We study the ground-state phase diagram of the quantum J 1 − J 2 model on the honeycomb lattice by means of an entangled-plaquette variational ansatz. Values of energy and relevant order parameters are computed in the range 0 J 2 /J 1 1. The system displays classical order for J 2 /J 1 0.2 (Néel) and for J 2 /J 1 0.4 (collinear). In the intermediate region, the ground state is disordered. Our results show that the reduction of the half-filled Hubbard model to the model studied here does not yield accurate predictions.
We present results of a theoretical study of para-hydrogen and
ortho-deuterium clusters at low temperature (0.5 K < T < 3.5 K), based on Path
Integral Monte Carlo simulations. Clusters of size up to N=21 para-hydrogen
molecules are nearly entirely superfluid at T < 1 K. For 21 < N < 30, the
superfluid response displays strong variations with N, reflecting structural
changes that occur on adding or removing even a single molecule. Some clusters
in this size range display quantum melting, going from solid- to liquid-like as
T tends to 0. Melting is caused by quantum exchanges of molecules. The largest
para-hydrogen cluster for which a significant superfluid response is observed
comprises 27 molecules. Evidence of a finite superfluid response is presented
for ortho-deuterium clusters of size up to 14 molecules. Magic numbers are
observed, at which both types of clusters feature pronounced stability.Comment: 11 pages, 16 figure
Abstract. We propose a new ansatz for the ground-state wave function of quantum many-body systems on a lattice. The key idea is to cover the lattice with plaquettes and obtain a state whose configurational weights can be optimized by means of a variational Monte Carlo algorithm. Such a scheme applies to any dimension, without any 'sign' instability. We show results for various twodimensional spin models (including frustrated ones). A detailed comparison with available exact results, as well as with variational methods based on different ansatze, is offered. In particular, our numerical estimates are in quite good agreement with exact ones for unfrustrated systems, and compare favorably to other methods for frustrated ones.
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