Oscillatory-Precessional Motion of a Rydberg Electron Around a Polar Molecule

We provide a detailed classical description of the oscillatory-precessional motion of an electron in the field of an electric dipole. Specifically, we demonstrate that in the general case of the oscillatory-precessional motion of the electron (the oscillations being in the meridional direction (θ-di...

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Main Author: Eugene Oks
Format: Article
Language:English
Published: MDPI AG 2020-08-01
Series:Symmetry
Subjects:
Online Access:https://www.mdpi.com/2073-8994/12/8/1275
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spelling doaj-2cc32c697b1249f687319e5a9839f4242020-11-25T01:27:02ZengMDPI AGSymmetry2073-89942020-08-01121275127510.3390/sym12081275Oscillatory-Precessional Motion of a Rydberg Electron Around a Polar MoleculeEugene Oks0Physics Department, 380 Duncan Drive, Auburn University, Auburn, AL 36849, USAWe provide a detailed classical description of the oscillatory-precessional motion of an electron in the field of an electric dipole. Specifically, we demonstrate that in the general case of the oscillatory-precessional motion of the electron (the oscillations being in the meridional direction (θ-direction) and the precession being along parallels of latitude (φ-direction)), both the θ-oscillations and the φ-precessions can actually occur on the same time scale—contrary to the statement from the work by another author. We obtain the dependence of φ on θ, the time evolution of the dynamical variable θ, the period T<sub>θ</sub> of the θ-oscillations, and the change of the angular variable φ during one half-period of the θ-motion—all in the forms of one-fold integrals in the general case and illustrated it pictorially. We also produce the corresponding explicit analytical expressions for relatively small values of the projection p<sub>φ</sub> of the angular momentum on the axis of the electric dipole. We also derive a general condition for this conditionally-periodic motion to become periodic (the trajectory of the electron would become a closed curve) and then provide examples of the values of p<sub>φ</sub> for this to happen. Besides, for the particular case of p<sub>φ</sub> = 0 we produce an explicit analytical result for the dependence of the time t on θ. For the opposite particular case, where p<sub>φ</sub> is equal to its maximum possible value (consistent with the bound motion), we derive an explicit analytical result for the period of the revolution of the electron along the parallel of latitude.https://www.mdpi.com/2073-8994/12/8/1275polar moleculeRydberg electronclassical motionperiodic orbits
collection DOAJ
language English
format Article
sources DOAJ
author Eugene Oks
spellingShingle Eugene Oks
Oscillatory-Precessional Motion of a Rydberg Electron Around a Polar Molecule
Symmetry
polar molecule
Rydberg electron
classical motion
periodic orbits
author_facet Eugene Oks
author_sort Eugene Oks
title Oscillatory-Precessional Motion of a Rydberg Electron Around a Polar Molecule
title_short Oscillatory-Precessional Motion of a Rydberg Electron Around a Polar Molecule
title_full Oscillatory-Precessional Motion of a Rydberg Electron Around a Polar Molecule
title_fullStr Oscillatory-Precessional Motion of a Rydberg Electron Around a Polar Molecule
title_full_unstemmed Oscillatory-Precessional Motion of a Rydberg Electron Around a Polar Molecule
title_sort oscillatory-precessional motion of a rydberg electron around a polar molecule
publisher MDPI AG
series Symmetry
issn 2073-8994
publishDate 2020-08-01
description We provide a detailed classical description of the oscillatory-precessional motion of an electron in the field of an electric dipole. Specifically, we demonstrate that in the general case of the oscillatory-precessional motion of the electron (the oscillations being in the meridional direction (θ-direction) and the precession being along parallels of latitude (φ-direction)), both the θ-oscillations and the φ-precessions can actually occur on the same time scale—contrary to the statement from the work by another author. We obtain the dependence of φ on θ, the time evolution of the dynamical variable θ, the period T<sub>θ</sub> of the θ-oscillations, and the change of the angular variable φ during one half-period of the θ-motion—all in the forms of one-fold integrals in the general case and illustrated it pictorially. We also produce the corresponding explicit analytical expressions for relatively small values of the projection p<sub>φ</sub> of the angular momentum on the axis of the electric dipole. We also derive a general condition for this conditionally-periodic motion to become periodic (the trajectory of the electron would become a closed curve) and then provide examples of the values of p<sub>φ</sub> for this to happen. Besides, for the particular case of p<sub>φ</sub> = 0 we produce an explicit analytical result for the dependence of the time t on θ. For the opposite particular case, where p<sub>φ</sub> is equal to its maximum possible value (consistent with the bound motion), we derive an explicit analytical result for the period of the revolution of the electron along the parallel of latitude.
topic polar molecule
Rydberg electron
classical motion
periodic orbits
url https://www.mdpi.com/2073-8994/12/8/1275
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