A non-local, Lorentz-invariant, hidden-variable interpretation of relativistic quantum mechanics based on particle trajectories
arXiv:quant-ph/0110007 · doi:10.1088/0305-4470/34/46/310
Abstract
We demonstrate how to construct a lorentz-invariant, hidden-variable interpretation of relativistic quantum mechanics based on particle trajectories. The covariant theory that we propose employs a multi-time formalism and a lorentz-invariant rule for the coordination of the space-time points on the individual particle trajectories. In this way we show that there is no contradiction between nonlocality and lorentz invariance in quantum mechanics. The approach is illustrated for relativistic bosons, using a simple model to discuss the individual non-locally correlated particle motion which ensues when the wavefunction is entangled. A simple example of measurement is described.
12 pages, 2 figures
References in corpus (2)
Cited by in corpus (11)
- A Relativistic Version of the Ghirardi-Rimini-Weber Model
- Can Bohmian mechanics be made relativistic?
- Applied Bohmian Mechanics
- The "Unromantic Pictures" of Quantum Theory
- On the uniqueness of paths for spin-0 and spin-1 quantum mechanics
- A relativistically covariant version of Bohm's quantum field theory for the scalar field
- Relativistically invariant extension of the de Broglie-Bohm theory of quantum mechanics
- Lorentz-invariant, retrocausal, and deterministic hidden variables
- The effect of time-dilation on Bell experiments in the retrocausal Brans model
- Consequences of a Two-Time Relativistic Bohmian Model
- On substantive Lorentz invariance and quantum theory