2017
DOI: 10.1103/physrevb.95.134439
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Semiclassical approach to quantum spin ice

Abstract: International audienceWe propose a semiclassical description of the low-energy properties of quantum spin ice in the strong Ising limit. Within the framework of a semiclassical, perturbative Villain expansion, that can be truncated at arbitrary order, we give an analytic and quantitative treatment of the deconfining phase. We find that photon-photon interactions significantly renormalize the speed of light and split the two transverse photon polarizations at intermediate wave vectors. We calculate the photon v… Show more

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Cited by 14 publications
(40 citation statements)
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“…[33], we evaluated the correlator Dynamical structure factor S zz (q, ω) along high symmetry directions in the semiclassical QSI model at T = 10 −4 g. Photons manifest as a sharp, gapless, linearly dispersing branch of classical normal modes. The frequency of these modes matches excellently with large-S analytic predictions (green line) [38,58]. The integrated structure factor of the modes (red dots) is independent of q, as expected on grounds of equipartition.…”
Section: Photonssupporting
confidence: 77%
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“…[33], we evaluated the correlator Dynamical structure factor S zz (q, ω) along high symmetry directions in the semiclassical QSI model at T = 10 −4 g. Photons manifest as a sharp, gapless, linearly dispersing branch of classical normal modes. The frequency of these modes matches excellently with large-S analytic predictions (green line) [38,58]. The integrated structure factor of the modes (red dots) is independent of q, as expected on grounds of equipartition.…”
Section: Photonssupporting
confidence: 77%
“…A single set of remarkably sharp normal modes appear in the data [58]. The frequencies of the numerically obtained modes match perfectly with analytic results for the large-S photon dispersion [38] (green line in Fig. 2), confirming that the CSL simulated by our method is indeed equivalent to large-S QSI.…”
Section: Photonssupporting
confidence: 76%
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“…[13,14], namely c √ 0.8J(J − V). We expect higher-order corrections in the 1/S expansion to substantialy reduce this discrepancy [16]. The ground state of the S → ∞ model was obtained as a function of V/J by comparing the large-S minimum energy of ordered and resonating phases suggested in the literature [13,14,33].…”
Section: Diamond Latticementioning
confidence: 99%