2001
DOI: 10.1103/physrevb.63.180508
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Mott-superfluid transition in bosonic ladders

Abstract: We show that in a commensurate bosonic ladder, a quantum phase transition occurs between a Mott insulator and a superfluid when interchain hopping increases. We analyse the properties of this transition as well as the physical properties of the two phases. We discuss the physical consequences for experimental systems such as Josephson Junction arrays.

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Cited by 40 publications
(50 citation statements)
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“…For example, parallel approaches can be used to study models of coupled 1D hard-core lattice bosons, where similar effective theories can be constructed. 33,34,35,36,37,38 When local density fluctuations become stronger, more local states with different particle numbers should be kept. Following the above reasoning, an effective theory with more bosonic phase fields should be reached.…”
Section: Discussionmentioning
confidence: 99%
“…For example, parallel approaches can be used to study models of coupled 1D hard-core lattice bosons, where similar effective theories can be constructed. 33,34,35,36,37,38 When local density fluctuations become stronger, more local states with different particle numbers should be kept. Following the above reasoning, an effective theory with more bosonic phase fields should be reached.…”
Section: Discussionmentioning
confidence: 99%
“…Quasi-1D systems such as ladders have been of special interest to understand the phenomenon of high-temperature superconductivity, spin-gapped metallic state [22][23][24] etc. The extra coupling between the legs of the ladder makes these systems unique, as a result of which, the quantum phase transitions are influenced substantially even in a simple model like the Bose-Hubbard ladder [25][26][27]. Also, the effect of kinetic frustration along with various interactions can lead to interesting new phases in ladder systems [28][29][30][31][32][33][34][35][36], which are not possible in one dimensional lattice systems.…”
Section: Introductionmentioning
confidence: 99%
“…In this case, a cos 2φ s cos 2φ a term is present and favors an insulating state 11 . The interchain Josephson coupling cos √ 2θ a competes with this term making the system conducting when large enough 24 . The application of H > H c1 suppresses the interchain Josephson coupling turning the ladder insulating in the vortex phase.…”
mentioning
confidence: 99%