Evaporation/condensation of Ising droplets
Recently Biskup et al. [Europhys. Lett. 60 (2002) 21] studied the behaviour of d-dimensional finite-volume liquid-vapour systems at a fixed excess $\delta N$ of particles above the ambient gas density. They identify a dimensionless parameter $\Delta (\delta N)$ and a universal constant $\Delta_\math...
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| Hauptverfasser: | , , |
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| Dokumenttyp: | Article (Journal) Kapitel/Artikel |
| Sprache: | Englisch |
| Veröffentlicht: |
23 Sep 2005
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| In: |
Arxiv
Year: 2005, Pages: 1-6 |
| Online-Zugang: | Verlag, lizenzpflichtig, Volltext: http://arxiv.org/abs/hep-lat/0509112
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| Verfasserangaben: | Andreas Nussbaumer, Elmar Bittner and Wolfhard Janke |
| Zusammenfassung: | Recently Biskup et al. [Europhys. Lett. 60 (2002) 21] studied the behaviour of d-dimensional finite-volume liquid-vapour systems at a fixed excess $\delta N$ of particles above the ambient gas density. They identify a dimensionless parameter $\Delta (\delta N)$ and a universal constant $\Delta_\mathrm{c}(d)$ and show that for $\Delta < \Delta_c$ a droplet of the dense phase occurs while for $\Delta > \Delta_c$ the excess is absorbed in the background. The fraction $\lambda_\Delta$ of excess particles forming the droplet is given explicitly. Furthermore, they state, that the same is true for solid-gas systems. To verify these results, we have simulated the spin-1/2 Ising model on a square lattice at constant magnetisation equivalent to a fixed particle excess in the lattice-gas picture. We measured the largest minority droplet, corresponding to the solid phase, at various system sizes ($L=40, ..., 640$). Using analytic values for the spontaneous magnetisation $m_0$, the susceptibility $\chi$ and interfacial free energy $\tau_\mathrm{W}$ for the infinite system, we were able to determine $\lambda_\Delta$ in very good agreement with the theoretical prediction. |
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| Beschreibung: | Gesehen am 13.10.2022 |
| Beschreibung: | Online Resource |