Relativity and Aether Theory: A Crucial Distinction
| Scientific Paper | |
|---|---|
| Title | Relativity and Aether Theory: A Crucial Distinction |
| Read in full | Link to paper |
| Author(s) | Joseph Levy |
| Keywords | Relativity, Aether |
| Published | 2006 |
| No. of pages | 13 |
Read the full paper here
Abstract
We study the case of two rockets which meet at a point O of an 'inertial co-ordinate system' S, and are scheduled to move at constant speed, in opposite directions, toward two targets placed at equal distances from point O. At the instant they meet, the clocks inside the rockets are set to zero. When they reach the targets the rockets meet two clocks A and B whose reading is identical. This question which was tackled in ref [1] is studied here in depth. Assuming the existence of a preferred aether frame in which the one-way speed of light is isotropic, and the anisotropy of this speed in the other frames, we show that, if the equal reading of the clocks A and B results from an exact synchronization, the clocks inside the rockets will display different readings when they reach A and B in contradiction with the relativity principle. Conversely, if the clocks A and B, which display an equal reading, have been synchronized by means of the Einstein-Poincaré procedure, the inboard clocks will also display the same reading, a fact which seems in agreement with the relativity principle. But this synchronization method presupposes the invariance of the one-way speed of light, in contradiction with the assumptions made, and, therefore, introduces a measurement error. This demonstrates that if we assume the existence of an aether frame, the apparent relativity principle is not a fundamental principle; it depends on an arbitrary synchronization. In any case, this is an example of an experimental measurement which can be explained by aether theory without the assumption of the invariance of the one-way speed of light in all 'inertial frames'.
Overview
Joseph Levy's paper — also posted as arXiv physics/0610067 and here in a version "supplemented by additional information and other references" — addresses one question: is a preferred aether frame compatible with the relativity principle? He notes that physicists have divided on this. Einstein initially regarded the aether as superfluous and later, in the 1920 Leiden address Sidelights on Relativity, readmitted an aether "not thought of as endowed with the quality of ponderable media", explicitly denying it a state of motion. Henri Poincaré, by contrast, accepted the Lorentz picture — a genuine preferred frame in which contraction and clock retardation are real, velocity-dependent processes — while at the same time calling the impossibility of detecting the earth's absolute motion "a general law of nature" that we should "admit without restriction".
Levy's device for testing this is a symmetric two-rocket thought experiment, and his answer is a distinction rather than a refutation. The relativity principle, he argues, holds for apparent speeds and times — the ones we actually measure with light-synchronized clocks and contracted rulers — and fails for real ones. It is therefore not a fundamental postulate but an artefact of an arbitrary synchronization convention. Crucially, he does not claim the experiment would come out differently from special relativity's prediction. It comes out the same; his claim is that the identical result has a different cause.
The argument
The two-rocket experiment
Two rockets meet at a point O of an inertial coordinate system S and move at constant speed in opposite directions toward points A and B, equidistant from O along the x-axis. Their inboard clocks are set to zero at O; clocks stationed at A and B read identically when the rockets arrive. There is no acceleration or deceleration anywhere in the process, which removes the usual escape route of the twin paradox.
Special relativity's prediction is straightforward: the light speed is isotropic in every inertial frame, so exact synchronization of the A and B clocks is unproblematic, their equal reading is the real time, and by symmetry the inboard clocks read that value divided by γ. Levy's frame S is assumed to move at speed v relative to the aether frame S0; he uses the Lorentz expressions C − v and C + v for the real one-way light speed along and against that motion — "the expressions used by Lorentz to explain the Michelson experiment" — and takes half the rest length of AB to be l, contracted to l√(1 − v²/C²) when measured with an uncontracted standard.
Case 1: exact synchronization
If the clocks at A and B are truly synchronized with the clock at O, so that their common reading is the real time, the conclusion is immediate. The two rockets do not have the same speed relative to the aether frame, so their clocks are retarded by different amounts and will read differently on arrival. Only if S happened to be at rest in S0 would the readings agree — and that outcome would itself tell us whether S is moving relative to the aether. So with exactly determined speeds, Levy concludes, "Poincaré's relativity principle is shown to be at variance with the existence of a preferred aether frame."
