63 research outputs found

    Unexpected z-Direction Ising Antiferromagnetic Order in a frustrated Spin-1/2 J1βˆ’J2J_1-J_2 XY Model on the Honeycomb Lattice

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    Using the density matrix renormalization group (DMRG) on wide cylinders, we study the phase diagram of the spin-1/2 XY model on the honeycomb lattice, with first-neighbor (J1=1J_1 = 1) and frustrating second-neighbor (J2>0J_2>0) interactions. For the intermediate frustration regime 0.22≲J2≲0.360.22\lesssim J_2\lesssim0.36, we find a surprising antiferromagnetic Ising phase, with ordered moments pointing along the z axis, despite the absence of any S_z_z interactions in the Hamiltonian. Surrounding this phase as a function of J2J_2 are antiferromagnetic phases with the moments pointing in the xβˆ’yx-y plane for small J2J_2 and a close competition between an xβˆ’yx-y plane magnetic collinear phase and a dimer phase for large values of J2J_2. We do not find any spin liquid phases in this model.Comment: 5 pages, 5 figures, minor changes made for publication on PR

    Weak plaquette valence bond order in the S=1/2S=1/2 honeycomb J1βˆ’J2J_1-J_2 Heisenberg model

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    Using the density matrix renormalization group, we investigate the S=1/2S=1/2 Heisenberg model on the honeycomb lattice with first- (J1J_1) and second-neighbor (J2J_2) interactions. We are able to study long open cylinders with widths up to 12 lattice spacings. For J2/J1J_2/J_1 near 0.3, we find an apparently paramagnetic phase, bordered by an antiferromagnetic phase for J2≲0.26J_2\lesssim 0.26 and by a valence bond crystal for J2≳0.36J_2\gtrsim 0.36. The longest correlation length that we find in this intermediate phase is for plaquette valence bond (PVB) order. This correlation length grows strongly with cylinder circumference, indicating either quantum criticality or weak PVB order.Comment: 9 pages, 15 figures, minor changes are made for publication in Phys. Rev. Let

    Time reversal Aharonov-Casher effect in mesoscopic rings with Rashba spin-orbital interaction

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    The time reversal Aharonov-Casher (AC) interference effect in the mesoscopic ring structures, based on the experiment in Phys. Rev. Lett. \textbf{97}, 196803 (2006), is studied theoretically. The transmission curves are calculated from the scattering matrix formalism, and the time reversal AC interference frequency is singled out from the Fourier spectra in numerical simulations. This frequency is in good agreement with analytical result. It is also shown that in the absent of magnetic field, the Altshuler-Aronov-Spivak type (time reversal) AC interference retains under the influence of strong disorder, while the Aharonov-Bohm type AC interference is suppressed.Comment: 5 pages, 4 figures, accepted by Phys. Rev.

    Disorder-Induced Mimicry of a Spin Liquid in YbMgGaO4_4

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    We suggest that a randomization of the pseudo-dipolar interaction in the spin-orbit-generated low-energy Hamiltonian of YbMgGaO4_4 due to an inhomogeneous charge environment from a natural mixing of Mg2+^{2+} and Ga3+^{3+} can give rise to orientational spin disorder and mimic a spin-liquid-like state. In the absence of such quenched disorder, 1/S1/S and density matrix renormalization group calculations both show robust ordered states for the physically relevant phases of the model. Our scenario is consistent with the available experimental data and further experiments are proposed to support it.Comment: 5+ main text, 7+ supplemental, text asymptotically close to PR

    Topography of Spin Liquids on a Triangular Lattice

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    Spin systems with frustrated anisotropic interactions are of significant interest due to possible exotic ground states. We have explored their phase diagram on a nearest-neighbor triangular lattice using the density-matrix renormalization group and mapped out the topography of the region that can harbor a spin liquid. We find that this spin-liquid phase is continuously connected to a previously discovered spin-liquid phase of the isotropic J1β€‰β£βˆ’β€‰β£J2J_1\!-\!J_2 model. The two limits show nearly identical spin correlations, making the case that their respective spin liquids are isomorphic to each other.Comment: Accepted to PRL; 5 p., 11+ p. supplemental; main text is longer than the accepted versio
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