plasma
Article
A Supersensitive Method for Spectroscopic Diagnostics of
Electrostatic Waves in Magnetized Plasmas
Eugene Oks
1,
*, Elisabeth Dalimier
2,3
and Paulo Angelo
2,3
Citation: Oks, E.; Dalimier, E.;
Angelo, P. A Supersensitive Method
for Spectroscopic Diagnostics of
Electrostatic Waves in Magnetized
Plasmas. Plasma 2021, 4, 780–788.
https://doi.org/10.3390/
plasma4040040
Academic Editor:
Andrey Starikovskiy
Received: 19 November 2021
Accepted: 6 December 2021
Published: 10 December 2021
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1
Physics Department, Auburn University, 380 Duncan Drive, Auburn, AL 36849, USA
2
Laboratoire Pour L’utilisation des Lasers Intenses, Sorbonne Université, CEDEX 05, F-75252 Paris, France;
elisabeth.dalimier@upmc.fr (E.D.); paulo.angelo@upmc.fr (P.A.)
3
Centre National de la Recherche Scientifique, Ecole Polytechnique, CEA—Université Paris-Saclay,
CEDEX 05, F-75252 Paris, France
* Correspondence: goks@physics.auburn.edu
Abstract: For relatively strong magnetic fields, hydrogen atoms can have delocalized bound states
of almost macroscopic dimensions. Therefore, such states are characterized by a Giant Electric
Dipole Moment (GEDM), thus making them very sensitive to an external electric field. We con-
sidered the manifestations of the GEDM states in hydrogen spectral line profiles in the presence
of a quasimonochromatic electrostatic wave of a frequency ω in a plasma. We demonstrated that
in this situation, hydrogen spectral lines can exhibit quasi-satellites, which are the envelopes of
Blochinzew-type satellites. We showed that the distinctive feature of such quasi-satellites is that their
peak intensity is located at the same distance from the line center (in the frequency scale) for all
hydrogen spectral lines, the distance being significantly greater than the wave frequency ω. At
the absence of the GEDM (and for relatively strong electrostatic waves), the maxima of the satellite
envelopes would be at different distances from the line center for different hydrogen lines. We
demonstrated that this effect would constitute a supersensitive diagnostic method for measuring the
amplitude of electrostatic waves in plasmas down to ~10 V/cm or even lower.
Keywords: strong magnetic fields; center-of-mass effects; giant electric dipole moments; supersensi-
tive diagnostics of electrostatic waves in plasmas
1. Introduction
There are numerous methods for spectroscopic diagnostics of plasmas (see, e.g.,
books [1–11] listed in chronological order). Among these methods are those designed for
spectroscopic diagnostics of various electrostatic waves in plasmas (see, e.g., books [3,10,11]).
These methods, based on the shape of spectral lines of atoms and ions, cover the range of
amplitudes of the electrostatic waves from ~1 kV/cm to ~1 GV/cm. In the present paper
we describe a possibility to extend the sensitivity of such methods to ~10 V/cm or even
lower, as follows.
There are plenty of studies showing that for hydrogenic atoms/ions in a uniform
magnetic field, the center-of-mass motion and the relative (internal) motion are coupled by
the magnetic field and, rigorously speaking, cannot be separated (see, e.g., papers [12–14]
and references therein). A pseudoseparation is possible for hydrogen atoms. It leads to a
Hamiltonian for the relative motion that depends on a center-of-mass integral of the motion
K called pseudomomentum but does not depend on the center-of-mass coordinate [14].
We remind that the pseudomomentum K is the canonical variable conjugated to the center-
of-mass coordinate.
A diamagnetic potential term in the Hamiltonian for the relative motion is responsible
for the formation of an additional potential well far away from the hydrogen nucleus
(proton). For relatively strong magnetic fields, the new bound states inside this well are
delocalized states of almost macroscopic dimensions. Therefore, the bound state inside this
Plasma 2021, 4, 780–788. https://doi.org/10.3390/plasma4040040 https://www.mdpi.com/journal/plasma