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note
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The ortho and meta carbon signals of the solid-state spectrum at +63 °C (125.0 and 128.5 ppm, respectively) were assigned by analogy with the shifts (125.0 and 129.3 ppm, respectively) of the solution spectrum (see Experimental Section). Such an assignment was further supported by the observation that these two signals grow much more than those of all other carbons when a standard single pulse experiment (without cross polarization) is applied with a 16 s delay time. This is due to the faster relaxation rate that is a consequence of the rapid rotation of the phenyl ring at high temperature (all other carbon signals would require a delay at least 10 times longer to display a significant growth in this single pulse experiment).
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43
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2442510727
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note
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13C signals, computed for the isolated molecule, is the same as that occurring in the crystal. It has to be stressed, however, that such an assignment is immaterial for the experimental determination of the rotation barrier, since the opposite assignment would obviously yield the same ΔG‡ value.
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49
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2442613699
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Within the experimental uncertainty the ΔG‡ value was found to be independent of temperature, indicating that the ΔS‡ term must be quite small.
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