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arXiv:2305.08206 · Physics of Plasmas

Electronic resonances in expanding non-neutral ultracold plasma

Sergey Ya. Bronin, Evgenii Vladimirovich Vikhrov, Sergey A. Saakyan, Boris B. Zelener, B. V. Zelener

Published Mar 1, 2024• 4 citations
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Abstract

Calculations of the spectrum of eigen oscillations of an inhomogeneous ultracold plasma are presented both in the absence and in the presence of charge imbalance. The collective modes of these plasma oscillations are recorded in experiments as absorption resonances of a radio frequency electric field. It is shown that in the presence of friction of the electronic component, a discrete spectrum of plasma eigen oscillations is formed. The dependence of the frequency of these resonances on the plasma expansion time in the presence of a charge imbalance is obtained. There is good agreement with the experiments of different authors.

DOI
10.1063/5.0194420

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Comment on "Observation of Collective Modes of Ultracold Plasmas"

Yurii V. Dumin

We discuss a theoretical interpretation of the experiment by Fletcher, Zhang, and Rolston [PRL, 96, 105003 (2006)], who revealed a number of subharmonics of the electron emission under external irradiation of the freely-expanding clouds of ultracold plasmas. The original interpretation of these subharmonics as standing waves of plasma oscillations (the so-called Tonks-Dattner resonances) encounters a number of problems, such as the lack of adequate boundary conditions and incorrect dependence on the plasma temperature and the degree of neutrality. It is the aim of the present comment to mention that a more promising interpretation may be based on the peaks in the efficiency of ionization of the secondary Rydberg atoms, formed during the plasma cloud expansion and cooling. The presence of the last-mentioned peaks is well supported by the independent experiment by Maeda and Gallagher [PRL, 93, 193002 (2004)].

arXiv:0906.5162•Jun 28, 2009•0 citations
Calculations of the spectrum of eigen oscillations of an inhomogeneous ultracold plasma are presented both in the absence and in the presence of charge imbalance. The collective modes of these plasma oscillations are recorded in experiments as absorption resonances of a radio frequency electric field. It is shown that in the presence of friction of the electronic component, a discrete spectrum of plasma eigen oscillations is formed. The dependence of the frequency of these resonances on the plasma expansion time in the presence of a charge imbalance is obtained. There is good agreement with the experiments of different authors.
We investigate the collective dynamics of electrons in ultracold neutral plasmas driven by an oscillating radio-frequency field. We point out the importance of a sharp density drop at the plasma boundary that arises due to unavoidable charge imbalances, and show that this plasma edge provides the major mechanism for energy absorption from the external field. Using a cold fluid theory, we derive the corresponding absorption frequency and validate our findings by microscopic molecular dynamics simulations. The proposed edge-mode is shown to provide a consistent explanation for the observed absorption spectra measured in different experiments. Understanding the response of the electronic plasma component to weak external driving is essential since it grants experimental access to the time-evolving density and temperature of ultracold plasmas.
Using a new technique to directly detect current induced on a nearby electrode, we measure plasma oscillations in ultracold plasmas, which are influenced by the inhomogeneous and time-varying density and changing neutrality. Electronic detection avoids heating and evaporation dynamics associated with previous measurements and allows us to test the importance of the plasma neutrality. We apply dc and pulsed electric fields to control the electron loss rate and find that the charge imbalance of the plasma has a significant effect on the resonant frequency, in excellent agreement with recent predictions suggesting coupling to an edge mode.
Abstract The results of calculations using the molecular dynamics method of low-frequency ion oscillations in ultracold plasma, previously observed in the experiment, are presented. Oscillations of the radial velocity of ions and changes in the direction of their flows during the expansion of ultracold plasma in a quadrupole magnetic field are detected. This is due to the influence of the magnetic field on the charge imbalance, which leads to the simultaneous existence of potential wells for both electrons and ions. Ion temperature oscillations with a frequency close to the ion plasma frequency are also detected. Satisfactory agreement with the experiment is obtained.
Ultracold plasmas are regarded as quasineutral but not strictly neutral. The results of charge imbalance in the expansion of ultracold plasmas are reported. The calculations are performed by a full molecular-dynamics simulation. The details of the electron velocity distributions are calculated without the assumption of electron global thermal equilibrium and Boltzmann distribution. Spontaneous evolutions of the charge imbalance from the initial states with perfect neutrality are given in the simulations. The expansion of outer plasma slows down with the charge imbalance. The influences of plasma size and parameters on the charge imbalance are discussed. The radial profiles of electron temperature are given for the first time, and the self-similar expansion can still occur even if there is no global thermal equilibrium. The electron disorder induced heating is also found in the simulation.
We discuss a theoretical interpretation of the experiment by Fletcher, Zhang, and Rolston [PRL, 96, 105003 (2006)], who revealed a number of subharmonics of the electron emission under external irradiation of the freely-expanding clouds of ultracold plasmas. The original interpretation of these subharmonics as standing waves of plasma oscillations (the so-called Tonks-Dattner resonances) encounters a number of problems, such as the lack of adequate boundary conditions and incorrect dependence on the plasma temperature and the degree of neutrality. It is the aim of the present comment to mention that a more promising interpretation may be based on the peaks in the efficiency of ionization of the secondary Rydberg atoms, formed during the plasma cloud expansion and cooling. The presence of the last-mentioned peaks is well supported by the independent experiment by Maeda and Gallagher [PRL, 93, 193002 (2004)].