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. 2023 Aug 16;14(35):9389–9399. doi: 10.1039/d3sc03089j

Fig. 7. (a) HYSCORE performed at 5 K and g spectral position for 1.0C60@Cu0.1-PCN-223 plotted after data processing. (b) Rabi oscillations recorded for 1.0C60@Cu0.1-PCN-223 at 20 K and g spectral position applying various microwave power attenuation. (c) Fast Fourier transform (FFT) of the Rabi oscillations with an asterisk denoting Larmor frequency of proton spins ≈13.5 MHz while arrows denote Rabi frequencies. (d) Linear dependence of the Rabi frequency, νR, as a function of the oscillating microwave field, B1, calculated according to ref. 63 and 64.

Fig. 7