (10 − $^{2}$µ$_{B}$ /Co) x =0.07 P$_{O2}$ =10 − 4 Pa 3 . 8 ± 0 . 5 − 37 . 17 ± 5 0 . 27 ± 2 . 0 - x =0.10 P$_{O2}$ =10 − 2 Pa 1 . 9 ± 0 . 5 − 12 . 3 ± 5 3 . 4 ± 0 . 8 2 . 5 ± 0 . 3 P$_{O2}$ =10 − 3 Pa 3 . 0 ± 0 . 5 − 37 . 0 ± 5 1 . 6 ± 0 . 8 1 . 4 ± 0 . 3 P$_{O2}$ =10 − 4 Pa 3 . 8 ± 0 . 5 − 8 . 7 ± 5 1 . 7 ± 0 . 8 -