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		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Hard_disk_model&amp;diff=20577</id>
		<title>Hard disk model</title>
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		<updated>2022-09-29T21:12:11Z</updated>

		<summary type="html">&lt;p&gt;90.92.206.1: /* Phase transitions */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&#039;&#039;&#039;Hard disks&#039;&#039;&#039; are [[Hard sphere model |hard spheres]] in two dimensions. The hard disk  [[intermolecular pair potential]] is given by&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.1699114  Nicholas Metropolis, Arianna W. Rosenbluth, Marshall N. Rosenbluth, Augusta H. Teller and Edward Teller, &amp;quot;Equation of State Calculations by Fast Computing Machines&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;21&#039;&#039;&#039; pp.1087-1092  (1953)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://lib-www.lanl.gov/cgi-bin/getfile?00371200.pdf W. W. Wood &amp;quot;Monte Carlo calculations of the equation of state of systems of 12 and 48 hard circles&amp;quot;, Los Alamos Scientific Laboratory Report &#039;&#039;&#039;LA-2827&#039;&#039;&#039; (1963)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;&lt;br /&gt;
\Phi_{12}\left( r \right) = \left\{ \begin{array}{lll}&lt;br /&gt;
\infty &amp;amp; ; &amp;amp; r &amp;lt;  \sigma \\&lt;br /&gt;
0      &amp;amp; ; &amp;amp; r \ge \sigma \end{array} \right.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt; \Phi_{12}\left(r \right) &amp;lt;/math&amp;gt; is the [[intermolecular pair potential]] between two disks at a distance &amp;lt;math&amp;gt;r := |\mathbf{r}_1 - \mathbf{r}_2|&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt; \sigma &amp;lt;/math&amp;gt; is the diameter of the disk. This page treats hard disks in a two-dimensional space, for three dimensions see the page [[hard disks in a three dimensional space]].&lt;br /&gt;
==Phase transitions==&lt;br /&gt;
Despite the apparent simplicity of this model/system, the phase behaviour and the nature of the phase transitions remains an area of active study ever since the early work of Alder and Wainwright &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRev.127.359 B. J. Alder and T. E. Wainwright &amp;quot;Phase Transition in Elastic Disks&amp;quot;, Physical Review &#039;&#039;&#039;127&#039;&#039;&#039; pp. 359-361 (1962)]&amp;lt;/ref&amp;gt;. Recent works show a phase diagram containing an isotropic, a hexatic, and a solid phase &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevE.73.065104 C. H. Mak &amp;quot;Large-scale simulations of the two-dimensional melting of hard disks&amp;quot;, Physical Review E &#039;&#039;&#039;73&#039;&#039;&#039; 065104(R) (2006)]&amp;lt;/ref&amp;gt;. Highly efficient event-chain Monte Carlo simulations of over 1 million hard disks by Bernard and Krauth have solidified this picture, with a first-order phase transition between the fluid at packing fraction &amp;lt;math&amp;gt;\eta = 0.700&amp;lt;/math&amp;gt; and the hexatic phase at &amp;lt;math&amp;gt;\eta = 0.716&amp;lt;/math&amp;gt;, and a continuous transition between the hexatic and solid phases at  &amp;lt;math&amp;gt;\eta = 0.720&amp;lt;/math&amp;gt; &amp;lt;ref&amp;gt;[https://doi.org/10.1103/PhysRevLett.107.155704 E. P. Bernard and W. Krauth &amp;quot;Two-Step Melting in Two Dimensions: First-Order Liquid-Hexatic Transition&amp;quot;, Physical Review Letters &#039;&#039;&#039;107&#039;&#039;&#039; 155704  (2011)]&amp;lt;/ref&amp;gt;. Note that the maximum possible packing fraction is given by &amp;lt;math&amp;gt;\eta = \pi / \sqrt{12} \approx 0.906899...&amp;lt;/math&amp;gt; &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1007/BF01181430 L. Fejes Tóth &amp;quot;Über einen geometrischen Satz.&amp;quot; Mathematische Zeitschrift &#039;&#039;&#039;46&#039;&#039;&#039; pp. 83-85 (1940)]&amp;lt;/ref&amp;gt;. This scenario has since been confirmed using a variety of simulation methods &amp;lt;ref&amp;gt;[https://doi.org/10.1103/PhysRevLett.107.155704 M. Engel, J. A. Anderson, S. C. Glotzer, M. Tsobe, E. P. Bernard, and W. Krauth &amp;quot;Hard-disk equation of state: First-order liquid-hexatic transition in two dimensions with three simulation methods&amp;quot;, Physical Review E &#039;&#039;&#039;87&#039;&#039;&#039; 042134 (2013)]&amp;lt;/ref&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
