Lattice field theory simulations of graphene

被引:134
作者
Drut, Joaquin E. [1 ]
Laehde, Timo A. [2 ]
机构
[1] Ohio State Univ, Dept Phys, Columbus, OH 43210 USA
[2] Univ Washington, Dept Phys, Seattle, WA 98195 USA
来源
PHYSICAL REVIEW B | 2009年 / 79卷 / 16期
基金
美国国家科学基金会;
关键词
band structure; equations of state; Fermi level; graphene; lattice field theory; Monte Carlo methods; HYBRID MONTE-CARLO; RENORMALIZATION-GROUP FLOW; FERMI-LIQUID BEHAVIOR; QUANTUM CHROMODYNAMICS; SUSPENDED GRAPHENE; SYMMETRY-BREAKING; CONTINUUM-LIMIT; TRANSITION; PHASE; DIMENSIONS;
D O I
10.1103/PhysRevB.79.165425
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We discuss the Monte Carlo method of simulating lattice field theories as a means of studying the low-energy effective theory of graphene. We also report on simulational results obtained using the Metropolis and Hybrid Monte Carlo methods for the chiral condensate, which is the order parameter for the semimetal-insulator transition in graphene, induced by the Coulomb interaction between the massless electronic quasiparticles. The critical coupling and the associated exponents of this transition are determined by means of the logarithmic derivative of the chiral condensate and an equation-of-state analysis. A thorough discussion of finite-size effects is given, along with several tests of our calculational framework. These results strengthen the case for an insulating phase in suspended graphene, and indicate that the semimetal-insulator transition is likely to be of second order, though exhibiting neither classical critical exponents, nor the predicted phenomenon of Miransky scaling.
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页数:14
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