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Beilstein J. Nanotechnol. 2017, 8, 943–955, doi:10.3762/bjnano.8.96
Figure 1: Chemical structures of the anionic complex fragments [Cu(opba)]2− (P1, left) and [Cu(opbon-Pr2)]2− (...
Figure 2: Echo detected ESR spectra of P1 at a frequency ν = 9.85 GHz (X-band) and at T = 20 K for the magnet...
Figure 3: Time dependence of the intensity of the echo signal for complex P1 at T = 30 K on a linear (main pa...
Figure 4: Temperature dependence of the phase relaxation time Tm of P1 and P2 at a frequency ν = 9.85 GHz mea...
Figure 5: Echo detected ESR spectra of P1 (top) and P2 (bottom) at a frequency ν = 33.899 GHz (P1) and 33.915...
Figure 6: Temperature dependence of the phase relaxation time Tm of P1 and P2 at a frequency ν = 33.9 GHz for...
Figure 7: Temperature dependence of the longitudinal relaxation time T1 of P1 and P2 at a frequency ν = 33.9 ...
Figure 8: CPMG echoes for complex P1 for two levels of the microwave power attenuation of 3 dB and 13 dB. Not...
Figure 9: CPMG experiment on complex P1 at ν = 33.9 GHz, T = 20 K, and H||z-axis: Separation of the refocused...
Figure 10: The calculated decay of the primary echo signal as a function of the time delay τ between the two p...
Figure 11: The calculated decay of the echo signal in the CPMG experiment as a function of the number n of the...
Figure 12: Comparison of the experimental and model dependences of the decay of the primary (a,c) and CPMG ech...