Abstract
The modern theory of spin resonance and relaxation1,2 leads to a non-Markovian equation of motion for the spin density matrix. However, explicit expressions for the relaxation functions are always given in the short correlation time limit: it is assumed that the relevant time correlation functions decay on a much shorter time scale than the experimental one. It is well known that this Markovian approximation does not hold in many situations of interest, e. g. in supercooled liquids and solids at low temperatures.
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References
A. Abragam and M. Goldstein: Nuclear magnetism: Order and disorder, Clarendon Press, Oxford (1982).
M. Mehring; High Resolution NMR in Solids, Springer Verlag, Bonn-Heidelberg-New York (1983).
G. Diezemann, W. Schirmacher; submitted to J. Phys. Condens. Matter
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© 1990 Springer-Verlag Berlin Heidelberg
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Diezemann, G., Schirmacher, W. (1990). High Field Nuclear Spin Relaxation in Liquids and Solids. In: Mehring, M., von Schütz, J.U., Wolf, H.C. (eds) 25th Congress Ampere on Magnetic Resonance and Related Phenomena. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-76072-3_116
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DOI: https://doi.org/10.1007/978-3-642-76072-3_116
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