Abstract
We investigate the effect of dimensional crossover in the ground state of the antiferromagnetic spin-$1$ Heisenberg model on the anisotropic triangular lattice that interpolates between the regime of weakly coupled Haldane chains ($J^{\prime}\! \!\ll\!\! J$) and the isotropic triangular lattice ($J^{\prime}\!\!=\!\!J$). We use the density-matrix renormalization group (DMRG) and Schwinger boson theory performed at the Gaussian correction level above the saddle-point solution. Our DMRG results show an abrupt transition between decoupled spin chains and the spirally ordered regime at $(J^{\prime}/J)_c\sim 0.42$, signaled by the sudden closing of the spin gap. Coming from the magnetically ordered side, the computation of the spin stiffness within Schwinger boson theory predicts the instability of the spiral magnetic order toward a magnetically disordered phase with one-dimensional features at $(J^{\prime}/J)_c \sim 0.43$. The agreement of these complementary methods, along with the strong difference found between the intra- and the interchain DMRG short spin-spin correlations; for sufficiently large values of the interchain coupling, suggests that the interplay between the quantum fluctuations and the dimensional crossover effects gives rise to the one-dimensionalization phenomenon in this frustrated spin-$1$ Hamiltonian.
Highlights
The role played by quantum fluctuations in low dimensional antiferromagnets is quite well understood when frustration is not present.[1]
In this paper we investigate the phenomenon of one dimensionalization in the AF spin-1 Heisenberg model that interpolates between the 1D decoupled chains and the triangular lattice by mean of two complementary methods: density-matrix renormalization group (DMRG) and the Schwinger boson theory performed at the more reliable Gaussian correction level above the saddle-point solution
We have investigated the one dimensionalization phenomenon in the spin-1 Heisenberg model on the anisotropic triangular lattice using two complementary methods: DMRG and Schwinger boson theory computed up to Gaussian correction level
Summary
The role played by quantum fluctuations in low dimensional antiferromagnets is quite well understood when frustration is not present.[1]. The interpolation between the decoupled chains and the frustrated triangular lattice (see Fig 1 with J = 1 and J = J , with J varying from 0 to 1), for spin-1/2, yields a non trivial interplay between the dimensional crossover and the quantum fluctuation effects that induces a marked reduction of the interchain correlations. Coming from the 2D magnetically ordered regime, the DMRG computation of the critical value Jc is quite difficult to determine since incommensurate spiral phases are expected near the transition to the Haldane regime This requires the implementation of open boundary conditions along with larger lattice sizes in order to properly accommodate the magnetic wave vector[19]. We resort to the Schwinger boson theory, which is reliable for the study of 2D systems.[20,22,23,24]
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