2022
DOI: 10.3389/fphy.2022.879092
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Preservation of a Dust Crystal as it Falls in an Afterglow Plasma

Abstract: In an experiment, the power that sustains a plasma was extinguished, so that microspheres, which had been levitated, fell downward toward a lower electrode. At the beginning of their fall, the microspheres were self-organized with a crystalline structure. This structure was found to be preserved as the microspheres accelerated all the way to the lower electrode. Although microspheres had, in this afterglow plasma, large positive charges of 12,500 e, their interparticle repulsion was unable to significantly alt… Show more

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Cited by 20 publications
(12 citation statements)
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“…In a cc-rf argon discharge at f rf = 13.56 MHz with an argon pressure p = 1.067 Pa, 8.69 μm diameter melamine spherical particles were levitated and formed and twodimensional plasma crystal. Then, the power was abruptly shut down, and the microparticles fell (note that the particle arrangement was not significantly altered during the fall [93]). In this experiment, due to the large value of the coupling capacitor, the negative self-bias of the powered electrode that develops naturally when the plasma is on (V dc ≃ − 150 V), decayed in a timescale of ~3 s, a time much longer than the plasma afterglow timescales, therefore, maintaining a large quasi dc electric field between the electrodes during the afterglow period.…”
Section: Dust Dynamics Dust Decharging and Residual Charges In Plasma...mentioning
confidence: 99%
“…In a cc-rf argon discharge at f rf = 13.56 MHz with an argon pressure p = 1.067 Pa, 8.69 μm diameter melamine spherical particles were levitated and formed and twodimensional plasma crystal. Then, the power was abruptly shut down, and the microparticles fell (note that the particle arrangement was not significantly altered during the fall [93]). In this experiment, due to the large value of the coupling capacitor, the negative self-bias of the powered electrode that develops naturally when the plasma is on (V dc ≃ − 150 V), decayed in a timescale of ~3 s, a time much longer than the plasma afterglow timescales, therefore, maintaining a large quasi dc electric field between the electrodes during the afterglow period.…”
Section: Dust Dynamics Dust Decharging and Residual Charges In Plasma...mentioning
confidence: 99%
“…The study of dusty plasma crystals in various discharge configurations has been a hot research topic in the dusty plasma because of its wide scope in understanding various mediums at the kinetic level. [18,[32][33][34]96,97] Apart from neutral pressure and input rf power, the external magnetic field can also alter the characteristics of dust-plasma crystal. [64] The dust grains in a crystalline state perform random motion about their equilibrium position in the absence of an external B-field, but they have rotational motion if the magnetic field is introduced.…”
Section: Crystallization and Melting Of Dusty Plasma Crystalmentioning
confidence: 99%
“…However, nonconducting (Teflon/nylon) ring always remains in floating condition (floating potential), which could provide a better confinement to charged dust particles in strongly magnetized plasma. Thus, nonconducting confinement rings of appropriate radius and thickness should be used to perform dusty plasma experiments in strong B‐field. A recent experimental study by Chaubey et al [ 100–102 ] in after‐glow dusty plasma demonstrates the presence of large positive charges on the dust surface and their ability to be held above a lower powered (biased) electrode without the presence of a plasma background. If the levitated positively charged dust grains are exposed to the strong external magnetic field (few Tesla) then Lorentz force may act on them and start to gyrate (rotate) about B‐field lines in the plane perpendicular to B‐field.…”
Section: Potential Futuristic Steps To Get Magnetized Dusty Plasmamentioning
confidence: 99%
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“…In Earth-based experiments, due to the macroscopic size, the dust particles normally levitate close to the lower electrode, in the plasma sheath, where the gravitational force is balanced by the sheath electric force. In addition, the repulsive Yukawa interaction (the expansion) is commonly balanced by applying an external magnetic field [25][26][27][28][29] or by externally applied radial confinement potential [30],…”
Section: Introductionmentioning
confidence: 99%