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Physical Review A

Stability and correlations in dilute two-dimensional boson systems (5 pages)

Ole Gade Sørensen, A. S. Jensen, Han Guangze, D. V. Fedorov

Published Jan 1, 2004• 0 citations
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Stability and correlations in dilute two-dimensional boson systems

Han Guangze, O. Sørensen, A. S. Jensen +1 more

The hyperspherical adiabatic expansion method is used to describe correlations in a symmetric boson system rigorously confined to two spatial dimensions. The hyperangular eigenvalue equation turns out to be almost independent of the hyperradius, whereas the solutions are strongly varying with the strength of the attractive two-body potentials. Instability is encountered in hyperangular, hyperradial, and mean-field equations for almost identical strengths inversely proportional to the particle number. The derived conditions for stability are similar to mean-field conditions and closely related to the possible occurrence of the Thomas and Efimov effects. Renormalization in mean-field calculations for two spatial dimensions is probably not needed.

arXiv:cond-mat/0401285•Physical Review A•Jul 21, 2004•2 citations

Two-Boson Correlations in Various One-Dimensional Traps

Anna Okopińska, Przemysław Kościk

arXiv:1009.1482•Few-Body Systems•Feb 18, 2009•4 citations

Stable Dilute Supersolid of Two-Dimensional Dipolar Bosons

Zhen-Kai Lu, Yun Li, Dmitry S. Petrov +1 more

We consider two-dimensional bosonic dipoles oriented perpendicularly to the plane. On top of the usual two-body contact and long-range dipolar interactions we add a contact three-body repulsion as expected, in particular, for dipoles in the bilayer geometry with tunneling. The three-body repulsion is crucial for stabilizing the system, and we show that our model allows for stable continuous space supersolid states in the dilute regime and calculate the zero-temperature phase diagram.

arXiv:1409.7737•Physical Review Letters•Aug 14, 2015•121 citations
The hyperspherical adiabatic expansion method is used to describe correlations in a symmetric boson system rigorously confined to two spatial dimensions. The hyperangular eigenvalue equation turns out to be almost independent of the hyperradius, whereas the solutions are strongly varying with the strength of the attractive two-body potentials. Instability is encountered in hyperangular, hyperradial, and mean-field equations for almost identical strengths inversely proportional to the particle number. The derived conditions for stability are similar to mean-field conditions and closely related to the possible occurrence of the Thomas and Efimov effects. Renormalization in mean-field calculations for two spatial dimensions is probably not needed.