Gn. Throumoulopoulos et D. Pfirsch, NEGATIVE-ENERGY PERTURBATIONS IN CIRCULARLY CYLINDRICAL EQUILIBRIA WITHIN THE FRAMEWORK OF MAXWELL-DRIFT KINETIC-THEORY, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 53(3), 1996, pp. 2767-2777
The conditions for the existence of negative-energy perturbations (whi
ch could be nonlinearly unstable and cause anomalous transport) are in
vestigated in the framework of linearized collisionless Maxwell-drift
kinetic theory for the case of equilibria of magnetically confined, ci
rcularly cylindrical plasmas and vanishing initial field perturbations
. For wave vectors with a nonvanishing component parallel to the magne
tic field, the plane equilibrium conditions (derived by Throumoulopoul
os and Pfirsch [Phys Rev. E 49, 3290 (1994)]) are shown to remain vali
d, while the condition for perpendicular perturbations (which are foun
d to be the most important modes) is modified. Consequently, besides t
he tokamak equilibrium regime in which the existence of negative-energ
y perturbations is related to the threshold value of 2/3 of the quanti
ty eta(nu) = partial derivative InTnu/partial derivative InNnu, a new
regime appears, not present in plane equilibria, in which negative-ene
rgy perturbations exist for any value of eta(nu). For various analytic
cold-ion tokamak equilibria a substantial fraction of thermal electro
ns are associated with negative-energy perturbations (active particles
). In particular, for linearly stable equilibria of a paramagnetic pla
sma with hat electron temperature profile (eta(e) = 0), the entire vel
ocity space is occupied by active electrons. The part of the velocity
space occupied by active particles increases from the center to the pl
asma edge and is larger in a paramagnetic plasma than in a diamagnetic
plasma with the same pressure profile. It is also shown that, unlike
in plane equilibria, negative-energy perturbations exist in force-free
reversed-field pinch equilibria with a substantial fraction of active
particles. The present results, in particular the fact that a thresho
ld value of eta(nu), is not necessary for the existence of negative-en
ergy perturbations, enhance even more the relevance of these modes.