2015
DOI: 10.1080/00268976.2015.1027754
|View full text |Cite
|
Sign up to set email alerts
|

Cooking strongly coupled plasmas

Abstract: We present the orbital-free method for dense plasmas which allows for efficient variable ionisation molecular dynamics. This approach is a literal application of density functional theory where the use of orbitals is bypassed by a semi-classical estimation of the electron kinetic energy through the Thomas-Fermi theory. Thanks to a coherent definition of ionisation, we evidence a particular regime in which the static structure no longer depends on the temperature: the -plateau. With the help of the well-known T… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...

Citation Types

0
1
0

Year Published

2016
2016
2020
2020

Publication Types

Select...
2

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(1 citation statement)
references
References 45 publications
0
1
0
Order By: Relevance
“…15,16 Interestingly, when the plasma is partially ionized, the coupling parameter Γ can stay constant along isochores as a result of the increase of ionization compensating the increase of temperature. [17][18][19][20] In plasma mixtures, the coupling parameter Γ may be different for each species giving rise to interesting coexistences between different coupling regimes. [21][22][23] In the Yukawa model, the polarization of the electrons close to each ion is accounted for by a screened potential V Y (r) = Qe exp(−κr)/r, where κ is an inverse screening length.…”
mentioning
confidence: 99%
“…15,16 Interestingly, when the plasma is partially ionized, the coupling parameter Γ can stay constant along isochores as a result of the increase of ionization compensating the increase of temperature. [17][18][19][20] In plasma mixtures, the coupling parameter Γ may be different for each species giving rise to interesting coexistences between different coupling regimes. [21][22][23] In the Yukawa model, the polarization of the electrons close to each ion is accounted for by a screened potential V Y (r) = Qe exp(−κr)/r, where κ is an inverse screening length.…”
mentioning
confidence: 99%