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Probing intermolecular interactions and three dimensional packing of organic molecules by solid state NMR

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Figure

Figure 2.1. Product operator representation of an isolated spin I = 1/2 nu-cleus in a magnetic field using the energy levels of the |α⟩ andβ | ⟩ states.The difference in energy, in units of ¯h, is given by the Larmor frequency,ω0 = −γB0
Figure 2.3.Product operator representation ofconventions described in Fig.quantum x-anti-phase and multiple- operators for a coupled pair of I = 1/2 nuclei, I and S, using the 2.1.
Figure 2.4. Chemical Shift Anisotropy powder lineshapes for an isolatedsidebands under MAS are separated bynormalised
Figure 3.1.Pulse sequence and corresponding coherence transfer pathwaydiagram (see §3.1.4) for a ‘π/2 − acquire’ experiment on spin, I
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