Case 2: Einstein-Poincaré synchronization
The second case is the substantive one. Under the Einstein–Poincaré convention a signal is sent from O to B and reflected back, and clock B is called synchronous if it reads T/2 at reflection. Since the one-way speed is not isotropic in S, this introduces a systematic error. Levy computes the real transit time from O to B as l√(1 − v²/C²)/(C − v), and the apparent time actually recorded, after allowing for clock retardation, as l√(1 − v²/C²)/C. The difference is a synchronism discrepancy Δ = lv/C², with the apparent time shorter than the real time at B. Repeating for A gives −Δ, the apparent time there being longer. Levy stresses that, contrary to special relativity, aether theory does not regard l/C as the real light transit time from O to B.
The corrected readings are then τ + Δ at B and τ − Δ at A, and the real transit times in the aether frame become t0B = (τ + lv/C²)/√(1 − v²/C²) and t0A = (τ − lv/C²)/√(1 − v²/C²). Levy points out that these "assume the same mathematical form as the conventional transformations", but insists the interpretation differs: τ and l are not the real coordinates, having been obtained with E–P synchronized clocks and contracted rulers.
The inboard clocks agree anyway
Because the apparent transit times in S are equal by construction, the apparent speeds are vapp = l/τ on both sides, but these correspond to two different real speeds v′ and v″ and two different real times. Levy computes the inboard readings TB and TA, substitutes the real speeds, and finds (with the algebra given in Appendix 1) that both reduce to the same expression
TA = TB = √(τ² − l²/C²)
The dependence on v — on the motion of S through the aether — cancels exactly. For l/τ ≪ C this is approximately τ(1 − ½vapp²/C²). Levy remarks that this "highlights the equivalence of the slow clock transport synchronization procedure and the Einstein-Poincaré method, and provides a key to understand the GPS measurements".
Velocity composition as a measurement artefact
Appendix 2 makes the same move for velocity addition. In the underlying aether theory, real speeds are "simply additive": VB = v + v′ and VA = v − v″, a Galilean law. Computing the apparent speed from the E–P-synchronized clocks and the contracted standard, Levy obtains vapp = (VB − v)/(1 − VBv/C²) — the relativistic composition law. His conclusion is that the relativistic law "applies to apparent speeds and not to the real speeds which as we saw are simply additive".
Assessment
The paper is a clean and honest piece of work within the Lorentzian tradition, and its central calculation is correct. It is worth being precise about what it establishes. Levy does not claim any observational disagreement with special relativity; on the contrary, the whole force of Case 2 is that the aether-frame velocity v cancels from the observable result. What he demonstrates is the conventionality of distant simultaneity — that an anisotropic one-way light speed plus a compensating synchronization error reproduces the isotropic predictions exactly. This is a real and well-established result, familiar from the Reichenbach ε-synchronization literature and from Mansouri–Sexl test theory, and Levy derives it independently and transparently. The demonstration that relativistic velocity composition emerges from Galilean addition once measurement distortions are applied is the paper's most elegant passage, and the observation that slow clock transport and Einstein–Poincaré synchronization agree to the order computed is correct and useful.
The philosophical conclusion, however, is stronger than the mathematics licenses. Levy writes that the relativity principle "depends on arbitrary synchronization procedures" and is therefore not fundamental. But his own result shows the opposite symmetry: the observable outcome is independent of v, so no measurement in the experiment can distinguish his aether theory from special relativity. If two theories agree on every observable, the choice between them is not settled by the experiment, and calling one "real" and the other "apparent" is a metaphysical preference, not a finding. The preferred frame does no work here — it enters the calculation and exits it again — and a critic is entitled to apply Occam's razor at exactly that point. Levy does not engage this objection.
Two more specific weaknesses. Case 1 is not an alternative to Case 2 but a counterfactual: it presupposes access to an "exact synchronization" defined with respect to the aether frame, which requires already knowing v. Levy is aware of this and suggests in a footnote that astronomical estimates of the earth's absolute speed may soon permit near-exact synchronization; but until such a determination exists and is independently confirmed, Case 1 assumes precisely what the theory needs to establish. Second, the footnote on Hafele–Keating leans on critiques by Kelly and Essen and cites Van Flandern on GPS to suggest the relativity principle is in trouble, but this is dropped rather than argued, and the paper's own result does not support it — Levy's own analysis reproduces the standard prediction. The GPS remark in the conclusion likewise gestures at a "key" that is not supplied.
Read as what it is — a careful demonstration that a Lorentzian aether theory with real contraction, real clock retardation and anisotropic one-way light speed is observationally equivalent to special relativity in a symmetric transit experiment — the paper is sound on its own terms. Read as a demonstration that the relativity principle is not fundamental, it proves the equivalence rather than the deficiency.