0306055v2

related topics
{spin, pulse, spins}
{equation, function, exp}
{time, wave, function}
{cos, sin, state}
{temperature, thermal, energy}
{classical, space, random}
{energy, gaussian, time}
{state, algorithm, problem}
{cavity, atom, atoms}
{let, theorem, proof}
{vol, operators, histories}
{time, decoherence, evolution}
{time, systems, information}
{energy, state, states}
{operator, operators, space}

Non-Ergodic Nuclear Depolarization in Nano-Cavities

E. B. Fel'dman, M. G. Rudavets

abstract: Recently, it has been observed that the effective dipolar interactions between nuclear spins of spin-carrying molecules of a gas in a closed nano-cavities are independent of the spacing between all spins. We derive exact time-dependent polarization for all spins in spin-1/2 ensemble with spatially independent effective dipolar interactions. If the initial polarization is on a single (first) spin,$P_1(0)= 1$ then the exact spin dynamics of the model is shown to exhibit a periodical short pulses of the polarization of the first spin, the effect being typical of the systems having a large number, $N$, of spins. If $N \gg 1$, then within the period $4\pi/g$ ($2\pi/g$) for odd (even) $N$-spin clusters, with $g$ standing for spin coupling, the polarization of spin 1 switches quickly from unity to the time independent value, 1/3, over the time interval about $(g\sqrt{N})^{-1}$, thus, almost all the time, the spin 1 spends in the time independent condition $P_1(t)= 1/3$. The period and the width of the pulses determine the volume and the form-factor of the ellipsoidal cavity. The formalism is adopted to the case of time varying nano-fluctuations of the volume of the cavitation nano-bubbles. If the volume $V(t)$ is varied by the Gaussian-in-time random noise then the envelope of the polarization peaks goes irreversibly to 1/3. The polarization dynamics of the single spin exhibits the Gaussian (or exponential) time dependence when the correlation time of the fluctuations of the nano-volume is larger (or smaller) than the $<(\delta g)^2 >^{-1/2} $, where the $<(\delta g)^2>$ is the variance of the $g(V(t))$ coupling. Finally, we report the exact calculations of the NMR line shape for the $N$-spin gaseous aggregate.

oai_identifier:
oai:arXiv.org:quant-ph/0306055
categories:
quant-ph
comments:
26 pages, 3 figures
doi:
10.1134/1.1675888
arxiv_id:
quant-ph/0306055
journal_ref:
JETP V98 N2 (2004) pp 207-219
report_no:
quant-ph/0306055
created:
2003-06-06
updated:
2003-06-07

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