scholarly journals Formation of Kinetics Coherent Structures in Weakly Collisional Media

Plasma ◽  
2021 ◽  
Vol 4 (2) ◽  
pp. 359-365
Author(s):  
Alexander Karimov ◽  
Vladislav Bogdanov

The formation of nonlinear, nonstationary structures in weakly collisional media with collective interactions are investigated analytically within the framework of the kinetic description. This issue is considered in one-dimensional geometry using collision integral in the Bhatnagar-Gross-Krook form and some model forms of the interparticle interaction potentials that ensure the finiteness of the energy and momentum of the systems under consideration. As such potentials, we select the Yukawa potential, the δ-potential, which describes coherent structures in a plasma. For such potentials we obtained a dispersion relation which makes it possible to estimate the size and type of the forming structures.

2011 ◽  
Vol 23 (37) ◽  
pp. 374107 ◽  
Author(s):  
Ru Wang ◽  
Zhuo Wang ◽  
Joe Leigh ◽  
Nahil Sobh ◽  
Larry Millet ◽  
...  

2002 ◽  
Vol 12 (9) ◽  
pp. 61-64
Author(s):  
C. Pasquier ◽  
M. Héritier ◽  
D. Jérome

We present a model comparing the free energy of a phase exhibiting a segregation between spin density wave (SDW) and metallic domains (eventually superconducting domains) and the free energy of homogeneous phases which explains the findings observed recently in (TMTSF)2PF6. The dispersion relation of this quasi-one-dimensional organic conductor is linearized around the Fermi level. Deviations from perfect nesting which stabilizes the SDW state are described by a unique parameter t$'_b$, this parameter can be the pressure as well.


VLSI Design ◽  
1998 ◽  
Vol 8 (1-4) ◽  
pp. 489-493
Author(s):  
H. Kosina ◽  
C. Troger

Nonparabolicity effects in two-dimensional electron systems are quantitatively analyzed. A formalism has been developed which allows to incorporate a nonparabolic bulk dispersion relation into the Schrödinger equation. As a consequence of nonparabolicity the wave functions depend on the in-plane momentum. Each subband is parametrized by its energy, effective mass and a subband nonparabolicity coefficient. The formalism is implemented in a one-dimensional Schrödinger-Poisson solver which is applicable both to silicon inversion layers and heterostructures.


2011 ◽  
Vol 109 (10) ◽  
pp. 103526 ◽  
Author(s):  
M. de Dios-Leyva ◽  
Julio C. Drake-Pérez

Author(s):  
A. Alejo-Molina ◽  
J. J. Sánchez-Mondragon ◽  
D. A. May-Arrioja ◽  
D. Romero-Antequera ◽  
J. Escobedo-Alatorre ◽  
...  

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