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. Author manuscript; available in PMC: 2016 Apr 1.
Published in final edited form as: J Magn Reson. 2014 Dec 29;253:129–137. doi: 10.1016/j.jmr.2014.11.015

Figure 3.

Figure 3

Dipolar-decoupled natural abundance 13C NMR spectra of some solids obtained using single Hartmann-Hahn cross-polarization contacts of 1 ms duration. The cross-polarization spectra, obtained both with and without magic-angle spinning, are compared to some standard Fourier transform 13C NMR spectra of various materials in solution. Each spectrum is 8 kHz wide (at 22.6 MHz). The magnetic field increases from left to right. From reference [24].