Collective modes of a strongly interacting Bose gas: probing the Mott transition
arXiv:1106.0575 · doi:10.1103/PhysRevA.85.013635
Abstract
We analyze the collective modes of a harmonically trapped, strongly interacting Bose gas in an optical lattice in the vicinity of the Mott insulator transition. For that aim we employ the dynamical Gutzwiller equations, by performing real-time evolution and by solving the equations in linear response. We find a strong dependence on the spatial dimension of the system: while in one dimension the frequency of the dipole mode vanishes at the Mott transition, in higher dimensions the dominant dipole mode is featureless and we find a signature only in the breathing mode. We discuss implications for experiments with bosonic and fermionic atoms.
10 pages, 7 figures; updated figures, published version
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Cited by in corpus (5)
- Excitation spectra of many-body systems by linear response: General theory and applications to trapped condensates
- Breathing mode in the Bose-Hubbard chain with a harmonic trapping potential
- Excitation spectra of fragmented condensates by linear response: General theory and application to a condensate in a double-well potential
- Frustrated Quantum Magnetism with Bose Gases in Triangular Optical Lattices at Negative Absolute Temperatures
- Application of the inhomogeneous Kibble-Zurek mechanism to quench dynamics in the transition from a Mott-insulator to a superfluid in a finite system