Waves, Particles, and Facts

Vladislav Konovalov

The problems solving of a quantum mechanics is obtained by a classic way or with the help of a corpuscular quantum mechanics In this chapter we shall analyze fundamentals of a modern quantum mechanics. It as a matter of fact not corpuscular and wave. Will be shown, that though it and operates with mass and energy of a particle, as a matter of fact properties of particles in it are skipped in a favour to wave properties. In this case it is easy to receive quantum system conditions, stands only legally or clandestinely to present a particle as a standing wave. Thus find explanation some experimental facts which are not explained by classic mechanics. Simultaneously there are outcomes, not having physical sense. For example, any bound particle in a wave quantum mechanics appears disjointed on separate slices and spread on space, since a particle is not present there, where the wave function is peer to zero point (in nodes of a standing wave) and is spread in space, where the wave function is different from zero point (in antinodes of a standing wave). Particle, bound with a standing wave, too is immobile, though can be in a force field and should move. But then the standing wave is

S. M. Blinder

Mugur B. Răuţ

In this paper I propose an explanation of the double slit experiment results, considered in a general form, in terms of the Doppler effect, as a consequence of applying the principle of complementarity. It is shown that, if we accept the fact that both particle and wave are manifestations of the same conceptual whole, in the general form of the particle-wave dualism, then the Doppler effect will be a manifestation for both wave and particle, and the double slit experiment will be a qualitative illustration of this fact.

Roger G. Newton

Roderich Tumulka

Yuri A. Rylov

It is shown that the wave function describes the state of the statistical ensemble E[S] of individual particles, or the statistical average particle . This result follows from the fact that in the classical limit h=0 the Schroedinger equation turns to the dynamic equations for the statistical ensemble of classical particles. The statement that the wave function describes the state of an individual particle is incompatible with the quantum mechanics formalism. It is shown that the statistical interpretation of quantum mechanics is a corollary of the fact, that the QM formalism is the technique of the statistical ensemble description, restricted by constraints of the dynamic equation linearity.