Equation of state of two-dimensional He-3 at zero temperature (Articolo in rivista)

Type
Label
  • Equation of state of two-dimensional He-3 at zero temperature (Articolo in rivista) (literal)
Anno
  • 2012-01-01T00:00:00+01:00 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#doi
  • 10.1103/PhysRevB.85.184401 (literal)
Alternative label
  • Nava, M.; Motta, A.; Galli, D. E.; Vitali, E.; Moroni, S. (2012)
    Equation of state of two-dimensional He-3 at zero temperature
    in Physical review. B, Condensed matter and materials physics
    (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#autori
  • Nava, M.; Motta, A.; Galli, D. E.; Vitali, E.; Moroni, S. (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroVolume
  • 85 (literal)
Rivista
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  • 7 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroFascicolo
  • 18 (literal)
Note
  • ISI Web of Science (WOS) (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#affiliazioni
  • University of Milan; IOM CNR DEMOCRITOS Natl Simulat Ctr; International School for Advanced Studies (literal)
Titolo
  • Equation of state of two-dimensional He-3 at zero temperature (literal)
Abstract
  • We have performed a quantum Monte Carlo study of a two-dimensional bulk sample of interacting 1/2-spin structureless fermions, a model of He-3 adsorbed on a variety of preplated graphite substrates. We have computed the equation of state and the polarization energy using both the standard fixed-node approximate technique with a simple backflow trial function and a formally exact methodology, relying on bosonic imaginary-time correlation functions of operators suitably chosen in order to extract fermionic energies. As the density increases, the fixed-node approximation predicts a transition to an itinerant ferromagnetic fluid, whereas the unbiased methodology indicates that the paramagnetic fluid is the stable phase until crystallization takes place. We find that two-dimensional He-3 at zero temperature crystallizes from the paramagnetic fluid at a density of 0.061 angstrom(-2) with a narrow coexistence region of 0.002 angstrom(-2). Remarkably, the spin susceptibility turns out in very good agreement with experiments. (literal)
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