Abstract

A circularly orbiting electromagnetic harmonic wave may appear when a 1S electron encounters a decelerating stopping positively charged hole inside a semiconductor. The circularly orbiting electromagnetic harmonic wave can have an interaction with a conducting electron which has a constant time independent drift velocity.

Highlights

  • The general theory of relativity has predicted the bending of light [1] which is an electromagnetic wave [2]

  • The circularly orbiting electromagnetic harmonic wave can have an interaction with a conducting electron which has a constant time independent drift velocity

  • In this article the interaction Hamiltonian of an electromagnetic field with an electron is derived by the use of the Lorentz force equation [7], the relativistic momentum relation [7] and the Hamilton equation [7]

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Summary

Introduction

The general theory of relativity has predicted the bending of light [1] which is an electromagnetic wave [2]. If the positively charged hole or the positively charged positron is decelerating and stopping while encountering the negatively charged electron of the 1S orbital, the law of the conservation of momentum predicts that the K wave vector of light which is proportional to the momentum of the emerging light or the emerging electromagnetic wave should be tangential to a circular orbit [5]. Light which is an electromagnetic wave and having a periodic nature can be decomposed into its harmonic functions. In this article the interaction Hamiltonian of an electromagnetic field with an electron is derived by the use of the Lorentz force equation [7], the relativistic momentum relation [7] and the Hamilton equation [7]

The Representation of a Circularly
K r 2
Conclusions
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