AWAKENResearch Paper

Academic Research Paper

The Hidden
Intersections

How point-free topology reveals that the Banach-Tarski pieces were never truly disjoint — and the paradox dissolves.

~30 pages|Full ZFC|2025
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The Problem

The Banach-Tarski Paradox

A theorem so counterintuitive it earned the name “paradox” despite being a rigorous proof.

What the Theorem Says

A solid ball B³ can be decomposed into a finite number of pieces (five suffice) and reassembled using only rigid motions (rotations and translations) into two solid balls, each identical to the original.

  • 1Take a solid ball in ℜ³
  • 2Cut it into 5 disjoint pieces (as point-sets)
  • 3Rotate and translate the pieces (no stretching)
  • 4Obtain two complete copies of the original ball

Proved by Banach & Tarski (1924). Requires the Axiom of Choice.

Why It's Called a Paradox

Rigid motions preserve volume. One ball has volume V. Two balls have volume 2V. Something has gone terribly wrong:

  • “Volume was created from nothing”
  • “Conservation of measure is violated”
  • “Physical reality can't work this way”
  • “Mathematics must be broken somewhere”

But what if the pieces aren't really disjoint?

Three Options

The Standard Responses

For a century, mathematicians have offered three ways to live with the paradox.

Accept It

The pieces are non-measurable — volume is simply undefined for them. No contradiction because there's nothing to conserve.

Technically correct, but unsatisfying

Reject the Axiom of Choice

Work in the Solovay model where all sets are measurable. But this costs Hahn-Banach, Tychonoff, and much of functional analysis.

Too expensive — cures the disease by killing the patient

Fix the Definition of 'Part'

Replace point-set topology with locale theory, where 'part of a space' means something richer than 'subset of points.' The pieces overlap.

Our approach — works in full ZFC

Key Insight

Two sets can share no points and still overlap as parts of a space

In locale theory, “part of a space” means something richer than “subset of points.” A sublocale captures how a part sits within the ambient topology. Two sublocales can be point-disjoint yet topologically intertwined.

A Concrete Example

Consider the rational numbers ℚ and the irrationals ℝ \ ℚ inside the real line.

As point-sets:

Completely disjoint. ℚ ∩ (ℝ \ ℚ) = ∅. Not a single point in common.

As sublocales:

Both are dense. Their meet contains S&sub0; (the regular opens). They share the entire topological skeleton of ℝ.

The real line ℝ
ℚ (dense)
ℝ\ℚ (dense)

The Banach-Tarski pieces are exactly like this: point-disjoint but everywhere dense, filling every neighborhood of B³. As sublocales, they necessarily overlap.

The Argument

Five Steps to Dissolution

Each step is independently verifiable. Together, they form a complete resolution of the Banach-Tarski paradox within full ZFC.

Step 1

The Pieces Are Dense

Every Banach-Tarski piece meets every open ball in B³. The pieces are everywhere dense — they thread through the entire sphere.

Step 2

Dense Subsets Become Dense Sublocales

The canonical embedding from subsets to sublocales preserves density. A dense subset of ℝⁿ maps to a dense sublocale.

Step 3

Dense Sublocales Always Overlap

Isbell’s density theorem: the meet of any family of dense sublocales is dense. Dense sublocales cannot be disjoint.

Step 4

The Overlap Has Full Measure

Simpson’s theorem: Lebesgue measure extends to all sublocales via outer measure. The shared sublocale S₀ has μ*(S₀) = μ(B³).

Step 5

The Paradox Is Blocked

Finite additivity requires disjoint pieces. The BT pieces are not disjoint as sublocales. So you cannot add their measures.

The Litmus Test

BT vs. Dougherty-Foreman

The Dougherty-Foreman paradox uses open sets as pieces. Open sets are complemented in the locale — genuinely disjoint as sublocales. The locale framework correctly distinguishes the two cases.

Pieces are...

BT

Non-measurable, everywhere dense

DF

Open sets (Borel measurable)

Disjoint as sets?

BT

Yes

DF

Yes

Disjoint as sublocales?

BT

No — dense sublocales always overlap

DF

Yes — open sets are complemented in the frame

Uses Axiom of Choice?

BT

Yes (non-constructive pieces)

DF

No (explicit construction)

Paradox in locale framework?

BT

No — additivity is blocked by overlap

DF

Yes — genuinely disjoint, genuinely paradoxical

The locale framework doesn't blindly dissolve all paradoxes — it makes precise distinctions. BT is blocked because its pieces overlap as sublocales. DF goes through because its pieces are genuinely disjoint.

The Framework

Why Locales Are the Right Setting

Locale theory isn't an ad hoc fix for one paradox. It's an independently motivated framework that resolves BT as a side effect.

Tychonoff Without Choice

In locale theory, the Tychonoff theorem holds without the Axiom of Choice. Products of compact locales are compact — no selection axiom needed.

Constructive Mathematics

Locales are the natural framework for topology in constructive and predicative mathematics. Results that require AC classically often become constructive in locale theory.

Physical Space

Physical space has no dimensionless, sizeless points. Locales model space via its observable structure — the open sets — without requiring a substrate of points.

The Paper

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Selected References

2012

Simpson, A.

Measure, randomness and sublocales

APAL 163(11), 1642–1659

2012

Picado, J. & Pultr, A.

Frames and Locales: Topology without Points

Birkhäuser

1995

Leroy, J.

Un théorème de Banach-Tarski dans le cadre localique

arXiv:1303.5631

2025

Lehner, T.

Measure theory via locales

arXiv:2510.08826

1972

Isbell, J.

Atomless parts of spaces

Math. Scand. 31, 5–32

1993

Wagon, S.

The Banach-Tarski Paradox

Cambridge University Press

1994

Dougherty, R. & Foreman, M.

Banach-Tarski decompositions using sets with the property of Baire

JAMS 7(1), 75–124

1982

Johnstone, P.T.

Stone Spaces

Cambridge University Press

Read the Full Paper

The Hidden Intersections: A Locale-Theoretic Resolution of the Banach-Tarski Paradox

~30 pages covering density, sublocales, Isbell's theorem, Simpson's measure extension, and the complete resolution — all within full ZFC.

“The Banach-Tarski pieces are not disjoint parts of the sphere. They are dense, overlapping aspects of it — and the paradox was always an artifact of confusing points with parts.”

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