George P. Shpenkov

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 The First Discovery of the 21st century : Two phenomena - "Relict" background radiation and the Lamb "shifts" - have the same source! (click lamb.asp)

Curriculum Vita

Brief Biography

Discovery & Inventions

Selected Publications
Memorandum RPhS


Dialectical Physics

Dialectical View
Early Papers
Periodic Table
Table of Isotopes
Isotopes of Carbon
Isotopes of Helium


Physical Metric

Table of Objective Dimensionalities
The Physical Metric


Atomic Structure

Anisotropy of Graphene
Carbon and Oxygen
Graphene Nanoribbons
Orbitals (Eng)
Orbitals (Rus)
Electron Spin (Rus)
Electron Spin (Eng)
Virtual Particles (Rus)
Virtual Particles (Eng)
Atomic Nucleus (Rus)
Atomic Nucleus (Eng)
Nature of Gravity (Rus)
Nature of Gravity (Eng)
Planetary Orbits (Rus)
Planetary Orbits (Eng)
Cosmic Background (Rus)
Cosmic Background (Eng)
Neutron Moments (Rus)
Neutron Moments (Eng)
Proton Moments (Rus)
Proton Moments (Eng)
Fundamental Period (Rus)
Fundamental Period (Eng)
Decimal Code (Rus)
Decimal Code (Eng)
Wave Model (Rus)
Wave Model (Eng)



EGF2016, Paris-France
23DGK-2015 Göttingen
ICNAAM-2012 Kos
GR19-2010 Mexico



Family and myself






The majority is fully convinced of that the hydrogen atom is quite well described by Schrödinger's wave function. But throughout an existence of quantum mechanics (QM), the

Three-dimensional distribution of extremes of Schrödinger's
Y-functions has never been presented.
Why so?

Let us turn to the example. Following QM, the density of probability of the presence of a single electron in the hydrogen atom, at every point and at every instant, is proportional to . Therefore, at l = 1 and m = 0, extremes of are in two polar points s1 and s2, i.e., on the extreme radial sphere determined by the solutions of the radial equation for the radial function R1(r).

The surface (a) and corresponding to it two polar extremes s1 and s2 (b) of on the radial sphere R1(r); p is the proton.

Obviously, transitions of the electron between two points, s1 and s2, separated by the equatorial plane of the zero probability, are impossible. We arrive at the fact that with the equal probability the electron can be either in s1 or s2. It means that the electron (being in the state determined by the quantum numbers l = 1 and m = 0) "hangs" above the "north" or "south" poles of the proton surface, forming together with the proton an electric dipole directed along the polar z-axis, and its orbital (magnetic and mechanical) moments are equal to zero.

Obviously, such a structure of the hydrogen atom,
originated from the QM interpretation, is inconsistent with experiment.
The similar inconsistency is inherent in all other functions with different quantum numbers l and m.





2.73 K Background
h and a Constants
Electron Spin
> Lamb shift
DM as against SM
Neutron Magnetic Moment
Proton Magnetic Moment
Avogadro Constant
Ampere's Law
Hall Effect
Cosmological Redshift
Imaginary Unit


Related Links

Mass-Charge Nature
Binumbers of Dialectics
Fundamental Period
Algebra of Dialectics
Coulomb's Law
Waves and Current



Lecture, Wroslaw-2013
On the Higgs boson
Lecture in WAT
Warsaw, 20.10.06
Gravitational Waves
Strong Interactions
Letter to Karshenboim



Dynamic Model
Electric constant e0


Lectures on
Dialectical Physics

Volume 1
Volume 2
Volume 3
Volume 4
Volume 5
Volume 6



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2002-2015 George Shpenkov

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