Abstract

According to the existing paradigm, helium atoms and helium-like ions (hereafter, heliumic systems) in a relatively weak external static electric field do not exhibit the linear Stark effect—in distinction to hydrogen atoms and hydrogen-like ions. In the present paper we consider the classical dynamics of a muonic-electronic heliumic system in Rydberg states–starting from the concept from our previous paper. We show that there are two states of the system where the averaged electric dipole moment is non-zero. Consequently, in these states the heliumic system should exhibit the linear Stark effect even in a vanishingly small electric field, which is a counter-intuitive result. We also demonstrate the possibility of controlling the overall precession of the electronic orbit by an external electric field. In particular, we show the existence of a critical value of the external electric field that would “kill” the precession and make the electronic orbit stationary. This is another counter-intuitive result. We calculate analytically the value of the critical field and show that it is typically smaller or even much smaller than 1 V/cm.

Highlights

  • According to the existing paradigm, helium atoms and helium-like ions in a relatively weak external electric field do not exhibit the linear Stark effect—in distinction to hydrogen atoms and hydrogen-like ions. It is well-known that the linear Stark effect in hydrogenic systems is due to the fact that the overwhelming majority of states of these systems are characterized by a non-zero value of the averaged electric dipole moment

  • We demonstrate the possibility of controlling the overall precession of the electronic orbit by an external electric field

  • We have considered the classical dynamics of Rydberg states of muonic-electronic helium or helium-like ions

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Summary

Introduction

According to the existing paradigm, helium atoms and helium-like ions in a relatively weak external electric field do not exhibit the linear Stark effect—in distinction to hydrogen atoms and hydrogen-like ions (see, e.g., the textbooks [1,2]). It is well-known that the linear Stark effect in hydrogenic systems (atoms and ions) is due to the fact that the overwhelming majority of states of these systems are characterized by a non-zero value of the averaged electric dipole moment. The linear Stark effect has classical roots, as it is well-known since at least 1923—see, e.g., Born book [4] of 1923, as well as book [5] (problem 2.32) and book [6]

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