Kondo Metal and Ferrimagnetic Insulator on the Triangular Kagom\'e Lattice

We obtain the rich phase diagrams in the Hubbard model on the triangular Kagom\'e lattice as a function of interaction, temperature and asymmetry, by combining the cellular dynamical mean-field theory with the continuous time quantum Monte Carlo method. The phase diagrams show the asymmetry separates the critical points in Mott transition of two sublattices on the triangular Kagom\'e lattice and produces two novel phases called plaquette insulator with an obvious gap and a gapless Kondo metal. When the Coulomb interaction is stronger than the critical value Uc, a short range paramagnetic insulating phase, which is a candidate for the short rang resonating valence-bond spin liquid, emerges before the ferrimagnetic order is formed independent of asymmetry. Furthermore, we discuss how to measure these phases in future experiments

Strict ergodicity of affine p-adic dynamical systems on Zp

AbstractLet p⩾2 be a prime number and let Zp be the ring of all p-adic integers. For all α,β,z∈Zp, define Tα,β(z)=αz+β. It is shown that the dynamical system (Zp,Tα,β) is minimal if and only if α∈1+prpZp and β is a unit, here rp=1 (respectively rp=2) if p⩾3 (respectively if p=2), and that when it is minimal, it is strictly ergodic and topologically conjugate to (Zp,T1,1) with an analytic and isometric conjugacy. More importantly, when the system is not minimal, we find all its strictly ergodic components. As application, monomial systems Sn,ρ(z)=ρzn on the group 1+pZp are also discussed