2015/04/14 by Igor Travěnec, Igor Travenec, Ladislav Šamaj +1 · 7 citations
Chemistry · Materials Science · Physics and Astronomy · #Cold Atom Physics and Bose-Einstein Condensates #Condensed matter physics #Coulomb #Dimensionless quantity #Electron #Electrostatics and Colloid Interactions #Hard spheres #Lattice (music) #Limiting #Material Dynamics and Properties #Phase (matter) #Phase diagram #Phase transition #Physics #Quantum mechanics #SPHERES #Yukawa potential #cond-mat.soft
paper · pdf · doi:10.1103/physreve.92.022306
published in Physical Review E 92(2), 022306 (American Physical Society)
arxiv created 2015/04/14 · openalex publication_date 2015/08/17 · arxiv updated 2015/08/26 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We study the ground-state Wigner bilayers of pointlike particles with Yukawa pairwise interactions, confined to the surface of two parallel hard walls at dimensionless distance η. The model involves as limiting cases the unscreened Coulomb potential and hard spheres. The phase diagram of Yukawa particles, studied numerically by Messina and Löwen [Phys. Rev. Lett. 91, 146101 (2003)], exhibits five different staggered phases as η varies from 0 to intermediate values. We present a lattice summation method using the generalized Misra functions which permits us to calculate the energy per particle of the phases with a precision much higher than usual in computer simulations. This allows us to address some tiny details of the phase diagram. Going from the hexagonal phase I to phase II is shown to occur at η=0. All second-order phase transitions are proved to be of mean-field type. We also derive the asymptotic shape of critical lines close to the Coulomb and hard-spheres limits. In and close to the hard-spheres limit, the dependence of the internal parameters of the present phases on η is determined exactly.