The Schrödinger Equation, the Zero-Point Electromagnetic Radiation, and the Photoelectric Effect

Abstract

A Schrodinger type equation for a mathematical probability amplitude Ψ(x,t) is derived from the generalized phase space Liouville equation valid for the motion of a microscopic particle, with mass M and charge e, moving in a potential V(x). The particle phase space probability density is denoted Q(x,p,t), and the entire system is immersed in the “vacuum” zero-point electromagnetic radiation. We show, in the first part of the paper, that the generalized Liouville equation is reduced to a simpler Liouville equation in the equilibrium limit where the small radiative corrections cancel each other approximately. This leads us to a simpler Liouville equation that will facilitate the calculations in the second part of the paper. Within this second part, we address ourselves to the following task: Since the Schrodinger equation depends on $\hbar $ , and the zero-point electromagnetic spectral distribution, given by $\rho _{0}{(\omega )} = \hbar \omega ^{3}/2 \pi ^{2} c^{3}$ , also depends on $\hbar $ , it is interesting to verify the possible dynamical connection between ρ 0(ω) and the Schrodinger equation. We shall prove that the Planck’s constant, present in the momentum operator of the Schrodinger equation, is deeply related with the ubiquitous zero-point electromagnetic radiation with spectral distribution ρ 0(ω). For simplicity, we do not use the hypothesis of the existence of the L. de Broglie matter-waves. The implications of our study for the standard interpretation of the photoelectric effect are discussed by considering the main characteristics of the phenomenon. We also mention, briefly, the effects of the zero-point radiation in the tunneling phenomenon and the Compton’s effect.