In a few previous papers, we developed a so-called classical fluctuation model providing (generalized) ''symmetrization rules '' - these make the classical expressions for energy transfer probabilities compliant with the detailed balance principle. For various physical processes, the symmetrized expressions of the transfer probabilities were shown to be remarkably improved - with respect to the performances of standard semiclassical models - in view of approaching quantum-mechanical results. Therefore, the possibility that a still undiscovered classical physics potential to describe quantum effects may be revealed by the model must be investigated. In this and a few next papers, we introduce some conceptual developments of the model and dis...
The classical action: Integral (0,T) dt1 L(v(t1), x(t1),t1) may be varied to find a stationary solu...
In a previous paper, we developed a so-called fluctuation model for the inelastic collisional intera...
Using an analogy with statistical thermodynamics and the Einstein equation for fluctuation probabili...
In a few previous papers, we developed a so-called classical fluctuation model providing (generalize...
In a few previous papers, we developed a so-called classical fluctuation model, which revealed remar...
In a few previous papers, we developed a theoretical framework displaying the thermodynamic, mechani...
In this paper, we join two different theoretical approaches to the problem of finding a classical-li...
This paper is the third one of a series of four. In the previous ones, we developed a thermodynamic ...
In a few previous papers, we discussed the fundamentals of the so-called Bernoulli oscillators physi...
In a few previous papers, we discussed the fundamentals of the so-called Bernoulli oscillators physi...
We revise here the fundamental structure of our oscillators model aimed at removing (some of) the in...
In the previous Part I of this paper, we developed a theoretical model to account for energy and mas...
Based on the Bohr's correspondence principle it is shown that relativistic mechanics and quantum mec...
The classical action: Integral (0,T) dt1 L(v(t1), x(t1),t1) may be varied to find a stationary solu...
In a previous paper, we developed a so-called fluctuation model for the inelastic collisional intera...
Using an analogy with statistical thermodynamics and the Einstein equation for fluctuation probabili...
In a few previous papers, we developed a so-called classical fluctuation model providing (generalize...
In a few previous papers, we developed a so-called classical fluctuation model, which revealed remar...
In a few previous papers, we developed a theoretical framework displaying the thermodynamic, mechani...
In this paper, we join two different theoretical approaches to the problem of finding a classical-li...
This paper is the third one of a series of four. In the previous ones, we developed a thermodynamic ...
In a few previous papers, we discussed the fundamentals of the so-called Bernoulli oscillators physi...
In a few previous papers, we discussed the fundamentals of the so-called Bernoulli oscillators physi...
We revise here the fundamental structure of our oscillators model aimed at removing (some of) the in...
In the previous Part I of this paper, we developed a theoretical model to account for energy and mas...
Based on the Bohr's correspondence principle it is shown that relativistic mechanics and quantum mec...
The classical action: Integral (0,T) dt1 L(v(t1), x(t1),t1) may be varied to find a stationary solu...
In a previous paper, we developed a so-called fluctuation model for the inelastic collisional intera...
Using an analogy with statistical thermodynamics and the Einstein equation for fluctuation probabili...