Equation 117 · The Atlas That Refuses to Close
What does this equation mean?
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.
Read it piece by piece
Symbol delta_ij
deltj is part of the quantity the equation computes from the expression on the right.
Symbol u
u occurs above the fraction bar. The numerator is divided by the entire denominator below it.
Symbol Sigma
Sigma occurs above the fraction bar. The numerator is divided by the entire denominator below it.
Symbol X_i^mu
u occurs above the fraction bar. The numerator is divided by the entire denominator below it.
Symbol X_j^mu
u occurs above the fraction bar. The numerator is divided by the entire denominator below it.
Symbol rho_M
rh occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.
=
The expressions on both sides represent the same quantity under the stated assumptions.
See an illustrated explanation →subtraction
Subtract the following term or group from the preceding one. A leading minus marks a negative quantity.
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.
Numerator: big|X_i^mu(u,Sigma) - X_j^mu(u,Sigma)big|_Sigma
The complete quantity above the fraction bar.
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 , the observer-dependent stress-energy centroid , and the canonical Newton–Wigner operator , form a genuine, well-behaved sub-atlas. Define, for any two of them evaluated on the same hypersurface , . the proper spatial separation within between the two charts’ answers, normalized by the spin-to-mass length fixed in the first section. 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…
Read the full surrounding passage
Collect the pieces. Three charts, the Newtonian centroid , the observer-dependent stress-energy centroid , and the canonical Newton–Wigner operator , form a genuine, well-behaved sub-atlas. Define, for any two of them evaluated on the same hypersurface , . the proper spatial separation within between the two charts’ answers, normalized by the spin-to-mass length fixed in the first section. 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 0 for any spin, and it vanishes as S 0 for any observer or Lorentz frame. It is bounded above by exactly 1 for the observer-transition case, since || 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.
For background, read the article’s source list.
Return to The Atlas That Refuses to Close