Equation 41 · Every Crystal Has Its Own Speed of Light
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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 = (1 - /)^{-1/2} : 1.15 at v = 0.5\, , 2.29 at 0.9\, . 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/)^2 , the fractional error in 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 = (1 - /)^{-1/2} : 1.15 at v = 0.5\, , 2.29 at 0.9\, . 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/)^2 , the fractional error in stays under one percent as long as the wavepacket’s momentum sits below roughly a tenth of ; for graphene, where 1.510^{9} inverse metres, the clean window covers momenta up to about 1.510^{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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