2007
DOI: 10.1139/p07-121
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De Broglie waves as an effect of clock desynchronization

Abstract: De Broglie waves are a simple consequence of special relativity applied to the complex-phase oscillations of stationary states. As de Broglie showed in his doctoral thesis, the synchronized oscillations of an extended system at rest, even a classical one, become de Broglie-like waves when boosted to finite velocity. The waves illustrate the well-known but seldom demonstrated relativistic effect of clock desynchroniation (or dephasing) in moving frames. Although common manifestations of stationary-state oscilla… Show more

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Cited by 24 publications
(24 citation statements)
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“…A spatial distribution with a synchronized phase oscillation in its rest frame becomes a de Broglie wave in the lab after a boost by the eigenspinor Λ. [35] Re-expressing the proper time as the Lorentz invariant τ = xū 0 S , we find the phase factor in terms of lab coordinates…”
Section: De Broglie Waves and Spin Interactionmentioning
confidence: 90%
“…A spatial distribution with a synchronized phase oscillation in its rest frame becomes a de Broglie wave in the lab after a boost by the eigenspinor Λ. [35] Re-expressing the proper time as the Lorentz invariant τ = xū 0 S , we find the phase factor in terms of lab coordinates…”
Section: De Broglie Waves and Spin Interactionmentioning
confidence: 90%
“…Equation 25is a generalized Davies-Unruh temperature and is perspectival. The de Broglie matter-waves are fundamentally relativistic entities [26,27], and the two velocities u ω , v ω represent the inclination of the space-and time axis, respectively. If we chose a massless (no rest-mass) wave, we are in the invariant situation, where v ω = u ω = c and Equation 25turns into the well known Davies-Unruh formula:…”
Section: Minkowski Spacementioning
confidence: 99%
“…Although this is a correct description of the time dilation effect on frequency, it does not correctly account for the phase of the zitter motion of the non-stationary test particle as observed in the laboratory frame. The latter is properly [12] determined by Lorentz transformation as ωτ = γω(t − υ · x/c 2 ), where τ is the time coordinate in the test zitter particle rest frame, and x is the test zitter particle position. The present version (v13) of this article is corrected accordingly beginning at Eq.…”
Section: Erratamentioning
confidence: 99%