Hm. Pastawski et al., Occurrence of dynamic irreversibility in multi-body quantum systems: A test employing nuclear magnetic resonance, REV MEX FIS, 44, 1998, pp. 1-6
The NMR technique allows to create a non-equilibrium local polarization and
to detect its later evolution. Besides, it is possible to change the sign
of the effective dipolar Hamiltonian and therefore retrace an apparently di
ffusive dynamics leading to a polarization echo. Our experiments in polycry
stalline samples of (C5H5)Mn(CO)(3) and (C5H5)(2)Fe showed that those echoe
s attenuate as function of the time elapsed until the dynamics is reverted.
In the former, a strong irreversible quadrupolar interaction (non inverted
), produces an exponential decay. The latter has strong many-body interacti
ons (reversible) whose quasi-chaotic dynamics has a local instability sensi
tive to the presence of small residual interactions (non-inverted). Thus an
irreversible Gaussian decay appears. Numerical solutions of model systems
agree with this hypothesis. To control the dynamical parameters we applied
to structurally similar crystals: (C5H5)(2)Fe and (C5H5)(2)Co, a pulse sequ
ence devised ad-hoc. It limits the complexity of the dynamical state for ea
ch t(R), slowing down its contribution to the attenuation and revealing the
presence of an eventual underlying source of irreversibility. For (C5H5)(2
)Co an exponential decay [attributable to the magnetism of the Co(II)] emer
ges when the dynamics is sufficiently reduced, while for (C5H5)(2)Fe the at
tenuation remains Gaussian. This shows that irreversibility is controlled b
y the reversible dynamics.