This paper is the third one of a series of four. In the previous ones, we developed a thermodynamic and mechanical framework introducing the properties of the so-called Bernoulli oscillators. These last are classical oscillators submitted to an external force coming from the quantum vacuum, and driving a distinguished part of the oscillator motion itself which we call the hidden degree of freedom (HDF). In paper II, an expression for the HDF-potential effective in the classical expression of the mechanical energy theorem has been given. In order to show that this expression is consistent with a quantum mechanical context, a few unknown functions must be determined. To this purpose, we set up in this paper a mechanical-statistical framewor...
In this note, we investigate two velocities present in a quantum bound state. The first is the root...
In the previous Part I of this paper, we developed a theoretical model to account for energy and mas...
This book gathers state-of-the-art advances on harmonic oscillators including their types, functions...
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 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 a few previous papers, we developed a so-called classical fluctuation model providing (generalize...
In this paper, we join two different theoretical approaches to the problem of finding a classical-li...
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...
In a previous note on the quantum harmonic oscillator, it was seen that for the ground state (-1/2m)...
A bound quantum state wavefunction has a factor exp(iEt), where E is the energy, but in the calculat...
Both quantum mechanics and classical statistical mechanics predict the same momentum and spatial den...
In this note, we investigate two velocities present in a quantum bound state. The first is the root...
In the previous Part I of this paper, we developed a theoretical model to account for energy and mas...
This book gathers state-of-the-art advances on harmonic oscillators including their types, functions...
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 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 a few previous papers, we developed a so-called classical fluctuation model providing (generalize...
In this paper, we join two different theoretical approaches to the problem of finding a classical-li...
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...
In a previous note on the quantum harmonic oscillator, it was seen that for the ground state (-1/2m)...
A bound quantum state wavefunction has a factor exp(iEt), where E is the energy, but in the calculat...
Both quantum mechanics and classical statistical mechanics predict the same momentum and spatial den...
In this note, we investigate two velocities present in a quantum bound state. The first is the root...
In the previous Part I of this paper, we developed a theoretical model to account for energy and mas...
This book gathers state-of-the-art advances on harmonic oscillators including their types, functions...