Below-unitarity-threshold branch cut in the $$\left\langle {\bar qq} \right\rangle $$ coefficient of the axial-vector two-current correlation function

1993 ◽  
Vol 60 (2) ◽  
pp. 235-241 ◽  
Author(s):  
V. Elias ◽  
J. L. Murison ◽  
M. D. Scadron ◽  
T. G. Steele
2003 ◽  
Vol 118 (23) ◽  
pp. 10382-10386 ◽  
Author(s):  
T. V. Lokotosh ◽  
N. P. Malomuzh ◽  
K. S. Shakun

1998 ◽  
Vol 57 (5) ◽  
pp. 6195-6197 ◽  
Author(s):  
K. N. Pathak ◽  
S. Ranganathan ◽  
R. E. Johnson ◽  
R. K. Sharma ◽  
K. Tankeshwar

2015 ◽  
Vol 30 (07) ◽  
pp. 1550035 ◽  
Author(s):  
E. Apresyan ◽  
Sh. Khachatryan ◽  
A. Sedrakyan

The response of fermionic system to external gauge fields is defined by current–current correlation function Πμν(q, q0). Transport properties of different physical quantities are determined by zero energy–momentum limit of it. As it is known close to half-filling the physics of graphene is described by (2+1)-dimensional Dirac theory. In this paper, we calculate current–current correlation function in Dirac theory in a presence of chemical potential η and gap m.


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