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PM Cereghetti

Publications and source records attributed to PM Cereghetti.

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Phonon-assisted spin diffusion in solids

The spin flip-flop transition rate is calculated for the case of spectral spin diffusion within a system of dipolarly coupled spins in a solid where the lattice vibrations are present. Long-wavelength acoustic phonons time-modulate the interspin distance r(ij) and enhance the transition rate via the change of the 1/r(3)(ij) term in the coupling dipolar Hamiltonian. The phonon-assisted spin diffusion rate is calculated by the golden rule in the Debye approximation of the phonon density of states. The coupling of the spins to the phonons introduces temperature dependence into the transition rate, in contrast to the spin diffusion in a rigid lattice, where the rate is temperature-independent. The direct (one-phonon absorption or emission) processes introduce a linear temperature dependence into the rate at temperatures not too close to T = 0. Two-phonon processes introduce a more complicated temperature dependence that again becomes simple analytical for temperatures higher than the Debye temperature, where the rate is proportional to T(2), and in the limit T --> 0, where the rate varies as T(7). Raman processes (one-phonon absorption and another phonon emission) dominate by far the phonon-assisted spin flip-flop transitions. Copyright 2000 Academic Press.

Journal Article↗

87Rb spin diffusion in ferroelectric RbH2PO4 studied by two dimensional exchange NMR

We separate the contributions of spectral spin diffusion and chemical exchange in the 2D exchange NMR spectra of 87Rb in the pseudo-spin glass Rb1-x(ND4)xD2PO4 by studying the 87Rb spin diffusion in the isostructural compound RbH2PO4 at 85K, where the system is frozen in the ferroelectric phase state. The fact that the spin-diffusion time (TSD) of a particular point in the 2D spectrum depends essentially on its distance from the diagonal, allowed, even for the case of an unresolved 2D spectrum, to determine TSD as a function of the frequency separation Delta over two orders of magnitude. In accordance with existing theories, T-1SD(Delta) was found to be of Gaussian shape. However, we found huge discrepancies between the calculated and the experimentally determined second moments. This failure of the theory is not understood at present. Copyright 1999 Academic Press.

Journal Article↗