Vacuum Structure and Dynamics; Particle Formation

ORAL

Abstract

We model the vacuum as filled of neutral vacuuons, each consisting of a p- vaculeon of charge +e at the core and an n- vaculeon of -e on the envelope, mutually bound with a Coulomb energy $\sim 10^6$ J. The model is derived based on overall experimental observations. In particular, as shown in the pair annihilation $e^-+ e^+ \rightarrow \gamma + \gamma $, the two emitted $\gamma$ rays carry the energy ($2 M_e c^2=1022$ keV) converted from the mass $2M_{e^-} $ of $e^-$ and $e^+$ only, whilst the Coulomb potential energy $V = -\frac{e^2}{4 \pi \epsilon_0 r_0}$ between their charges $+ e$ and $-e$ separated at $r_0$, are not released. Energy conservation requires $V$ and its certain carriers must remain in the vacuum after the annihilation. The afore-modeled vacuum will be polarized by the static field of an external charge, induced with a shear elasticity, and thereby able to propagate the disturbances of the charge's accelerating movements as transverse elastic waves---whence the electromagnetic waves. We have given a systematic representation of the statics and dynamics of this vacuum based on classical equations of motion and solutions (JXZJ \& P-IJ, {\it Unification of Classical, Quantum and Relativistic Mechanics and the Four Forces}, Fwd Prof R Lundin, Nova Science, NY, 2005). The solutions in particular yield a basic material particle, like an electron, proton, etc, formed of a massless oscillatory charge and its resulting electromagnetic waves in the vacuum, having the overall observational properties of the basic material particles.

Authors

  • J.X. Zheng-Johansson

    IOFPR, SWE

  • P.-I. Johansson

    Uppsala Univ, SWE