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One Postulate
Emad Mostaque · 2026

Appendix — Historical Record

The Long Road to One Postulate

Einstein's 1905 paper depended on two postulates. Physicists noticed almost immediately that this felt unsatisfying. The attempt to prove the second from the first — or to derive relativity from one postulate alone — has a 138-year history. Until now, one crucial piece was always missing.

10

Key Events

138

Years of effort

1888

When the tool arrived

1888

Wilhelm Killing — The Killing Form

Discovers a diagnostic tool for Lie algebras that, 138 years later, will prove which universe we live in. Killing publishes "Die Zusammensetzung der stetigen endlichen Transformationsgruppen" — introducing the bilinear form that bears his name.

1895

Lorentz — Transformation Equations

Derives the transformation equations that will eventually bear his name. Gets the mathematics exactly right — but attributes the results to a physical compression of matter moving through an invisible medium called the luminiferous ether.

1904

Poincaré — The Group Structure

Recognises that the Lorentz transformations form a group — a deep mathematical insight. Coins the term "Lorentz group." Einstein will build on this foundation the following year, but the algebraic depth of the group structure will take a century more to fully exploit.

1905

Einstein — Special Relativity (Two Postulates)

Publishes "On the Electrodynamics of Moving Bodies." Two postulates, one revolution. Postulate I: the laws of physics are the same in all inertial frames. Postulate II: the speed of light in vacuum is the same in all inertial frames. But why two?

1910

Ignatowski — Relativity from One Postulate

First to show that the Lorentz transformations can be derived without explicitly assuming the constancy of c. Derives the general transformation group from symmetry alone, parameterised by a constant κ. Leaves κ undetermined — neither its sign nor its value can be fixed from the algebra alone. A crucial step forward with one piece missing.

1921The Unsolved Problem

Pauli — "Nothing Can Be Said About the Sign of κ"

In his landmark encyclopaedia article on relativity, Pauli correctly identifies that the sign of κ cannot be determined from symmetry arguments alone — or so he believes. Accepts this as a fundamental limitation of the one-postulate approach. The gap becomes the received wisdom of the field.

1964

Lévy-Leblond — Revisiting One-Postulate Relativity

Rederives the Lorentz transformations from one postulate in a more rigorous and pedagogically clear way. Confirms the existence of the three-case family (κ < 0, κ = 0, κ > 0). Still cannot fix the sign of κ from purely algebraic arguments. The gap identified by Pauli stands.

2008

Silagadze — "Relativity Without Tears"

A comprehensive pedagogical paper revisiting the one-postulate derivation and making the argument accessible to a wider audience. Reviews the full family of transformation groups. Still κ is left undetermined — the gap persists. The paper's title is prescient: tears are still needed, until the Killing form is applied.

2015The Unsolved Problem

Drory — "The Necessity of the Second Postulate"

Argues — incorrectly, as the 2026 paper shows — that the second postulate is genuinely necessary and cannot be derived from the first. Takes Pauli's limitation as definitive. The argument is rigorous but misses the one tool that can resolve the sign: the Killing form of the resulting Lie algebra.

2026The Solution

Mostaque — One Postulate

The Killing form — Killing's 1888 diagnostic — settles the sign. B(boosts) = 4κ must be positive for the algebra to be non-degenerate and consistent with the Lorentz group structure. κ > 0 is the only algebraically consistent possibility. Pauli's gap is closed. The second postulate was always redundant.

"
One may show that the sign of κ cannot be determined from these considerations.
Wolfgang Pauli, 1921 — Theory of Relativity (encyclopaedia article)

Pauli identified precisely the gap this paper closes. The sign of κ determines whether relativity is Lorentzian (κ > 0), Galilean (κ = 0), or physically inconsistent (κ < 0). For 105 years, Pauli's assessment stood as received wisdom. The Killing form changes everything — B(boosts) = 4κ must be positive for the algebra to be non-degenerate.

The Missing Piece — Applied 2026

The Killing Form

B(X, Y) = Tr(ad X ∘ ad Y)

Killing's 1888 diagnostic for Lie algebras

Applied to Boosts

B(boosts) = 4κ

Calculated directly from the symmetry algebra

Non-Degeneracy Condition

κ ≠ 0, κ > 0

Lorentzian structure requires positive κ

The Killing form was available since 1888. The one-postulate programme began in 1910. For 116 years, the tool and the problem existed in the same mathematical literature — and were never connected. This paper makes that connection.

From 1888 to 2026 — 138 years from Killing's discovery to its application.

The tool was always there. The question was always there. Now we have the answer.

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