scholarly journals Deriving the hard thermal loops of QCD from classical transport theory

1994 ◽  
Vol 72 (22) ◽  
pp. 3461-3463 ◽  
Author(s):  
P. F. Kelly ◽  
Q. Liu ◽  
C. Lucchesi ◽  
C. Manuel
1994 ◽  
Vol 50 (6) ◽  
pp. 4209-4218 ◽  
Author(s):  
P. F. Kelly ◽  
Q. Liu ◽  
C. Lucchesi ◽  
C. Manuel

2002 ◽  
Vol 65 (2) ◽  
Author(s):  
Sen Cheng ◽  
Scott Pratt ◽  
Peter Csizmadia ◽  
Yasushi Nara ◽  
Dénes Molnár ◽  
...  

2004 ◽  
Vol 82 (9) ◽  
pp. 671-678 ◽  
Author(s):  
M E Carrington ◽  
T Fugleberg ◽  
D Pickering ◽  
M H Thoma

In the present paper, we calculate the dielectric functions of an ultra-relativistic plasma, such as an electron–positron or a quark–gluon plasma. We use classical transport theory and take into account collisions within the relaxation time approximation. From these dielectric functions we derive the dispersion relations of longitudinal and transverse plasma waves. PACS Nos.: 12.38.Mh, 52.25.Dg, 52.27.Ep, 52.35.Hr


1997 ◽  
Vol 56 (2) ◽  
pp. R1295-R1298 ◽  
Author(s):  
Jochen Rau

1987 ◽  
Vol 38 (2) ◽  
pp. 245-262
Author(s):  
Alf H. Øien

Starting from classical transport theory, equations for particle density, particle momentum and electron and ion temperatures are derived for steady-state, toroidal plasma configurations in a parameter regime like that of ACT-I. A set of simplified equations for particle density and electron and ion temperatures are solved numerically. Radial density and temperature profiles are shown and compared with experiments.


Author(s):  
T. Groves

It is common in transmission electron microscopy to use specimens which are of the order of a micron in thickness. For such thicknesses it becomes likely that an incident electron will scatter more than once, and one would expect some drastic effects on image formation. A theory of image formation has been derived for thick specimens in the conventional (CEM) and scanning transmission (STEM) electron microscopes. This theory is based on a solution of the Boltzmann transport equation for plural scattering, and is expected to apply to the imaging of small objects embedded in thick amorphous films.We imagine an idealized specimen shown in Fig. 1. A point-like object is embedded in a thick film at a depth n1, measured in units of the mean free path λ for elastic scattering.


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