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As 1 au of ω is 6.579 683 921 × 1015 Hz from ref 54, and the resonance frequency of a nucleus with magnetogyric ratio γI is νI, γ IB/2π, the magnetic field density B for proton resonance is ≈15.45 T for ω, 1 × 10-7 au. However, if one takes this value for a proton, then, allowing for the corresponding magnetogyric ratios,56 ω is only 0.2514 times this frequency for 13C, 0.1014 times for 15N, and 0.1356 times for 17O for B, 15.45 T, It is unrealistic to use ω, 1 × 10-7 au for these heavier nuclei; therefore, the magnetoelectric shieldings of 13C, 15N, and 17O in the tables should be scaled by the same factors
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In the case of 17O with I, 5/2 there are also nuclear electric quadrupole contributions that are not present on the I, 1/2 nuclei. Therefore, the 17O nucleus, although displaying the largest isotropic magnetoelectric shielding in the compounds studied here, is most likely all but an ideal probe, due to low receptivity and unfavorable nuclear spin, which may cause undesirable lifetime broadening of signals
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