Equation 51 · Every Crystal Has Its Own Speed of Light
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Read the formula alongside the article passage below. Each part has a deeper page with its role in the equation, the supporting passage and nearby citations.
This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.
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Symbol v_LR
R is the quantity selected or evaluated by the optimization written on the right.
Symbol e
e appears in the objective or constraint used by the optimization on the right.
Symbol J_max
ax appears in the objective or constraint used by the optimization on the right.
=
The expressions on both sides represent the same quantity under the stated assumptions.
See an illustrated explanation →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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What the article says around this equation
The first verdict is a genuine win for the theory. Every exponent measured is super-linear — > 1 at seven of the eight points — exactly where the long-range bound says a finite-velocity linear cone is not guaranteed and faster-than-linear growth is required instead, and the propagation outright violates the nearest-neighbour bound = 12e once drops below 1 [ 4 ] . Read against a naive short-range picture, the ion chain is unambiguously non-local. The second verdict tempers the first: the three competing long-range thresholds theory offers — a worst-case bound, a typical-state bound, and a free-particle bound — all sit above = 2 , while Richerme’s…
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The first verdict is a genuine win for the theory. Every exponent measured is super-linear — > 1 at seven of the eight points — exactly where the long-range bound says a finite-velocity linear cone is not guaranteed and faster-than-linear growth is required instead, and the propagation outright violates the nearest-neighbour bound = 12e once drops below 1 [ 4 ] . Read against a naive short-range picture, the ion chain is unambiguously non-local. The second verdict tempers the first: the three competing long-range thresholds theory offers — a worst-case bound, a typical-state bound, and a free-particle bound — all sit above = 2 , while Richerme’s scan stops at = 1.19 , so the data occupy a regime where all three theories predict the same qualitative behaviour and the experiment cannot say which one is actually being tested. Discriminating between them would need a scan crossing a threshold, which this dataset was never built to provide. The third verdict resists tidying altogether: the XY measurement at = 1.19 gives = 1.67 0.08 , growing super-linearly even though a naive count of the interaction’s range would call it short enough to behave, and no published theory accounts for it. The confrontation names that gap rather than explaining it away.
Sources cited in the surrounding passage
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