The formation and dynamics of vertical dust chains in the radio frequency discharge plasma sheath have been investigated. The spatiotemporal evolution diagram allows the visualization of the dust chain formation process as well as the oscillation phenomenon. A clear stratification was observed, and spatially nonuniform self-organizing behavior of the dust chains, such as fractures and reconnections, was also observed, showing that the lower layers of the large-grained chains are less restricted, softer, and more prone to rearrangement. The spatial distribution characteristics of the charged particles in the sheath and the modified two-particle model, which takes into account the interparticle attraction, partially explain the mechanisms of the fracture and reorganization behavior of the dust chains.
{"title":"Dynamics and reorganization of dust chains in a complex plasma","authors":"Yang Liu, Baoxia Li, Guannan Shi, Feng Huang","doi":"10.1002/ctpp.202300179","DOIUrl":"10.1002/ctpp.202300179","url":null,"abstract":"<p>The formation and dynamics of vertical dust chains in the radio frequency discharge plasma sheath have been investigated. The spatiotemporal evolution diagram allows the visualization of the dust chain formation process as well as the oscillation phenomenon. A clear stratification was observed, and spatially nonuniform self-organizing behavior of the dust chains, such as fractures and reconnections, was also observed, showing that the lower layers of the large-grained chains are less restricted, softer, and more prone to rearrangement. The spatial distribution characteristics of the charged particles in the sheath and the modified two-particle model, which takes into account the interparticle attraction, partially explain the mechanisms of the fracture and reorganization behavior of the dust chains.</p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"64 9","pages":""},"PeriodicalIF":1.3,"publicationDate":"2024-04-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140626322","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The BBGKY hierarchy in the Wigner representation is used with an extended Singwi-Tosi-Land-Sjölander (STLS) ansatz for the two-particle distribution function [H. Kählert, G. J. Kalman, and M. Bonitz, Phys. Rev. E 90, 011101 (2014)] to study the density response function and the dispersion relation of collective modes in a strongly coupled quantum system. It is shown that the local field correction (LFC) and the dispersion relation reduce to the results of the Quasi-Localized Charge Approximation (QLCA) in the classical limit. In the quantum case, the LFC acquires a frequency-dependence, similar to the quantum version of the STLS theory. The dispersion relation is governed by a generalization of the QLCA dynamical matrix. The results are expected to be relevant for the analysis of collective modes in quantum liquids with strong correlations.
Wigner 表征中的 BBGKY 层次结构与双粒子分布函数的扩展 Singwi-Tosi-Land-Sjölander (STLS) 解析[H. Kählert, G. J. Kalman, and M. Bonitz, Phys. Rev. E 90, 011101 (2014)]一起用于研究强耦合量子系统中集体模式的密度响应函数和弥散关系。结果表明,局部场校正(LFC)和频散关系可以还原为经典极限中准局部电荷近似(QLCA)的结果。在量子情况下,LFC 与频率相关,类似于 STLS 理论的量子版本。色散关系受 QLCA 动态矩阵广义化的支配。这些结果有望用于分析具有强相关性的量子液体中的集体模式。
{"title":"Dynamics of strongly correlated quantum systems from an extended Singwi-Tosi-Land-Sjölander closure for the BBGKY hierarchy","authors":"Hanno Kählert","doi":"10.1002/ctpp.202400018","DOIUrl":"10.1002/ctpp.202400018","url":null,"abstract":"<p>The BBGKY hierarchy in the Wigner representation is used with an extended Singwi-Tosi-Land-Sjölander (STLS) ansatz for the two-particle distribution function [H. Kählert, G. J. Kalman, and M. Bonitz, Phys. Rev. E 90, 011101 (2014)] to study the density response function and the dispersion relation of collective modes in a strongly coupled quantum system. It is shown that the local field correction (LFC) and the dispersion relation reduce to the results of the Quasi-Localized Charge Approximation (QLCA) in the classical limit. In the quantum case, the LFC acquires a frequency-dependence, similar to the quantum version of the STLS theory. The dispersion relation is governed by a generalization of the QLCA dynamical matrix. The results are expected to be relevant for the analysis of collective modes in quantum liquids with strong correlations.</p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"64 6","pages":""},"PeriodicalIF":1.3,"publicationDate":"2024-04-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/ctpp.202400018","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140598195","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
F. Cai, S. Kado, G. Kawamura, C. Feng, R. Matoike, A. Miyashita, S. Ohshima, T. Minami, S. Inagaki, F. Kin, S. Kobayashi, A. Ishizawa, Y. Nakamura, H. Okada, S. Konoshima, T. Mizuuchi, Y. Feng, H. Frerichs, K. Nagasaki
The distribution pattern of the connection length in the divertor region of Heliotron J was calculated by the field line tracing method. A multifold layer structure, characterized by the range of connection length, was revealed to interpret the response of the transport of the lower-charged impurity ions to the divertor structure. Impurity transport simulated by the EMC3-EIRENE code shows that lower-charged impurity ions tend to concentrate in the first multifold layer. This result is consistent with the line-integral extreme ultraviolet spectroscopy measurement, which implies that the impurity's response to the divertor topological structure needs to be considered in interpreting the spectroscopy result.