Similar results have been found using the [[BBGKY hierarchy]] &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.3491039  Jarosław Piasecki, Piotr Szymczak, and John J. Kozak &amp;quot;Prediction of a structural transition in the hard disk fluid&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;133&#039;&#039;&#039; 164507 (2010)]&amp;lt;/ref&amp;gt; and by studying tessellations (the hexatic region: &amp;lt;math&amp;gt;0.680 &amp;lt; \eta &amp;lt; 0.729&amp;lt;/math&amp;gt;) &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1021/jp806287e John J. Kozak, Jack Brzezinski and Stuart A. Rice &amp;quot;A Conjecture Concerning the Symmetries of Planar Nets and the Hard disk Freezing Transition&amp;quot;, Journal of Physical Chemistry B &#039;&#039;&#039;112&#039;&#039;&#039; pp. 16059-16069 (2008)]&amp;lt;/ref&amp;gt;. Also studied via [[integral equations]] &amp;lt;ref&amp;gt;[https://doi.org/10.1063/1.5026496  Luis Mier-y-Terán, Brian Ignacio Machorro-Martínez, Gustavo A. Chapela, and Fernando del Río &amp;quot;Study of the hard-disk system at high densities: the fluid-hexatic phase transition&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;148&#039;&#039;&#039; 234502 (2018)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
Experimental results &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1103/PhysRevLett.118.158001 Alice L. Thorneywork, Joshua L. Abbott, Dirk G. A. L. Aarts, and Roel P. A. Dullens &amp;quot;Two-Dimensional Melting of Colloidal Hard Spheres&amp;quot;, Physical Review Letters &#039;&#039;&#039;118&#039;&#039;&#039; 158001 (2017)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Equations of state==&lt;br /&gt;
:&#039;&#039;Main article: [[Equations of state for hard disks]]&#039;&#039;&lt;br /&gt;
==Virial coefficients==&lt;br /&gt;
:&#039;&#039;Main article: [[Hard sphere: virial coefficients]]&#039;&#039;&lt;br /&gt;
==See also==&lt;br /&gt;
*[[Binary hard-disk mixtures]]&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1070/RM1970v025n02ABEH003794 Ya G Sinai &amp;quot;Dynamical systems with elastic reflections&amp;quot;, Russian Mathematical Surveys &#039;&#039;&#039;25&#039;&#039;&#039; pp. 137-189 (1970)]&lt;br /&gt;
*[http://dx.doi.org/10.1103/PhysRevB.30.2755     Katherine J. Strandburg, John A. Zollweg, and G. V. Chester &amp;quot;Bond-angular order in two-dimensional Lennard-Jones and hard-disk systems&amp;quot;, Physical Review B &#039;&#039;&#039;30&#039;&#039;&#039; pp. 2755 - 2759 (1984)]&lt;br /&gt;
*[http://dx.doi.org/10.1007/s00222-003-0304-9 Nándor Simányi &amp;quot;Proof of the Boltzmann-Sinai ergodic hypothesis for typical hard disk systems&amp;quot;, Inventiones Mathematicae  &#039;&#039;&#039;154&#039;&#039;&#039; pp. 123-178 (2003)]&lt;br /&gt;
*[http://dx.doi.org/10.1063/1.3687921 Roland Roth, Klaus Mecke, and Martin Oettel &amp;quot;Communication: Fundamental measure theory for hard disks: Fluid and solid&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;136&#039;&#039;&#039; 081101 (2012)]&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
*[http://www.smac.lps.ens.fr/index.php/Programs_Chapter_2:_Hard_disks_and_spheres Hard disks and spheres] computer code on SMAC-wiki.&lt;br /&gt;
[[Category: Models]]&lt;/div&gt;</summary>
		<author><name>90.92.206.1</name></author>
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