26 research outputs found
Equilibrium crystal shapes in the Potts model
The three-dimensional -state Potts model, forced into coexistence by
fixing the density of one state, is studied for , 3, 4, and 6. As a
function of temperature and number of states, we studied the resulting
equilibrium droplet shapes. A theoretical discussion is given of the interface
properties at large values of . We found a roughening transition for each of
the numbers of states we studied, at temperatures that decrease with increasing
, but increase when measured as a fraction of the melting temperature. We
also found equilibrium shapes closely approaching a sphere near the melting
point, even though the three-dimensional Potts model with three or more states
does not have a phase transition with a diverging length scale at the melting
point.Comment: 6 pages, 3 figures, submitted to PR
Improvement of reflection electron microscopy : LODREM
International audienc
The overheating of lead crystals
Overheating of crystals has scarcely been reported unlike undercooling which is frequently observed. Admittedly the absence of overheating is the consequence of the crystal surface being covered by a liquid film (surface premelting) well under the bulk melting temperature. In the present letter we show that overheating is possible, and is actually observed (ÎT ⌠3°C), when the crystals are bounded by non wettable facets ({111} facets) separated by relatively small curved regions covered by their melt.Contrairement Ă la surfusion qui est trĂšs frĂ©quemment observĂ©e, la surchauffe de cristaux mĂ©talliques n'a que rarement Ă©tĂ© signalĂ©e. L'explication gĂ©nĂ©ralement avancĂ©e est que la surface des cristaux est recouverte d'un film liquide (prĂ©fusion de surface) bien avant que la tempĂ©rature de fusion volumique ne soit atteinte. Le but de cette courte note est de montrer que la surchauffe est possible et peut effectivement ĂȘtre observĂ©e (ÎT ⌠3°C) lorsque les cristaux sont limitĂ©s par des faces non mouillĂ©es (faces {111}) sĂ©parĂ©es par des parties courbes de trĂšs faible extension recouvertes de leur film liquide