2020
DOI: 10.1103/physrevlett.124.087205
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Possible Kitaev Quantum Spin Liquid State in 2D Materials with S=3/2

Abstract: Quantum spin liquids (QSLs) form an extremely unusual magnetic state in which the spins are highly correlated and fluctuate coherently down to the lowest temperatures, but without symmetry breaking and without the formation of any static long-range-ordered magnetism. Such intriguing phenomena are not only of great fundamental relevance in themselves, but also hold the promise for quantum computing and quantum information. Among different types of QSLs, the exactly solvable Kitaev model is attracting much atten… Show more

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Cited by 132 publications
(93 citation statements)
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“…In a certain reference frame, the former appear as off-diagonal elements and the latter as a purely diagonal one (see, e.g., Refs. [32,34]). In order to analyze all bonds at once, we show the three eigenvalues of the J S tensor (denoted as J S ), which contain a combined effect of the two types of couplings, discussed above.…”
Section: A Cri 3 Bulkmentioning
confidence: 99%
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“…In a certain reference frame, the former appear as off-diagonal elements and the latter as a purely diagonal one (see, e.g., Refs. [32,34]). In order to analyze all bonds at once, we show the three eigenvalues of the J S tensor (denoted as J S ), which contain a combined effect of the two types of couplings, discussed above.…”
Section: A Cri 3 Bulkmentioning
confidence: 99%
“…Both DM and Kitaev interactions originate from spin-orbit coupling (SOC) and therefore they are usually small in 3d-based materials (smaller than the Heisenberg exchange). However, in the case of CrI 3 it is the orbitals of heavy iodine atoms that carry substantial SOC and is the source of anisotropic interactions [32][33][34][35]. The sets of magnetic interaction parameters extracted from various experiments and theoretical calculations are vastly different (for review, see Ref.…”
Section: Introductionmentioning
confidence: 99%
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“…Like the on-site magnetic anisotropy, the eigenvectors of the J 12 matrix can be used to specify the easy, intermediate, and hard axes of a given pair of magnetic atoms (see Appendix A). For very anisotropic systems, this leads to the Kitaev bonddependent symmetric exchange anisotropy [9,50]. The twosite interactions are augmented with the isotropic biquadratic interaction B 12 (S 1 • S 2 ) 2 and with the recently uncovered chiral biquadratic interaction…”
Section: Two-site Interactionsmentioning
confidence: 99%
“…First, the energy of different magnetic structures can be systematically mapped to a spin cluster expansion [45][46][47][48][49], of which the four-state mapping method is a simplified form able to determine all types of two-spin interactions (see, for instance, Ref. [50] for an application to the Kitaev interaction). In Ref.…”
Section: Introductionmentioning
confidence: 99%