Abstract
Using constant-pressure molecular-dynamics simulation we have studied the nature of ferroelastic phase transition in two-dimensional molecular monolayers. For Lennard-Jones interaction parameters appropriate for O2 molecules, we find, in contrast to the prediction of the renormalization-group calculation of the associated Ginzburg-Landau-Wilson Hamiltonian, a first-order phase transition to the paraelastic phase precipitated by the formation of large density of localized defects of herringbonelike structure. © 1986 The American Physical Society.
| Original language | English |
|---|---|
| Pages (from-to) | 484-487 |
| Number of pages | 4 |
| Journal | Physical Review Letters |
| Volume | 56 |
| Issue number | 5 |
| DOIs | |
| State | Published - Jan 1 1986 |
| Externally published | Yes |
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