We study electron correlations in the half-filled Hubbard model on two-dimensional Penrose lattice. Applying the real-space dynamical mean-field theory to large clusters, we discuss how low-temperature properties are affected by the quasiperiodic structure. By calculating the double occupancy and renormalization factor at each site, we clarify the existence of the Mott transition. The spatially-dependent renormalization characteristic of geometrical structure is also addressed.
KEYWORDS: Hubbard model, Penrose lattice, dynamical mean-field theoryQuasiperiodic systems have attracted considerable interest since the discovery of quasicrystal.1) One of the specific features is the existence of the long-range order without translational symmetry. This should induce interesting low-temperature properties in the metallic quasicrystals such as electric and thermal conductivities.2, 3) The tight-binding model on the quasiperiodic lattices, which may describe some quasicrystal compounds, has been studied and intrinsic properties such as the existence of the confined state and fractal dimensions, have been clarified. 7,8) In the former compound, the specific heat and susceptibility exhibit power-law behavior with a nontrivial exponent at low temperatures. In contrast, the approximant with the periodic structure shows conventional heavy fermion behavior. These should suggest that electron correlations and quasiperiodic structure play a crucial role in stabilizing quantum critical behavior at low temperatures. Therefore, it is desirable to clarify how electron correlations affect low temperature properties in the quasiperiodic system.Motivated by this, we study correlated electron systems on the quasiperiodic lattice. One of the simplest questions is how the introduction of the Coulomb interaction forms the quasiparticles and leads to the Mott transition in the system since coordination number and geometrical structure depend on the lattice sites. To attack this fundamental problem, we focus on the halffilled Hubbard model on a two-dimensional Penrose lattice, where a site is placed on each vertex of the rhombuses [see Fig. 1(a)]. We apply the real-space dynamical mean-field theory (RDMFT) 9) to the Hubbard model, and discuss electron correlations in the system. Calculating renormalization factor and double occupancy at each site, we study how the Coulomb interactions yield the spatially-dependent renormalization, typically close to the Mott transition point.In this paper, we consider the single-band Hubbard model on the Penrose lattice, which should be given by * E-mail address: takemori@stat.phys.titech.ac.jp