On the metastability of the hexatic phase during the melting of two-dimensional charged particle solids

被引:19
作者
Derzsi, Aranka [1 ]
Kovacs, Aniko Zs. [1 ]
Donko, Zoltan [1 ,2 ]
Hartmann, Peter [1 ,2 ,3 ]
机构
[1] Hungarian Acad Sci, Inst Solid State Phys & Opt, Wigner Res Ctr Phys, H-1525 Budapest, Hungary
[2] Boston Coll, Dept Phys, Chestnut Hill, MA 02467 USA
[3] Baylor Univ, CASPER, Waco, TX 76798 USA
关键词
MOLECULAR-DYNAMICS; LENNARD-JONES; 2; DIMENSIONS; TRANSITION; CRYSTAL; SYSTEMS; ORDER;
D O I
10.1063/1.4866019
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
For two-dimensional many-particle systems, first-order, second-order, single step continuous, as well as two-step continuous (KTHNY-like) melting transitions have been found in previous studies. Recent computer simulations, using particle numbers in the >= 10(5) range, as well as a few experimental studies, tend to support the two-step scenario, where the solid and liquid phases are separated by a third, so called hexatic phase. We have performed molecular dynamics simulations on Yukawa (Debye-Huckel) systems at conditions earlier predicted to belong to the hexatic phase. Our simulation studies on the time needed for the equilibration of the systems conclude that the hexatic phase is metastable and disappears in the limit of long times. We also show that simply increasing the particle number in particle simulations does not necessarily result in more accurate conclusions regarding the existence of the hexatic phase. The increase of the system size has to be accompanied with the increase of the simulation time to ensure properly thermalized conditions. (C) 2014 AIP Publishing LLC.
引用
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页数:5
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