{"title":"Impact of multifold magnetic structure on spectroscopy analysis in Heliotron J based on EMC3-EIRENE simulation","authors":"F. Cai, S. Kado, G. Kawamura, C. Feng, R. Matoike, A. Miyashita, S. Ohshima, T. Minami, S. Inagaki, F. Kin, S. Kobayashi, A. Ishizawa, Y. Nakamura, H. Okada, S. Konoshima, T. Mizuuchi, Y. Feng, H. Frerichs, K. Nagasaki","doi":"10.1002/ctpp.202300145","DOIUrl":"10.1002/ctpp.202300145","url":null,"abstract":"<p>The distribution pattern of the connection length in the divertor region of Heliotron J was calculated by the field line tracing method. A multifold layer structure, characterized by the range of connection length, was revealed to interpret the response of the transport of the lower-charged impurity ions to the divertor structure. Impurity transport simulated by the EMC3-EIRENE code shows that lower-charged impurity ions tend to concentrate in the first multifold layer. This result is consistent with the line-integral extreme ultraviolet spectroscopy measurement, which implies that the impurity's response to the divertor topological structure needs to be considered in interpreting the spectroscopy result.</p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"64 7-8","pages":""},"PeriodicalIF":1.3,"publicationDate":"2024-04-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/ctpp.202300145","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140598183","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Rachid Fermous, Moufida Benzekka, Rabia Amour, Rima Mebrek
In this paper, the role of dust grain's gravitational force on the nonlinear dust-acoustic oscillations in non-Maxwellian dusty plasma is analyzed. It is shown that increasing the number of non-thermal ions causes the diminution of the electrostatic potential's amplitude and a reduction in the number of oscillations introduced by the gravitational force. We have also found that reducing the size of the dust grain induces qualitatively the same effects as an increase in the number of non-thermal ions and when the gravitational force is considered, the electric charge exhibits oscillatory profile and becomes less negative far away from the origin. This result may be interesting in the study of astrophysical plasmas where the electromagnetic force is smaller than the gravitational one such as in the Halley Comet.
