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arXiv:1405.3260 · Physical Review B

Exotic magnetization plateaus in a quasi-two-dimensional Shastry-Sutherland model

G. R. Foltin, Salvatore R. Manmana, Kai Phillip Schmidt

Published Sep 3, 2014• 23 citations
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Abstract

We find unconventional Mott insulators in a quasi-2D version of the Shastry-Sutherland model in a magnetic field. In our realization on a four-leg tube geometry, these are stabilized by correlated hopping of localized magnetic excitations. Using perturbative continuous unitary transformations (pCUTs, plus classical approximation or exact diagonalization) and the density matrix renormalisation group method (DMRG), we identify prominent magnetization plateaus at magnetizations $M=1/8,3/16,1/4$, and $1/2$. While the plateau at $M=1/4$ can be understood in a semiclassical fashion in terms of diagonal stripes, the plateau at $M=1/8$ displays highly entangled wheels in the transverse direction of the tube. Finally, the $M=3/16$ plateau is most likely to be viewed as a classical 1/8 structure on which additional triplets are fully delocalized around the tube. The classical approximation of the effective model fails to describe all these plateau structures which benefit from correlated hopping. We relate our findings to the full 2D system, which is the underlying model for the frustrated quantum magnet $\mathrm{SrCu}{({\mathrm{BO}}_{3})}_{2}$.

DOI
10.1103/physrevb.90.104404

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We study the magnetization process in two-dimensional S=1/2S=1/2S=1/2 spin systems, to discuss the appearance of a plateau structure. The following three cases are considered: (1) the Heisenberg antiferromagnet and multiple-spin exchange model on the triangular lattice, (2) the Shastry-Sutherland-type lattice [which is a possible model for SrCu2(BO3)2],{\mathrm{SrCu}}_{2}({\mathrm{BO}}_{3}{)}_{2}],SrCu2​(BO3​)2​], (3) the 1/5-depleted lattice (for CaV4O9).{\mathrm{CaV}}_{4}{\mathrm{O}}_{9}).CaV4​O9​). We find in these systems that magnetization plateaus can appear owing to a transition from superfluid to a Mott insulator of magnetic excitations. The plateau states have charge-density-wave order of the excitations. The magnetizations of the plateaus depend on components of the magnetic excitations, the range of the repulsive interaction, and the geometry of the lattice.
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Abstract. We study an extended two-dimensional Shastry-Sutherland model in a magnetic field where besides the usual Heisenberg exchanges of the Shastry-Sutherland model two additional SU(2) invariant couplings are included. Perturbative continous unitary transformations are used to determine the leading order effects of the additional couplings on the pure hopping and on the long-range interactions between the triplons which are the most relevant terms for small magnetization. We then compare the energy of various magnetization plateaux in the classical limit and we discuss the implications for the two-dimensional quantum magnet SrCu2(BO3)2. 1.
The quantum phase transitions induced by a magnetic field are theoretically studied in a frustrated two-leg spin ladder. Using the density-matrix renormalization-group method, we find some magnetic phase transitions and plateaux in two different cases of strong and weak rung couplings. With the strong rung coupling, the three magnetization plateaux are found at 1/3, 1/2, and 2/3 due to the frustration. Those can be understood in terms of a quasi-spinon reconstructed from the singlet and the triplets of spins on a rung. The plateau at 1/2 corresponds to the valence bond solid of the quasispinons, while the plateaux at 1/3 and 2/3 can be associated with the array of quasi-spinons such as soliton lattice. This is different from the usual Bose-Einstein-condensation picture of triplons. Our results will be useful to understand magnetization curves in BiCu2PO6.