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Fluctuations of the two-dimensional quantum antiferromagnet in a disordered phase

V. I. Belinicher, João da Providência

Published May 11, 1999• 0 citations
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We investigate quantum phase transitions in the spin-1∕21∕21∕2 Heisenberg antiferromagnet on square lattices with inhomogeneous bond dilution. It is shown that quantum fluctuations can be continuously tuned by inhomogeneous bond dilution, eventually leading to the destruction of long-range magnetic order on the percolating cluster. Two multicritical points are identified at which the magnetic transition separates from the percolation transition, introducing a quantum phase transition. Beyond these multicritical points a quantum-disordered phase appears, characterized by an infinite percolating cluster with short ranged antiferromagnetic order. In this phase, the low-temperature uniform susceptibility diverges algebraically with non-universal exponents. This is a signature that the quantum-disordered phase is a quantum Griffiths phase, as also directly confirmed by the statistical distribution of local gaps. This study thus presents evidence of a genuine quantum Griffiths phenomenon in a two-dimensional Heisenberg antiferromagnet.
We report on the non‐trivial interplay between geometric randomess and quantum fluctuations in two‐dimensional S = 1/2 Heisenberg antiferromagnets (AFs), studied by quantum Monte Carlo. The case of the inhomogeneously bond‐diluted square lattice AF in zero field and of the site‐diluted bilayer AF in a finite magnetic field are emblematic examples of randomness‐induced quantum‐disordered phases on percolated lattices. These phases display unconventional properties, being gapless but with a finite correlation length.