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Due to the axial symmetry of the relevant electrical field gradient tensor the azimuthal angle needed not to be taken into account explicitly.
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36
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0004161838
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We have used the random number generator ran4, see Cambridge University Press, Cambridge
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We have used the random number generator ran4, see W. H. Press, B. P. Flannery, S. A. Teukolsky, and W. T. Vetterling, Numerical Recipes (Cambridge University Press, Cambridge, 1986).
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note
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i+1) is found on the surface of a cone located around the initial orientation. With a jump angle the cone exhibits an opening angle of 2. The variable 0≤ζ<2π specifies where, on the circle obtained from the intersection of this cone with the unit sphere, the C-D orientation vector is pointing to after the elementary jump.
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38
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22244449174
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note
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SIN signals the latter were multiplied by 4 3 (see Refs. 23 and 25).
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39
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22244477624
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For details see, e.g., Refs. 23 and 25
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For details see, e.g., Refs. 23 and 25.
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40
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unpublished
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T. Jörg et al. (unpublished).
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This is what should be expected in the slow motion regime; see
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22244433728
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p)〉 pattern. Therefore the determination of the jump angle distribution should not be affected by spin diffusion.
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Also
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Also F. Fujara, W. Petry, R. M. Diehl, W. Schnauss, and H. Sillescu, Europhys. Lett. 14, 563 (1991) find that the deuteron spin-lattice times measured for the C-D and O-D deuterons are identical in the regime of the α relaxation. In particular, this means that no indications for intramolecular reorientations were obtained.
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