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arXiv:solv-int/9710002 · Nuclear Physics B

Correlation functions for a strongly correlated boson system

N. M. Bogoliubov, Anatoli G. Izergin, N Kitanine

Published Apr 1, 1998• 99 citations
arXivHTMLPDF
DOI
10.1016/s0550-3213(98)00038-8

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The natural integrable correlated strongly coupled boson system in 1 + 1 dimensions is the qqq-boson hopping model; we calculate its critical exponent $\ensuremath{\theta}$ and determine its correlation functions. For small couplings the qqq-boson model has natural connections with the Bose gas and the XY\mathrm{XY}XY models of very large spin for which $\ensuremath{\theta}'\mathrm{s}$ and correlators are reported. For large couplings the hopping model is a new phase of interacting bosons substantially different from the impenetrable Bose gas.
We introduce a density functional formalism to study the ground-state properties of strongly correlated dipolar and ionic ultracold bosonic and fermionic gases, based on the self-consistent combination of the weak and the strong coupling limits. Contrary to conventional density functional approaches, our formalism does not require a previous calculation of the interacting homogeneous gas, and it is thus very suitable to treat systems with tunable long-range interactions. Because of its asymptotic exactness in the regime of strong correlation, the formalism works for systems in which standard mean-field theories fail.