Berezinskii-Kosterlitz-Thouless transition in two-dimensional dipolar stripes

A two-dimensional quantum system of dipoles, with a polarization angle not perpendicular to the plane, shows a transition from a gas to a stripe phase. We have studied the thermal properties of these two phases using the path-integral Monte Carlo (PIMC) method. By simulating the thermal density matr...

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Bibliographic Details
Authors: Bombín Escudero, Raul|||0000-0002-4553-1214, Mazzanti Castrillejo, Fernando Pablo|||0000-0001-6641-0609, Boronat Medico, Jordi|||0000-0002-0273-3457
Format: article
Publication Date:2019
Country:España
Institution:Universitat Politècnica de Catalunya (UPC)
Repository:UPCommons. Portal del coneixement obert de la UPC
Language:English
OAI Identifier:oai:upcommons.upc.edu:2117/176233
Online Access:https://hdl.handle.net/2117/176233
https://dx.doi.org/10.1103/PhysRevA.100.063614
Access Level:Open access
Keyword:Superfluidity
BKT transition
Superfluïdesa
Àrees temàtiques de la UPC::Física
Description
Summary:A two-dimensional quantum system of dipoles, with a polarization angle not perpendicular to the plane, shows a transition from a gas to a stripe phase. We have studied the thermal properties of these two phases using the path-integral Monte Carlo (PIMC) method. By simulating the thermal density matrix, PIMC provides exact results for magnitudes of interest such as the superfluid fraction and the one-body density matrix. As it is well known, in two dimensions the superfluid-to-normal phase transition follows the Berezinskii-Kosterlitz-Thouless (BKT) scenario. Our results show that both the anisotropic gas and the stripe phases follow the BKT scaling laws. At fixed density and increasing the tilting angle, the transition temperature decreases in going from the gas to the stripe phase. Superfluidity in the perpendicular direction to the stripes is rather small close to the critical temperature but it becomes larger at lower temperatures, mainly close to the transition to the gas. Our results are in qualitative agreement with the supersolidity observed recently in a quasi-one-dimensional array of dipolar droplets.