dorsal/arxiv
View SchemaQuantum interference and particle trajectories
| Authors | J. Luscombe |
|---|---|
| Categories | |
| ArXiv ID | physics/9706011 |
| URL | https://arxiv.org/abs/physics/9706011 |
Abstract
The existence of precise particle trajectories in any quantum state is accounted for in a consistent way by allowing delocalization of the particle charge. The relativistic mass of the particle remains within a small volume surrounding a singularity moving along the particle trajectory. The singularity is the source of an electric displacement field. The field induces a polarization charge in the vacuum and this charge is equated with the charge of the particle. Under dynamic conditions a distributed charge density rho(x,t) is induced in the vacuum. The volume integral of the charge density is equal to the charge of the particle and is rigorously conserved. The charge density is derived from a complex-valued physical field psi(x,t) such that rho(x,t) = |psi(x,t)|^2. The position probability density is equated with the mean charge density. The mean field psi(x,t) for many sample realizations with a given energy E and potential V(x) is the sum of the individual fields. In order for the sum to be non-zero, the components in the spectral decompositions of the individual fields must be spatially coherent. The particle has a spin frequency given by Planck's relation hv = T - V + mc^2, where T is the kinetic energy, determined from the momentum p and V is a quantum potential such that E = T + V is conserved. The instantaneous phase of the spin is given by the phase of exp(ikx) in the spectral decomposition a(k) of psi(x,t). It is spatially coherent, due to the dependence on x. The momentum probability distribution is given by the squared magnitude of the coefficients a(k). The Schrodinger equation is derived by requiring local conservation of mean energy.
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"abstract": "The existence of precise particle trajectories in any quantum state is\naccounted for in a consistent way by allowing delocalization of the particle\ncharge. The relativistic mass of the particle remains within a small volume\nsurrounding a singularity moving along the particle trajectory. The singularity\nis the source of an electric displacement field. The field induces a\npolarization charge in the vacuum and this charge is equated with the charge of\nthe particle. Under dynamic conditions a distributed charge density rho(x,t) is\ninduced in the vacuum. The volume integral of the charge density is equal to\nthe charge of the particle and is rigorously conserved. The charge density is\nderived from a complex-valued physical field psi(x,t) such that rho(x,t) =\n|psi(x,t)|^2. The position probability density is equated with the mean charge\ndensity. The mean field psi(x,t) for many sample realizations with a given\nenergy E and potential V(x) is the sum of the individual fields. In order for\nthe sum to be non-zero, the components in the spectral decompositions of the\nindividual fields must be spatially coherent. The particle has a spin frequency\ngiven by Planck\u0027s relation hv = T - V + mc^2, where T is the kinetic energy,\ndetermined from the momentum p and V is a quantum potential such that E = T + V\nis conserved. The instantaneous phase of the spin is given by the phase of\nexp(ikx) in the spectral decomposition a(k) of psi(x,t). It is spatially\ncoherent, due to the dependence on x. The momentum probability distribution is\ngiven by the squared magnitude of the coefficients a(k). The Schrodinger\nequation is derived by requiring local conservation of mean energy.",
"arxiv_id": "physics/9706011",
"authors": [
"J. Luscombe"
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"title": "Quantum interference and particle trajectories",
"url": "https://arxiv.org/abs/physics/9706011"
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