Zero-temperature phase diagram of the second layer of 4He adsorbed on graphene

The phase diagram at zero temperature of 4He adsorbed on a helium incommensurate triangular solid on top of a single graphene sheet has been obtained using the diffusion Monte Carlo method. We have found that, in accordance with previous experimental and simulation results for graphite, the ground s...

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Detalhes bibliográficos
Autores: Gordillo Bargueño, Maria Carmen|||0000-0003-1521-483X, Boronat Medico, Jordi|||0000-0002-0273-3457
Formato: artículo
Fecha de publicación:2012
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:2117/16697
Acesso em linha:https://hdl.handle.net/2117/16697
https://dx.doi.org/10.1103/PhysRevB.85.195457
Access Level:acceso abierto
Palavra-chave:Graphene
Monte Carlo method
Grafè
Montecarlo, Mètode de
Àrees temàtiques de la UPC::Física
Descrição
Resumo:The phase diagram at zero temperature of 4He adsorbed on a helium incommensurate triangular solid on top of a single graphene sheet has been obtained using the diffusion Monte Carlo method. We have found that, in accordance with previous experimental and simulation results for graphite, the ground state of 4He on this setup is a liquid that, upon compression, transforms into a triangular solid. To define the stability limits of both liquid and solid phases, we considered not only the adsorption energies of the atoms located on the second layer but the average energy of the atoms in both layers. Our results show that the lower density limit for a stable liquid in the second layer is 0.163±0.005 Å−2 and that the lower limit for the existence of an incommensurate solid on the second layer is 0.186±0.003 Å−2. Both values are in overall agreement with the results of torsional oscillator experiments and heat capacity measurements on graphite. The 4/7 and 7/12 registered solids are found to be metastable with respect to triangular incommensurate arrangements of the same density.