The quantum theory of dual charged particles

1974 ◽  
Vol 9 (16) ◽  
pp. 641-644
Author(s):  
V. I. Strazhev
Keyword(s):  
Quantum Theory ◽  
Charged Particles

Quantum theory of the radiative interaction of charged particles

1990 ◽  
Vol 23 (23) ◽  
pp. 5547-5553 ◽  
Author(s):  
S T Zavtrak ◽  
L I Komarov
Keyword(s):  
Quantum Theory ◽  
Charged Particles ◽  
Radiative Interaction

scholarly journals On the new field theory II─Quantum theory of field and charges

1937 ◽  
Vol 159 (898) ◽  
pp. 355-382 ◽  
Keyword(s):  
Field Theory ◽  
Electromagnetic Field ◽  
Quantum Theory ◽  
Quantum Electrodynamics ◽  
Present Author ◽  
Charged Particles ◽  
Quantum Mechanical ◽  
Mechanical Theory ◽  
Quantum Mechanical Theory ◽  
Quantum Treatment

The Purpose of this paper is to extend the quantum electrodynamics of the New Field theory to include the dynamics of charged particles. The work of Born and Infeld (Born 1934; Born and Infeld 1934 a , b , 1935) in which the theory has been developed, and of weiss (1936), has dealt with the quantum theory of the electromagnetic field alone, without allowing for the occurrence of point charges; this is inherent in their equation div D = 0. In a Previous paper (1936 a ), the present author has given a classical (i. e. non-quantum) treatment of the dynamics of point charges in the frame of the New Field theory. The analytical methods of that paper were chosen in such a way that they could be used in the generalization to a quantum-mechanical theory, and we shall here use them as the scaffolding for the present work. We shall therefore use the same notation as before. The more important symbols have the following meanings:

scholarly journals Telepathic Communication

2018 ◽  
Vol 1 (2) ◽  
pp. p42
Author(s):  
Mohammed Ziad Kebbe
Keyword(s):  
Quantum Theory ◽  
Human Brain ◽  
Nerve Cell ◽  
Charged Particles ◽  
Niels Bohr ◽  
Comparative Approach ◽  
A Posteriori ◽  
Scientific Opinion ◽  
Electrically Charged ◽  
Complex Question

In this multidisciplinary paper I will argue that speech module is but the tip of the ice berg of language whereas other language modules – such as thought – are still concealed in the dark recesses of the human brain. Considering several paths of possibilities that come to mind, I intend to address the question of whether language is really particles or waves. In essaying to answer such inextricably complex question, I will shun exegetical polemics and draw on an equally complex theory: the quantum theory as advanced by Niels Bohr (1913) whose views have recently been much absorbed by scientific opinion. My aim is to instantiate a posteriori that language is essentially a form of energy – electrically charged particles (which I will call thotons) generated when electrons leap downward from one fixed orbit to another within the nerve cell. Adopting a deductive comparative approach, I will argue that since electrons entangle each other even if they are in discrete locations, the thotons – here defined as the linguistic bits –are, by the same token, not tied down to any particular location; instead they could be anywhere and nowhere in the nerve cells of two or more minds even if they were on different sides of the globe.

scholarly journals The solution of the wave equation for the scattering of particles by a coulombian centre of force

1928 ◽  
Vol 118 (780) ◽  
pp. 542-549 ◽  
Keyword(s):  
Wave Equation ◽  
Quantum Theory ◽  
General Problem ◽  
Charged Particles ◽  
Successive Approximations ◽  
Method Of Successive Approximations ◽  
Theory Result

The problem of the scattering of a stream of charged particles by a Coulombian centre of force has been treated by Wentzel and by Oppenheimer, who use Born’s method of successive approximations. They have shown that, if ZZ' ε 2 / hv is small, the quantum theory gives the well-known Rutherford formula. Furthermore, if ZZ' ε 2 / hv is large, we know that the quantum theory result must tend towards the classical, and it seemed probable that the two theories would agree for intermediate values of this constant. In this paper we shall show that this is actually the case. We shall first consider the more general problem of scattering by a field V( r ). The wave equation is ∇ 2 ϕ +2 m / h 2 (E - V) ϕ = 0. (1)

Spectral method in quantum theory of channeling phenomena of fast charged particles in crystals

2010 ◽  
Vol 374 (46) ◽  
pp. 4690-4694 ◽  
Author(s):  
A.V. Kozlov ◽  
N.F. Shul'ga ◽  
V.A. Cherkaskiy
Keyword(s):  
Quantum Theory ◽  
Spectral Method ◽  
Charged Particles
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