1948
DOI: 10.1063/1.1746878
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Nuclear Resonance Absorption in Hydrated Crystals: Fine Structure of the Proton Line

Abstract: Fine structure has been observed in the nuclear paramagnetic resonance absorption line for protons in crystalline hydrates. The magnetic field of 6820 gauss was provided by a permanent magnet, the inherent stability of which facilitated detailed study of line shape. Measurements on a single crystal of CaSO4·2H2O show a splitting into four component lines with maximum separation varying from zero to 22 gauss, depending upon the direction of the externally applied magnetic field in the crystal. Both the number o… Show more

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Cited by 1,242 publications
(539 citation statements)
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“…The rest of the spectrum is the Pake doublet expected from the splitting of two 13 C dipoles. 7 This pattern can be fit to obtain directly the distance between the two dipoles, the desired carbon-carbon bond length. 5 ' 6 In this case the value obtained is 1.38+±0.02A.…”
Section: Resultsmentioning
confidence: 99%
“…The rest of the spectrum is the Pake doublet expected from the splitting of two 13 C dipoles. 7 This pattern can be fit to obtain directly the distance between the two dipoles, the desired carbon-carbon bond length. 5 ' 6 In this case the value obtained is 1.38+±0.02A.…”
Section: Resultsmentioning
confidence: 99%
“…We found from NMR measurements under a magnetic field of 4 Tesla that the splitting is magnetic field independent (not shown), which is one of the characteristics of the well-known Pake doublets. 34 From the splitting we can estimate the carbon-carbon (C-C) bond length as follows. Here, we neglect the curvature of a graphene sheet and assume that the local structure around a 13 C atom with three 13 C nearest neighbors is a hexagonalhoneycomb plane for simplicity.…”
Section: Methodsmentioning
confidence: 99%
“…(2) or (3) over all angles h. With a fixed separation between spins, this yields the so-called Pake pattern [14] that is characterized by sharp discontinuities at AEDH dd ð90 Þ and outer shoulders at AEDH dd ð0 Þ. The profile of the Pake pattern is given by the identity: I(DH dd ) Á dDH dd = sin h Á dh, which corresponds to the angular distribution for axial symmetry.…”
Section: Dipolar Powder Spectra and Distance Distributionsmentioning
confidence: 99%