Paper XII visual guide · Visual 16 of 27 · TWO DIFFERENT COMPACTNESS MECHANISMS

Finite dimension prevents tail escape

Main text: Theorem 8.7, Corollary 8.8 and Example 8.13 Main statement 8.7

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Original plate in the visual-guide PDF · Original atlas source

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Nested nonzero subspaces inside one fixed finite-dimensional space behave differently from nested tails inside an infinite-dimensional space.

Fixed carrier \(k^5\)

A descending chain stabilizes in five dimensions
Original drawing. Read the description below; expand the labels and data for selectable text.

Reading the drawing

Six rows display nested spans of five fixed basis vectors. The rightmost direction disappears successively until only the first remains. The finite-dimensional chain has a nonzero stable intersection in this example.

Drawing labels and data 11 labels

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  • \(m=1\)
  • \(m=2\)
  • \(m=3\)
  • \(m=4\)
  • \(m=5\)
  • \(m=6\)
  • \(e_1\)
  • \(e_2\)
  • \(e_3\)
  • \(e_4\)
  • \(e_5\)

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Evidence note from the source edition

The projectors retain initial basis directions with dimensions \(5,4,4,2,1,1,\ldots\). In this explicitly defined example the projector is constant from level five onward.

Infinite carrier \(\ell^2(\mathbb N)\)

A descending tail escapes in infinite dimension
Original drawing. Read the description below; expand the labels and data for selectable text.

Reading the drawing

Each row retains all basis vectors from its index onward. Dots at the right indicate the infinite tail. Every displayed row is nonzero, yet no fixed basis direction survives every row.

Drawing labels and data 20 labels

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  • \(m=1\)
  • \(\cdots\)
  • \(m=2\)
  • \(\cdots\)
  • \(m=3\)
  • \(\cdots\)
  • \(m=4\)
  • \(\cdots\)
  • \(m=5\)
  • \(\cdots\)
  • \(m=6\)
  • \(\cdots\)
  • \(e_1\)
  • \(e_2\)
  • \(e_3\)
  • \(e_4\)
  • \(e_5\)
  • \(e_6\)
  • \(e_7\)
  • \(e_8\)

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Evidence note from the source edition

Row \(m\) retains all basis vectors \(e_j\) with \(j\ge m\). Every row continues infinitely to the right. The display is a finite window, not a truncation of the actual carrier.

Why the finite chain eventually stops changing

Suppose idempotents satisfy

\[ e_{m+1}e_m=e_me_{m+1}=e_{m+1}. \]

Their ranges are nested. In dimension \(d\), nonzero ranges allow at most \(d-1\) strict dimension drops. There may be long gaps between drops, but only finitely many drops. The chain therefore becomes constant and has nonzero intersection.

Source reading note

A single repeated dimension does not certify final stabilization. The finite example deliberately has a plateau \(4,4\) before another drop. Finite dimension bounds the number of strict drops, not the time of the last one.

Why every infinite tail can be nonzero while their intersection vanishes

Let \(P_m\) project onto the closed span of \(e_m,e_{m+1},\ldots\). Each range is nonzero. But a vector belonging to every range has its \(j\)-th coordinate zero once \(m>j\). Every coordinate is therefore zero:

\[ \bigcap_{m\ge1}P_m\ell^2(\mathbb N)=\{0\}. \]

Read this as

Fixed finite-carrier stabilization, stable images in an inverse system, and infinite Hilbert-space tails are different situations. Their hypotheses cannot be exchanged.

Source and conversion record

The original atlas wording, equations, and drawing labels are retained. Drawings are views of the retained visual-guide PDF. Text descriptions and table headings are added reading aids. This conversion does not rebuild TeX, rerun the examples, audit proofs or compile Lean.

The guide contains 27 plates and 23 drawings: 21 from separate drawing files and two embedded directly in the page source. The unused rotated-support sketch is retained in the source archive. The final claim-delta and evidence pages preserve the distinction between the revised contract and the historical original wording.

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