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Equation 32 · Every Crystal Has Its Own Speed of Light

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cc

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cc

Symbol c

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Two facts transfer exactly, with no correction term anywhere, because they follow from locality alone rather than from any emergent Lorentz symmetry. Front-speed causality is simply the Lieb-Robinson bound restated: cLRc_{\mathrm{LR}} is a hard limit, and the statement that nothing propagates outside the cone is a proof about commutators, not an analogy borrowed from relativity. Effective causal order follows immediately — two operations separated by more than cLRc_{\mathrm{LR}} t commute up to an exponentially small tail, so a well-defined partial order of what can affect what exists inside the crystal for the same structural reason it exists in the vacuum. Massless-cone kinematics is the third…
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Two facts transfer exactly, with no correction term anywhere, because they follow from locality alone rather than from any emergent Lorentz symmetry. Front-speed causality is simply the Lieb-Robinson bound restated: cLRc_{\mathrm{LR}} is a hard limit, and the statement that nothing propagates outside the cone is a proof about commutators, not an analogy borrowed from relativity. Effective causal order follows immediately — two operations separated by more than cLRc_{\mathrm{LR}} t commute up to an exponentially small tail, so a well-defined partial order of what can affect what exists inside the crystal for the same structural reason it exists in the vacuum. Massless-cone kinematics is the third exact entry, carrying one scope condition: wherever a band is genuinely linear, its low-energy excitations obey the massless wave equation with cLRc_{\mathrm{LR}} , or the local Fermi velocity, standing in for c , and every kinematic consequence of that equation, Klein tunneling included, replays inside the window.

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