The boundary density profile of a Coulomb droplet. Freezing at the edge
arXiv:2009.02359 · doi:10.1088/1751-8121/abcab9
Abstract
We revisit the problem of computing the boundary density profile of a droplet of two-dimensional one-component plasma (2D OCP) with logarithmic interaction between particles in a confining harmonic potential. At a sufficiently low temperature but still in the liquid phase, the density exhibits oscillations as a function of the distance to the boundary of the droplet. We obtain the density profile numerically using Monte-Carlo simulations of the 2D OCP. We argue that the decay and period of those oscillations can be explained within a picture of the Wigner crystallization near the boundary, where the crystal is gradually melted with the increasing distance to the boundary.
arXiv comment26 pages, 13 figures; figure 12 updated
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Cited by in corpus (8)
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- Spacing distribution in the 2D Coulomb gas: Surmise and symmetry classes of non-Hermitian random matrices at non-integer
- W-infinity Symmetry in the Quantum Hall Effect Beyond the Edge
- Scaling Limits of Planar Symplectic Ensembles
- Universal Modelling of Oscillations in Fractional Quantum Hall Fluids
- Adiabatic Deformations of Quantum Hall Droplets
- Complex symmetric, self-dual, and Ginibre random matrices: Analytical results for three classes of bulk and edge statistics
- Quantum Hall edges beyond the plasma analogy