Accessing elusive two-dimensional phases of dipolar Bose-Einstein condensates by finite temperature

It has been shown that dipolar Bose-Einstein condensates that are tightly trapped along the polarization direction can feature a rich phase diagram. In this paper we show that finite temperature can assist in accessing parts of the phase diagram that otherwise appear hard to realize due to excessive...

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Detalhes bibliográficos
Autores: He, Liang-Jun, Sánchez Baena, Juan|||0000-0001-6825-2843, Maucher, Fabian, Zhang, Yong-Chang
Formato: artículo
Fecha de publicación:2025
País:España
Recursos:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/429254
Acesso em linha:https://hdl.handle.net/2117/429254
https://dx.doi.org/10.1103/PhysRevResearch.7.023019
Access Level:acceso abierto
Palavra-chave:Bose gases
Bose-Einstein condensates
Dipolar gases
Quantum phase transitions
Ultracold gases
Àrees temàtiques de la UPC::Física::Física molecular
Àrees temàtiques de la UPC::Física::Física de l'estat sòlid::Superconductors
Descrição
Resumo:It has been shown that dipolar Bose-Einstein condensates that are tightly trapped along the polarization direction can feature a rich phase diagram. In this paper we show that finite temperature can assist in accessing parts of the phase diagram that otherwise appear hard to realize due to excessively large densities and number of atoms being required. These include honeycomb and stripe phases both unconfined and with a finite extent. To map out a phase-diagram, we employ both variational analysis and full numerical calculations solving the finite-temperature extended Gross-Pitaevskii equation (TeGPE). Furthermore, we exhibit real-time evolution simulations leading to such states. We account for the effect of thermal fluctuations by means of Bogoliubov theory, employing the local density approximation. We find that finite temperatures can lead to a significant decrease in the necessary particle number and density that might ultimately pave a route for future experimental realizations.