{"title":"Nonlinear oscillations of dust-acoustic waves in non-Maxwellian dusty plasma under the gravitational force effect","authors":"Rachid Fermous, Moufida Benzekka, Rabia Amour, Rima Mebrek","doi":"10.1002/ctpp.202300170","DOIUrl":"10.1002/ctpp.202300170","url":null,"abstract":"<p>In this paper, the role of dust grain's gravitational force on the nonlinear dust-acoustic oscillations in non-Maxwellian dusty plasma is analyzed. It is shown that increasing the number of non-thermal ions causes the diminution of the electrostatic potential's amplitude and a reduction in the number of oscillations introduced by the gravitational force. We have also found that reducing the size of the dust grain induces qualitatively the same effects as an increase in the number of non-thermal ions and when the gravitational force is considered, the electric charge exhibits oscillatory profile and becomes less negative far away from the origin. This result may be interesting in the study of astrophysical plasmas where the electromagnetic force is smaller than the gravitational one such as in the Halley Comet.</p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"64 9","pages":""},"PeriodicalIF":1.3,"publicationDate":"2024-04-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140598436","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Phase separations in strongly coupled fine particles in plasmas are discussed and two-component mixtures are simulated by molecular dynamics with the background plasma being treated as continuum. The system size of laboratory experiments is assumed and separations into phases with a common electron density of the background plasma are analyzed. Since the charge on fine particles increases approximately in proportion to the size, we expect the larger component with stronger coupling condensates from the mixture. Results expressed in terms of strengths of Coulomb coupling and screening of the larger component seem to be mostly similar to the one-component case, at least in cases where the ratio of fine particle sizes is 2, and the mixing ratio is in the range from 0.25 to 0.75.
{"title":"Phase separations of strongly coupled fine particles and fine particle mixtures in plasmas","authors":"Hiroo Totsuji","doi":"10.1002/ctpp.202400011","DOIUrl":"10.1002/ctpp.202400011","url":null,"abstract":"<p>Phase separations in strongly coupled fine particles in plasmas are discussed and two-component mixtures are simulated by molecular dynamics with the background plasma being treated as continuum. The system size of laboratory experiments is assumed and separations into phases with a common electron density of the background plasma are analyzed. Since the charge on fine particles increases approximately in proportion to the size, we expect the larger component with stronger coupling condensates from the mixture. Results expressed in terms of strengths of Coulomb coupling and screening of the larger component seem to be mostly similar to the one-component case, at least in cases where the ratio of fine particle sizes is 2, and the mixing ratio is in the range from 0.25 to 0.75.</p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"64 6","pages":""},"PeriodicalIF":1.3,"publicationDate":"2024-04-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140598179","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The properties of small-amplitude solitary electron acoustic waves in a plasma where the hot electrons take regularized kappa distribution are investigated via the reductive perturbation method. It is found there only exists the sup-electron-acoustic rarefactive soliton, the electron acoustic velocity is modified by the regularized kappa distribution. The amplitude and width of the electron acoustic soliton decrease monotonously with the increase of the exponential cutoff parameter of hot electrons. But they vary with respect to the spectral index non-monotonously. As to the observed parameters in the Earth's inner magnetosphere, the speed, electric field strength, and the width of solitary electron acoustic wave are comparable with the observations.
{"title":"Small amplitude solitary electron acoustic wave for hot electrons taking regularized kappa distribution","authors":"Yong Liu, Meng–Lei Wang","doi":"10.1002/ctpp.202400009","DOIUrl":"10.1002/ctpp.202400009","url":null,"abstract":"<p>The properties of small-amplitude solitary electron acoustic waves in a plasma where the hot electrons take regularized kappa distribution are investigated via the reductive perturbation method. It is found there only exists the sup-electron-acoustic rarefactive soliton, the electron acoustic velocity is modified by the regularized kappa distribution. The amplitude and width of the electron acoustic soliton decrease monotonously with the increase of the exponential cutoff parameter of hot electrons. But they vary with respect to the spectral index non-monotonously. As to the observed parameters in the Earth's inner magnetosphere, the speed, electric field strength, and the width of solitary electron acoustic wave are comparable with the observations.</p>","PeriodicalId":10700,"journal":{"name":"Contributions to Plasma Physics","volume":"64 10","pages":""},"PeriodicalIF":1.3,"publicationDate":"2024-04-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140598189","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
David Rees, Joona Sissonen, Mathias Groth, Vesa-Pekka Rikala, Henri Kumpulainen, Beth Thomas, Mathias Brix, JET Contributors
The hydrogenic two-point model (H-2PM), an analytical model for the scrape-off layer that predicts a common electron and ion temperature and density along a flux tube from a target temperature and density, is adapted to a single-species helium (He) model, preserving the 2PM assumptions and analytical nature. Across a range of densities and heating powers, the predicted