2016
DOI: 10.1103/physrevb.93.214425
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Energy dynamics in the Heisenberg-Kitaev spin chain

Abstract: We study the Heisenberg-Kitaev chain in order to uncover the interplay between two qualitatively different integrable points in the physics of heat transport in one dimension. Focusing on high temperatures and using analytical as well as numerical approaches within linear response theory, we explore several directions in parameter space including exchange-coupling ratios, anisotropies, and external magnetic fields. We show the emergence of purely ballistic energy transport at all integrable points, manifest in… Show more

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Cited by 20 publications
(18 citation statements)
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“…Such conclusion is a bit different from the finding in Ref. [44], where the translation invariance of local energy densities is violated. The ground state of H can be considered as a current-carrying steady state of H GCM at zero temperature, and the ground-state expectation value of current operator J E ≡ Ĵ E acts as an order parameter indicating the presence of an energy current, as shown in Fig.…”
Section: Three-site Interactionscontrasting
confidence: 96%
“…Such conclusion is a bit different from the finding in Ref. [44], where the translation invariance of local energy densities is violated. The ground state of H can be considered as a current-carrying steady state of H GCM at zero temperature, and the ground-state expectation value of current operator J E ≡ Ĵ E acts as an order parameter indicating the presence of an energy current, as shown in Fig.…”
Section: Three-site Interactionscontrasting
confidence: 96%
“…Therefore we have shown the 2D Kitaev model to be a normal dissipative heat conductor. This is in stark contrast to the Kitaev ladder, which is an insulator with a vanishing Drude weight and dc limit of the dynamical conductivity [58], as well as the one dimensional Kitaev chain, which is a ballistic conductor [57] and features a finite Drude weight (DW). We find, that for the 2D Kitaev model, the DW is finite only on small systems or when gauge excitations are completely neglected.…”
Section: Discussionmentioning
confidence: 89%
“…We caution that the only requirement for h(r) is, that H =´d 3 r h(r). This may be a reason for differing quantitative results for the Drude weight and the regular conductivity spectrum, obtained in recent studies of various frustrated and spin ladder models [54,57,60,61]. However, it is generally believed that universal qualitative statements, concerning the existence or absence of finite Drude weights and dc conductivities are insensitive to the freedom of choice for the energy density.…”
Section: Thermal Transportmentioning
confidence: 99%
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“…It depends on θ in general. For θ=0, it will present an XZX type, while it exhibits a XZY type for θ = π/2 [61]. For simplicity we choose θ = π/2 in this term while still keep θ as an arbitrary variable in the compass chain.…”
Section: Appendix: Current Operator For the Compass Modelmentioning
confidence: 99%