[seminar] 09.06.2017. Jerzy Cioslowski: Wigner Crystallization in Central Potentials
Damir Pajic
dpajic at phy.hr
Mon Jun 5 17:28:40 CEST 2017
Drage kolegice i kolege,
Drago mi je da mogu najaviti sljedeći Seminar Fizičkog odsjeka:
Dear colleagues,
I would like to invite you to the following Seminar of the Department of
Physics:
petak/Friday 09.06.2017. u 15:15 h
room F201 (floor II)
Wigner Crystallization in Central Potentials
Prof. dr. Jerzy Cioslowski
http://www.fiz.univ.szczecin.pl/index.php/en/people/29.html?showall=1
Institute of Physics, University of Szczecin, Poland
and
Max-Planck-Institut für Physik komplexer Systeme, Dresden, Germany
In 1934, Eugene Wigner predicted spatial localization of electrons in a
low-density homogeneous electron gas (HEG). This Wigner crystallization,
which is triggered when the kinetic energy of HEG is sufficiently small
relative to the sum of the electron-electron repulsion energy and the
energy of interaction of electrons with the uniform neutralizing
background, is sudden i.e. it is associated with crossing of two energy
levels. In 3D, HEG crystallizes at the Wigner-Seitz radius r_s = 106
(in atomic units), producing the body-centered cubic lattice, whereas
in 2D the Wigner crystallization takes place at r_s = 31, the resulting
lattice being hexagonal (triangular).
In general, weak confinement is a prerequisite for formation of the
Wigner crystals, which are simply classical systems perturbed by
zero-point vibrations about equilibrium positions of the constituting
particles. In ground states of fully Coulombic systems (i.e. atoms and
molecules), autoionization precludes Wigner crystallization. However,
systems with unbound confining potentials (e.g. harmonium atoms)
crystallize gradually upon decrease of the confinement strength.
In this talk, several aspects of Wigner crystallization in central
confining potentials are discussed. In particular, the following
subjects are covered:
1. Harmonium atoms and their weak- and strong-correlation limits.
2. Robust interpolation between the weak- and strong-correlation limits.
3. Correlation in Coulomb crystals: the Madelung energy and its
variational estimation.
4. Smooth, oscillatory, and fluctuating components of energies of
Coulomb crystals.
5. The ground-and excited-state wavefunctions at the strong-correlation
limit.
6. The corresponding 1-matrices, natural spinorbitals, and their
occupancies.
Cjeloviti oglas je u prilogu./Formatted announcement is attached.
Lijep pozdrav / Best regards
Damir Pajić
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