1996
DOI: 10.1103/physreve.54.4155
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Alignment and instability of dust crystals in plasmas

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Cited by 266 publications
(196 citation statements)
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“…A negatively charged bottom particle [40] is attracted by the ion focus while it is repelled by the negatively charged top particle [1,8]. At the same time, the bottom particle continues to repel the top one whence accelerating it [9]. The forces working to produce this motion are the plasma forces [41].…”
Section: Coupled Pairs As Quasi-particlesmentioning
confidence: 99%
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“…A negatively charged bottom particle [40] is attracted by the ion focus while it is repelled by the negatively charged top particle [1,8]. At the same time, the bottom particle continues to repel the top one whence accelerating it [9]. The forces working to produce this motion are the plasma forces [41].…”
Section: Coupled Pairs As Quasi-particlesmentioning
confidence: 99%
“…[8].) On the other hand, they can be successfully used, as the studies performed recently have shown, as an active agent in the plasma crystal heating experiments [9,10], as a convenient practical diagnostic tool allowing to test in the simplest way the complex plasma elasticity modules [11][12][13], or as a probe of the plasma electric field distribution [14].…”
Section: Introductionmentioning
confidence: 99%
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“…According to [4] the vertical electric field in a sheath changes linearly with the height. This dependence is realized approximately in the regions not too close to the lower electrode and the border of the presheath: the quadratic approximation for the potential ϕ(z) in the plasma layer is also used in [5,6] for the analysis of the equations of motion of DC . Therefore in the case of a vertical potential well we use in eq.…”
Section: Equations Of Static Equilibriummentioning
confidence: 99%
“…Then the necessary inequality is ℓ < 6R D which is usually satisfied (see, for example, [3,5,6]). The linear terms in Eq.…”
Section: Equations Of Static Equilibriummentioning
confidence: 99%