The quantum tunneling effect usually first evokes the textbook case of a classically forbidden
crossing of a potential barrier. However this phenomenon can be far richer in quantum systems
whose classical counterpart exhibits dynamics that can be both chaotic or regular depending
on the initial conditions. Indeed, in the phase space of such systems, regular orbits form stable
islands, that can be seen as potential well, surrounded by a chaotic sea of unstable orbits (see
Fig). The tunneling oscillations between two neigbouring regular islands is then generically
mediated by a state delocalized in the chaotic sea. This leads to sharp resonances in the
tunneling oscillation frequencies, a phenomenon known as chaos-assisted tunneling [1].
From an experimental point of view, this rich physics can be simulated using driven optical
lattices. We recently demonstrated [2] in collaboration with a team of experimentalist, the first
explicit observation of such tunneling resonances in a quantum system. In this work we show
that the very same mechanism actually generates long-range hopping across distant sites of the
driven lattice, and we propose procedure for their experimental observation. These results open
the way to a new regime of tunability for quantum simulations, making possible to simulate
classes of systems that are difficult to address by other means.
[1] S. Tomsovic and d. Ullmo, Phys. Rev. E 50, 145 (1994)
[2] In preparation
- Poster
A modulated lattice (a) generates a classical phase space (b) that consists in islands of stable orbits (blue) and a sea of chaotic orbits (red). A particle in a stable site (red circle) is coupled to the n-th distant site (grey circle) with a coupling constant Jn. (c) Coupling constant |Jn| as a function of the distance between sites. In the regular case of a lattice at rest the couplings decay exponentially with distance, while in the chaos-assisted regime, long-range couplings are visible.
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