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Equation 36 · Every Crystal Has Its Own Speed of Light

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0.9 ceff0.9\,c_{\mathrm{eff}}

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ceffc_{\mathrm{eff}}

Symbol c_eff

the including.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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A fourth fact transfers, but only with a correction the paper computes rather than sets aside. A quasiparticle wavepacket moving at speed v inside the linear window carries an internal clock — a spinor phase, a zitterbewegung oscillation — that runs slow by the familiar factor γ\gamma = (1 - v2v^2/ceff2c_{\mathrm{eff}}^2)^{-1/2} : 1.15 at v = 0.5\,ceffc_{\mathrm{eff}} , 2.29 at 0.9\,ceffc_{\mathrm{eff}} . That dilation is real and, in principle, measurable, but only inside a window whose edge the band’s own curvature sets. Writing the correction as a term proportional to (k/Λcurv\Lambda_{\mathrm{curv}})^2 , the fractional error in γ\gamma stays under one percent as long as the wavepacket’s momentum sits below…
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A fourth fact transfers, but only with a correction the paper computes rather than sets aside. A quasiparticle wavepacket moving at speed v inside the linear window carries an internal clock — a spinor phase, a zitterbewegung oscillation — that runs slow by the familiar factor γ\gamma = (1 - v2v^2/ceff2c_{\mathrm{eff}}^2)^{-1/2} : 1.15 at v = 0.5\,ceffc_{\mathrm{eff}} , 2.29 at 0.9\,ceffc_{\mathrm{eff}} . That dilation is real and, in principle, measurable, but only inside a window whose edge the band’s own curvature sets. Writing the correction as a term proportional to (k/Λcurv\Lambda_{\mathrm{curv}})^2 , the fractional error in γ\gamma stays under one percent as long as the wavepacket’s momentum sits below roughly a tenth of Λcurv\Lambda_{\mathrm{curv}} ; for graphene, where Λcurv\Lambda_{\mathrm{curv}} ≈\approx 1.5×\times10^{9} inverse metres, the clean window covers momenta up to about 1.5×\times10^{8} inverse metres. Dilation is graded structured rather than exact for exactly this reason: it holds inside a window with a computable edge, and the paper’s contribution is computing where that edge sits rather than asserting the effect and moving on.

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