One dimensional H-1, H-2 and H-3

The ground-state properties of one-dimensional electron-spin-polarized hydrogen H-1, deuterium H-2, and tritium 3 Hare obtained by means of quantum Monte Carlo methods. The equations of state of the three isotopes are calculated for a wide range of linear densities. The pair correlation function and...

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Detalles Bibliográficos
Autores: Vidal, A.J., Astrakharchik, Grigori|||0000-0003-0394-8094, Vranješ Markic, Leandra, Boronat, J.
Tipo de recurso: artículo
Fecha de publicación:2016
País:España
Institución:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/88635
Acceso en línea:https://hdl.handle.net/2117/88635
https://dx.doi.org/10.1088/1367-2630/18/5/055013
Access Level:acceso abierto
Palabra clave:Monte Carlo method
Equations of state
Luttinger liquids
Hydrogen
Bose-Einstein condensation
quantum Monte Carlo methods
equation of state
Luttinger liquid
hydrogen
Tonks-Girardeau gas
ground-state
Anderson localization
Impenetrable bosons
gas
system
transport
energy
Montecarlo, Mètode de
Equacions d'estat
Hidrogen
Condensació de Bose-Einstein
Àrees temàtiques de la UPC::Física
Descripción
Sumario:The ground-state properties of one-dimensional electron-spin-polarized hydrogen H-1, deuterium H-2, and tritium 3 Hare obtained by means of quantum Monte Carlo methods. The equations of state of the three isotopes are calculated for a wide range of linear densities. The pair correlation function and the static structure factor are obtained and interpreted within the framework of the Luttinger liquid theory. We report the density dependence of the Luttinger parameter and use it to identify different physical regimes: Bogoliubov Bose gas, super-Tonks-Girardeau gas, and quasi-crystal regimes for bosons; repulsive, attractive Fermi gas, and quasi-crystal regimes for fermions. We find that the tritium isotope is the one with the richest behavior. Our results show unambiguously the relevant role of the isotope mass in the properties of this quantum system.