{ "id": "1702.08632", "version": "v1", "published": "2017-02-28T03:44:11.000Z", "updated": "2017-02-28T03:44:11.000Z", "title": "Critical behaviour in two-dimensional Coulomb Glass at zero temperature", "authors": [ "Preeti Bhandari", "Vikas Malik", "Syed Rashid Ahmad" ], "comment": "9 pages, 13 figures", "categories": [ "cond-mat.dis-nn" ], "abstract": "The lattice model of Coulomb Glass in two dimensions with box-type random field distribution is studied at zero temperature for system size upto $96^{2}$. To obtain the minimum energy state we annealed the system using Monte Carlo simulation followed by further minimization using cluster-flipping. The values of the critical exponents are determined using the standard finite size scaling. We found that the correlation length $\\xi$ diverges with an exponent $\\nu=1.0$ at the critical disorder $W_{c} = 0.2253$ and that $\\chi_{dis} \\approx \\xi^{4-\\bar{\\eta}}$ with $\\bar{\\eta}=2$ for the disconnected susceptibility. The staggered magnetization behaves discontinuously around the transition and the critical exponent of magnetization $\\beta=0$. The probability distribution of the staggered magnetization shows a three peak structure which is a characteristic feature for the phase coexistence at first-order phase transition. In addition to this, at the critical disorder we have also studied the properties of the domain for different system sizes. In contradiction with the Imry-Ma arguments, we found pinned and non-compact domains where most of the random field energy was contained in the domain wall. Our results are also inconsistent with Binder's roughening picture.", "revisions": [ { "version": "v1", "updated": "2017-02-28T03:44:11.000Z" } ], "analyses": { "keywords": [ "two-dimensional coulomb glass", "zero temperature", "critical behaviour", "box-type random field distribution", "monte carlo simulation" ], "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable" } } }