Relativistic random-phase-approximation response function for quasielastic electron scattering in local density approximation

1987 ◽  
Vol 35 (1) ◽  
pp. 298-304 ◽  
Author(s):  
K. Wehrberger ◽  
F. Beck
1990 ◽  
Vol 04 (16) ◽  
pp. 1023-1027 ◽  
Author(s):  
Y.C. KAO ◽  
M.F. YANG

We study the conductivity tensor for the pure anyon system at finite temperature by calculating the electromagnetic response function Kμν(ω, k) in the random-phase approximation. We find that the conductivity is indeed infinite through the vanishing of the renormalized Chern-Simons term for the statistical gauge fields in the limit k=0, ω→0. To study the Meissner effect at finite temperature, others have looked at Kµν(ω, k) in the limit ω=0, k→0. We compare the results and make some comments.


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