Abstract
Nuclear magnetic resonance (NMR) signals can only be observed from a sample which contains nuclei with a nonvanishing magnetic moment (cf. Table 1.1, first column). The resonance frequency is proportional to the magnetic field H 0 applied to the sample and different for nuclei of different kind (cf. Table 1.1, second column). The intensity of the NMR signal for equal numbers of nuclei at constant field H 0 also depends on the kind of nucleus and is maximum for protons (cf. Table 1.1, third column).
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Pfeifer, H. (1972). Nuclear Magnetic Resonance and Relaxation of Molecules Adsorbed on Solids. In: Diehl, P., Fluck, E., Kosfeld, R. (eds) NMR Basic Principles and Progress / NMR Grundlagen und Fortschritte. NMR Basic Principles and Progress / NMR Grundlagen und Fortschritte, vol 7. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-65312-4_2
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