2013
DOI: 10.1002/ctpp.201200070
|View full text |Cite
|
Sign up to set email alerts
|

Influence of Polarization Phenomena on Radial Distribution Function of Dust Particles

Abstract: A pseudopotential model of intergrain interaction in dusty plasmas is proposed to take into account both the electrostatic polarization and the screening phenomena. The derivation is entirely based on the renormalization theory of plasma particles interaction developed previously. Dust particles are assumed to be conductive such that the polarization phenomenon can strictly be treated in the charge-image approximation. Such an assumption imposes no restraint on generality of the present consideration because t… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
7
0
1

Year Published

2014
2014
2021
2021

Publication Types

Select...
7
1

Relationship

2
6

Authors

Journals

citations
Cited by 14 publications
(8 citation statements)
references
References 11 publications
0
7
0
1
Order By: Relevance
“…It should directly be stressed that the generalized Poisson-Boltzmann equation can rigorously be derived from the Bogolyubov chain of equations for the equilibrium distribution functions in the pair correlation approximation 31 and in the recent past it was successfully applied to a variety of plasmas, such as the semiclassical plasma, 32,33 the partially ionized hydrogen plasma, 34,35 and even the dusty plasma in the Debye approximation. 36,37 Equation (12) is actually a relation to determine the effective interaction potential, or the pseudopotential, U ab , through the true microscopic potentials u ab . It can be clearly seen that the pseudopotentials definitely take into account the screening in the buffer plasmas since they inevitably incorporate the number densities of electrons and protons.…”
Section: Plasma Parametersmentioning
confidence: 99%
“…It should directly be stressed that the generalized Poisson-Boltzmann equation can rigorously be derived from the Bogolyubov chain of equations for the equilibrium distribution functions in the pair correlation approximation 31 and in the recent past it was successfully applied to a variety of plasmas, such as the semiclassical plasma, 32,33 the partially ionized hydrogen plasma, 34,35 and even the dusty plasma in the Debye approximation. 36,37 Equation (12) is actually a relation to determine the effective interaction potential, or the pseudopotential, U ab , through the true microscopic potentials u ab . It can be clearly seen that the pseudopotentials definitely take into account the screening in the buffer plasmas since they inevitably incorporate the number densities of electrons and protons.…”
Section: Plasma Parametersmentioning
confidence: 99%
“…Analogous inference can absolutely be made in case of the decrease in www.cpp-journal.org the grain size parameter D.Note that quite a similar behavior of the correlation function was observed in the Percus-Yewick and superposition approximations with further experimental verification for the gas-discharge plasmas [38], cf. [39,40].…”
Section: Correlation Functions Of Dusty Plasmasmentioning
confidence: 99%
“…From a fundamental point of view, of great interest is the situation in which the electrostatic energy of dust particles interaction noticeably exceeds their thermal energy. In this case, the dust component is called strongly coupled, because the short‐range and long‐range order formation develops in the arrangement of dust particles with respect to one another . Such a behaviour of dust particles is conventionally interpreted as a liquid or even crystalline state, which provides a whole range of means for testing theoretical concepts specifically developed for many‐body systems with strong interparticle interactions .…”
Section: Introductionmentioning
confidence: 99%