Schwinger-Dyson equations and effective potential for composite fields in quantum electrodynamics in curved spacetime

1990 ◽  
Vol 7 (5) ◽  
pp. 887-892 ◽  
Author(s):  
S D Odintsov ◽  
Y I Shil'nov
2001 ◽  
Vol 81 (10) ◽  
pp. 1547-1555 ◽  
Author(s):  
V. A. Yerokhin ◽  
A. N. Artemyev ◽  
V. M. Shabaev ◽  
M. M. Sysak ◽  
O. M. Zherebtsov ◽  
...  

2018 ◽  
Vol 2018 (6) ◽  
Author(s):  
Tommi Markkanen ◽  
Sami Nurmi ◽  
Arttu Rajantie ◽  
Stephen Stopyra

1979 ◽  
Vol 19 (10) ◽  
pp. 2929-2934 ◽  
Author(s):  
Walter Dittrich ◽  
Wu-yang Tsai ◽  
Karl-Heinz Zimmermann

1993 ◽  
Vol 90 (3) ◽  
pp. 677-688 ◽  
Author(s):  
A. A. Bytsenko ◽  
E. Elizalde ◽  
S. D. Odintsov

2003 ◽  
Vol 18 (13) ◽  
pp. 937-946 ◽  
Author(s):  
MINU JOY ◽  
V. C. KURIAKOSE

Considering a massive ϕ6 self-interacting scalar field coupled arbitrarily to a (2+1)-dimensional Bianchi type-I spacetime, we evaluate the one-loop effective potential. It is found that ϕ6 potential can be regularized in (2+1)-dimensional curved spacetime. A finite expression for the energy–momentum tensor is obtained for this model. Evaluating the finite temperature effective potential, the temperature dependence of phase transitions is studied. The crucial dependence of the phase transitions on the spacetime curvature and on the coupling to gravity is also studied. The nature of phase transitions for the present model is clarified to be first order. A first-order phase transition proceeds by nucleation of bubbles of broken phase in the background of unbroken phase.


1997 ◽  
Vol 12 (06) ◽  
pp. 411-418 ◽  
Author(s):  
B. Geyer ◽  
Yu. I. Shil'nov

The effective potential of composite fermion fields in three-dimensional Thirring model in curved spacetime is calculated in linear curvature approximation. The phase transition accompanied by the creation of nonzero chiral invariant bifermionic vector-like condensate is shown to exist. The type of this phase transition is discussed.


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