The normalized incidence graph and its parabolic vertices #
The published proof of Proposition 8 dismisses the case p ≡ 1 (mod 4) as simpler
because of the parabolic lines. This file records the missing argument without folding
normalized trace coordinates back into the original Markoff coordinates.
The key fact is stronger than mere connectivity: after choosing i² = -1, a fiber whose
normalized coordinate is 2 or -2 meets every fiber on either different coordinate axis.
The three coordinate axes used to index normalized conic fibers.
- first : NormalizedCoordinateAxis
- second : NormalizedCoordinateAxis
- third : NormalizedCoordinateAxis
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A normalized conic fiber, indexed without identifying normalized and original coordinates.
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- BGS.Markoff.normalizedFiberAt BGS.Markoff.NormalizedCoordinateAxis.first x✝ = BGS.Markoff.normalizedFiber1 x✝
- BGS.Markoff.normalizedFiberAt BGS.Markoff.NormalizedCoordinateAxis.second x✝ = BGS.Markoff.normalizedFiber2 x✝
- BGS.Markoff.normalizedFiberAt BGS.Markoff.NormalizedCoordinateAxis.third x✝ = BGS.Markoff.normalizedFiber3 x✝
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The action of swapping the first two coordinates on axis labels.
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- BGS.Markoff.normalizedSwap12Axis BGS.Markoff.NormalizedCoordinateAxis.first = BGS.Markoff.NormalizedCoordinateAxis.second
- BGS.Markoff.normalizedSwap12Axis BGS.Markoff.NormalizedCoordinateAxis.second = BGS.Markoff.NormalizedCoordinateAxis.first
- BGS.Markoff.normalizedSwap12Axis BGS.Markoff.NormalizedCoordinateAxis.third = BGS.Markoff.NormalizedCoordinateAxis.third
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The action of swapping the last two coordinates on axis labels.
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- BGS.Markoff.normalizedSwap23Axis BGS.Markoff.NormalizedCoordinateAxis.first = BGS.Markoff.NormalizedCoordinateAxis.first
- BGS.Markoff.normalizedSwap23Axis BGS.Markoff.NormalizedCoordinateAxis.second = BGS.Markoff.NormalizedCoordinateAxis.third
- BGS.Markoff.normalizedSwap23Axis BGS.Markoff.NormalizedCoordinateAxis.third = BGS.Markoff.NormalizedCoordinateAxis.second
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Two normalized conic fibers meet when their set-theoretic intersection is nonempty.
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- BGS.Markoff.NormalizedFibersMeet s t = (s ∩ t).Nonempty
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Coordinate swapping transports a meeting of normalized fibers.
Swapping the last two coordinates transports a meeting of normalized fibers.
Divide a normalized trace coordinate by three without identifying its type with an original Markoff coordinate.
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Original-coordinate admissibility is exactly the complement of the zero and parabolic normalized trace values.
Scaling a meeting of an original first-axis and third-axis fiber gives the corresponding meeting in normalized trace coordinates.
Scaling a meeting of an original second-axis and third-axis fiber gives the corresponding meeting in normalized trace coordinates.
The normalized, type-distinct form of the existing admissible bridge for the first two axes.
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Transport the proved original-coordinate admissible bridge through the explicit scaling equivalence.
The normalized admissible bridge for primes congruent to one modulo four.
The graph-level admissible bridge, with coordinate permutations made explicit.
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The fixed-axis admissible bridge implies the full graph-level bridge. Every coordinate permutation is applied to the actual intersection witness.
The graph-level admissible bridge for all sufficiently large primes congruent to one modulo four.
The trace-2 fiber on the first axis meets every second-axis fiber.
The trace--2 fiber on the first axis meets every second-axis fiber.
A parabolic first-axis fiber meets every second-axis fiber.
The trace-2 fiber on the first axis meets every third-axis fiber.
The trace--2 fiber on the first axis meets every third-axis fiber.
A parabolic first-axis fiber meets every third-axis fiber.
When i² = -1, the zero fiber on the first axis meets every second-axis fiber.
When i² = -1, the zero fiber on the first axis meets every third-axis fiber.
A parabolic fiber on any axis meets every fiber on a different axis.
A zero-coordinate fiber meets every fiber on a different axis when -1 is a square.
Every coordinate excluded by admissibility meets every fiber on a different axis when
-1 is a square.
If one vertex is parabolic and the other vertex is on the same axis, any point of the other fiber supplies a common neighbor on either different axis.
A deterministic choice of an axis different from each of two supplied axes.
Equations
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.first BGS.Markoff.NormalizedCoordinateAxis.first = BGS.Markoff.NormalizedCoordinateAxis.second
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.first BGS.Markoff.NormalizedCoordinateAxis.second = BGS.Markoff.NormalizedCoordinateAxis.third
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.first BGS.Markoff.NormalizedCoordinateAxis.third = BGS.Markoff.NormalizedCoordinateAxis.second
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.second BGS.Markoff.NormalizedCoordinateAxis.first = BGS.Markoff.NormalizedCoordinateAxis.third
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.second BGS.Markoff.NormalizedCoordinateAxis.second = BGS.Markoff.NormalizedCoordinateAxis.first
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.second BGS.Markoff.NormalizedCoordinateAxis.third = BGS.Markoff.NormalizedCoordinateAxis.first
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.third BGS.Markoff.NormalizedCoordinateAxis.first = BGS.Markoff.NormalizedCoordinateAxis.second
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.third BGS.Markoff.NormalizedCoordinateAxis.second = BGS.Markoff.NormalizedCoordinateAxis.first
- BGS.Markoff.normalizedBridgeAxis BGS.Markoff.NormalizedCoordinateAxis.third BGS.Markoff.NormalizedCoordinateAxis.third = BGS.Markoff.NormalizedCoordinateAxis.first
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A nonempty fiber meets some fiber on every different axis: use the corresponding coordinate of a point already in the first fiber.
The complete parabolic bridge suppressed by the published proof.
For a parabolic vertex on axis and any nonempty vertex on other, this produces a common
neighbor on an axis different from both. Thus all interactions involving a parabolic vertex
have graph distance at most two; no admissibility hypothesis is imposed on the other vertex.
The same graph-level bridge for every coordinate omitted by the admissible argument,
including the zero-coordinate lines that also occur when -1 is a square.
For primes congruent to one modulo four, every parabolic incidence vertex has a common neighbor with every nonempty incidence vertex, uniformly over all coordinate axes.
At primes congruent to one modulo four, the zero and parabolic fibers omitted by the admissible incidence argument all have distance at most two from every nonempty fiber.
A full-surface fiber bridge. This does not yet remove the normalized origin from intersection witnesses, so it is intentionally not called the punctured incidence graph.
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The complete incidence bridge for sufficiently large primes congruent to one modulo four. The proof combines the transported admissible bridge with the separately proved zero and parabolic line geometry.