Manuscript VII-E@1 · VII-E.tex · section · b713cf3c

Intrinsic angle defect at the exchange

Intrinsic angle defect at the exchange · lines 2796–2877

VII-E@1#eq:alpha-E, VII-E@1#eq:alpha-N, VII-E@1#eq:kappa

Back to manuscript

The angle at a vertex of a spacelike planar face is computed using the positive definite restriction of to that face. At , the two edge rays of the -face may be represented by

Their squared norms are equal to

and their inner product is . Thus

Reflection gives the same angle for .

For the -face, use

Then

and has the same angle. Both angles lie in .

The event junction therefore has defect

Since

strict decrease of cosine on gives . Hence .

At the incoming northern triple junction, the central edge points in direction . Its angle with the north-east arm satisfies

Because ,

The -angle is the same, and the -angle is . The triple-junction defect is consequently

Reflection gives the same value at the southern incoming junction.

At an outgoing triple junction the roles of and exchange: the two equal angles are , and the third is . Its defect is again . All relevant edge directions are constant within their respective epochs, so these defects are independent of there.

Thus the sum of the two central triple defects equals the single event defect on both sides. This is a statement about intrinsic geometry of the marked piecewise-flat slice. It is consistent with the identity ambient transition products proved in prop:products,prop:collar.

Displayed formulas in this passage

  • VII-E@1#eq:alpha-E · line 2809

  • VII-E@1#eq:alpha-N · line 2822

  • VII-E@1#eq:kappa · line 2831

  • unlabeled · line 2801

  • unlabeled · line 2805

  • unlabeled · line 2818

  • unlabeled · line 2836

  • unlabeled · line 2847

  • unlabeled · line 2853

  • unlabeled · line 2858

Nearby in this section