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. Author manuscript; available in PMC: 2019 Oct 9.
Published in final edited form as: Langmuir. 2016 Apr 11;34(29):8678–8684. doi: 10.1021/acs.langmuir.5b04114

Figure 2:

Figure 2:

(a) 13C CPMAS pulse sequence. (b) XY8 phase cycling 13C{29Si} REDOR pulse sequence with alternating π pulses on both channels. (c) 29Si spin topology used in simulation of 13C{29Si} REDOR data showing nearly 180° angles between 13C=O – 29Si and 13C=O – 13Cα dipolar vectors. Arrow in the figure indicates the dipolar couplings that were varied in simulations. (d) 15N CPMAS pulse sequence. (e) XY8 phase cycling 15N{29Si} REDOR pulse sequence with alternating π pulses on both channels.