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Equation 117 · The Atlas That Refuses to Close

What does this equation mean?

δij(u,Σ)=∣Xiμ(u,Σ)−Xjμ(u,Σ)∣ΣρM,\delta_{ij}(u,\Sigma) = \frac{\big|X_i^\mu(u,\Sigma) - X_j^\mu(u,\Sigma)\big|_\Sigma}{\rho_M},

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.

Start withbig|X_i^mu(u,Sigma) - X_j^mu(u,Sigma)big|_Sigma
Divide byrho_M
This relates todelta_ij(u,Sigma)
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

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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δij\delta_{ij}

Symbol delta_ij

deltaia_ij is part of the quantity the equation computes from the expression on the right.

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uu

Symbol u

u occurs above the fraction bar. The numerator is divided by the entire denominator below it.

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Σ\Sigma

Symbol Sigma

Sigma occurs above the fraction bar. The numerator is divided by the entire denominator below it.

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XiμX_i^\mu

Symbol X_i^mu

XimX_i^mu occurs above the fraction bar. The numerator is divided by the entire denominator below it.

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XjμX_j^\mu

Symbol X_j^mu

XjmX_j^mu occurs above the fraction bar. The numerator is divided by the entire denominator below it.

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ρM\rho_M

Symbol rho_M

rhoMo_M occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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fraction

fraction

Divide the expression above the line by the one below it.

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subtraction

subtraction

Subtract the following term or group from the preceding one. A leading minus marks a negative quantity.

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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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∣Xiμ(u,Σ)−Xjμ(u,Σ)∣Σ\big|X_i^\mu(u,\Sigma) - X_j^\mu(u,\Sigma)\big|_\Sigma

Numerator: big|X_i^mu(u,Sigma) - X_j^mu(u,Sigma)big|_Sigma

The complete quantity above the fraction bar.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction. Read it with the definitions, units, and assumptions supplied by the article.

What the article says around this equation

Collect the pieces. Three charts, the Newtonian centroid RN\mathbf R_N , the observer-dependent stress-energy centroid Xμ(u,Σ)X^\mu(u,\Sigma) , and the canonical Newton–Wigner operator XNW\mathbf X_{\mathrm{NW}} , form a genuine, well-behaved sub-atlas. Define, for any two of them evaluated on the same hypersurface Σ\Sigma , δij(u,Σ)=∣Xiμ(u,Σ)−Xjμ(u,Σ)∣ΣρM\delta_{ij}(u,\Sigma) = \frac{\big|X_i^\mu(u,\Sigma) - X_j^\mu(u,\Sigma)\big|_\Sigma}{\rho_M}. the proper spatial separation within Σ\Sigma between the two charts’ answers, normalized by the spin-to-mass length fixed in the first section. δij\delta_{ij} is dimensionless by construction, symmetric, zero exactly when the two charts coincide, and it has now been checked, not merely asserted, in both directions this kind of construction is required to pass: it…
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Collect the pieces. Three charts, the Newtonian centroid RN\mathbf R_N , the observer-dependent stress-energy centroid Xμ(u,Σ)X^\mu(u,\Sigma) , and the canonical Newton–Wigner operator XNW\mathbf X_{\mathrm{NW}} , form a genuine, well-behaved sub-atlas. Define, for any two of them evaluated on the same hypersurface Σ\Sigma , δij(u,Σ)=∣Xiμ(u,Σ)−Xjμ(u,Σ)∣ΣρM\delta_{ij}(u,\Sigma) = \frac{\big|X_i^\mu(u,\Sigma) - X_j^\mu(u,\Sigma)\big|_\Sigma}{\rho_M}. the proper spatial separation within Σ\Sigma between the two charts’ answers, normalized by the spin-to-mass length fixed in the first section. δij\delta_{ij} is dimensionless by construction, symmetric, zero exactly when the two charts coincide, and it has now been checked, not merely asserted, in both directions this kind of construction is required to pass: it vanishes as v/c →\to 0 for any spin, and it vanishes as S →\to 0 for any observer or Lorentz frame. It is bounded above by exactly 1 for the observer-transition case, since |Δ\Deltax\mathbf x| ≤\le ρM\rho_M was shown above to saturate rather than merely approach that value. Both checks are this construction’s kill criterion, run rather than assumed: had either limit failed to collapse the disagreement to zero, the atlas would have been reporting confusion between an artefact of convention and an artefact of mismatched apparatus, exactly the failure this kind of object is meant to be judged by.

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