2022
DOI: 10.1088/1751-8121/aca36d
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Classical ground states of spin lattices

Abstract: We present a generalization of the Luttinger-Tisza-Lyons-Kaplan (LTLK) theory of classical ground states of Bravais lattices with Heisenberg coupling to non-Bravais lattices. It consists of adding certain Lagrange parameters to the diagonal of the Fourier transformed coupling matrix analogous to the theory of the general ground state problem already published. This approach is illustrated by an application to a modified honeycomb lattice, which has exclusive three-dimensional ground states as well as a classic… Show more

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Cited by 7 publications
(3 citation statements)
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“…, n analytically and thus obtain explicit or parametric expressions for the magnetization curve. Alternatively, we used a generalized Luttinger-Tisza method [43] to obtain analytical results for the latter case. This method provides rigorous results and it can be used to confirm the semi-analytical results.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…, n analytically and thus obtain explicit or parametric expressions for the magnetization curve. Alternatively, we used a generalized Luttinger-Tisza method [43] to obtain analytical results for the latter case. This method provides rigorous results and it can be used to confirm the semi-analytical results.…”
Section: Methodsmentioning
confidence: 99%
“…When the magnetic field H reaches or exceeds a certain saturation value H sat , all spins align parallel to the direction of the magnetic field. In calculating H sat for the systems considered in this work we have followed the approach presented in [43][44][45], which will be briefly recapitulated here. This approach is limited to finite spin systems but it turns out that the results for H sat are independent of the system size (provided N is not too small) and hence also hold for the infinite square-kagomé spin lattice.…”
Section: Data Availability Statementmentioning
confidence: 99%
“…5 with J × < 0 and J + ≥ 0, which can be derived by applying the generalized Luttinger-Tisza method of Ref. [40], see also the Mathematica files in the Supplement [41]. In this cuboc-d phase, the antipodal squares of the cuboctahedron are deformed into non-coplanar closed polygon chains with equal edges, while the square in the equatorial plane is deformed into a coplanar rectangle.…”
Section: Cuboc Ordermentioning
confidence: 99%