Abstract

The recent advances in creating nearly degenerate quantum dipolar gases in optical lattices are opening the doors for the exploration of equilibrium physics of quantum systems with anisotropic and long-range dipolar interactions. In this paper we study the zero- and finite-temperature phase diagrams of a system of hard-core dipolar bosons at half-filling, trapped in a two-dimensional square optical lattice. The dipoles are aligned parallel to one another and tilted out of the optical lattice plane by means of an external electric field. At zero-temperature, the system is a superfluid (SF) at all tilt angles θ provided that the strength of dipolar interaction is below a critical value . Upon increasing the interaction strength while keeping θ fixed, the SF phase is destabilized in favor of a checkerboard or a stripe solid (SS) depending on the tilt angle. We explore the nature of the phase transition between the two solid phases, identifying a region of metastable emulsion states intervening between the two solid lobes. Additionally, we study the stability of these quantum phases against thermal fluctuations and find that the SS is the most robust, making it the best candidate for experimental observation.

Highlights

  • Experimental progress in trapping and controlling ultra cold atoms and molecules has led to the observation of magnetic and electric dipolar interactions in a variety of systems [1,2,3,4,5,6,7,8,9,10,11,12,13]

  • We study a system of hardcore, dipolar bosons with induced dipole moment d, confined by a two-dimensional square optical lattice with lattice constant a and by an external harmonic trap

  • The SF phase is present at all tilt angles, provided that the interaction strength is below Vc (q) J, and upon increasing the interaction strength the system enters one of the two solid phases depending on the value of θ

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Summary

10 December 2015

In this paper we study the zero- and finite-temperature phase this work must maintain attribution to the diagrams of a system of hard-core dipolar bosons at half-filling, trapped in a two-dimensional square author(s) and the title of the work, journal citation optical lattice. At zero-temperature, the system is a superfluid (SF) at all tilt angles θ provided that the strength of dipolar interaction is below a critical value Vc (q). Upon increasing the interaction strength while keeping θ fixed, the SF phase is destabilized in favor of a checkerboard or a stripe solid (SS) depending on the tilt angle. We study the stability of these quantum phases against thermal fluctuations and find that the SS is the most robust, making it the best candidate for experimental observation

Introduction
Hamiltonian
Zero- and finite-temperature phase diagrams
Harmonic confinement
Experimental realization
Conclusions
Full Text
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